Transferencia de energía y cantidad de movimiento en magnetósferas inducidas Romanelli, Norberto Julio

Μέγεθος: px
Εμφάνιση ξεκινά από τη σελίδα:

Download "Transferencia de energía y cantidad de movimiento en magnetósferas inducidas Romanelli, Norberto Julio"

Transcript

1 Transferencia de energía y cantidad de movimiento en magnetósferas inducidas Romanelli, Norberto Julio Tesis Doctoral Facultad de Ciencias Exactas y Naturales Universidad de Buenos Aires Contacto: digital@bl.fcen.uba.ar Este documento forma parte de la colección de tesis doctorales y de maestría de la Biblioteca Central Dr. Luis Federico Leloir. Su utilización debe ser acompañada por la cita bibliográfica con reconocimiento de la fuente. This document is part of the doctoral theses collection of the Central Library Dr. Luis Federico Leloir. It should be used accompanied by the corresponding citation acknowledging the source. Fuente / source: Biblioteca Digital de la Facultad de Ciencias Exactas y Naturales - Universidad de Buenos Aires

2 t s 1 t s 2 t r s rt t ís r s r r 2 t t tós r s s s s r s t r t r r tít t r rs s r s ár s ís s r r rt r t r s t s s r és r rt 2 r ó 3 s r st s r r ss r r st t t str í 2 ís s s r s r s r

3

4 s r s t t s s r t r tr r st s s s str ís s r s t s s r r s 2 tr r t s tós r s s s st s r ás s í t s rt tá s 2 t P 2 t 3 s r st s r st t s s s s s t t rr t s t ór s s st r s t s s s s 2 s r ó s st t s ó s tr s r r í 2 t t tr s t s 2 s q s r s í t s t r r s s s s r s s r í s rt 2 s r s s s rs r 2 r 2 s 1 r ss 2 s r ó st s r s ó s q r t r ó s s 1ós r s t s r t s t 3 r t ór r s r ó t r á q t t t é t s s t s rr t 2 tr s r s rt r t rí ét rt r s t ór s rt s q s s s r s r r t ér tr s t s ér s s t s s s rt r s s t é s str t r s tós r s s 2 s s r s r t t r s t s r t s s r s r í ét r st s r t r r r í ét s t é st t r t 2 st t r s r s r st s r s r t t r st s r s r s s t s s t s tr st s tós r s r s s r s r st s r s ss s s t r t é s r s s r ó rtí s r s r t s t ós r tá s st s str rt s r3 s t s ó ét st s t r s 2 s r t r r st s rtí s q r s té t sí t s s tr t st t s s s tr t r ó s t s t s ér s s s s r s t s t r s s t 3 s 2 r t tr tr s s s r st t s r s s tr s r r í 2 t t P r s s P s s str ís s tós r s s í ét s s tr r r s ó t s ér

5

6 r s r r 2 r t t s r s str t t r s t t s s s t tr t t t st 2 t str 2s s s t s rr s t r t t s r s s t s r s2st r s 2 t s rs t s 2 s t 2 s s r ts r 2 r t s ss s t t r t t r t t s st 2 t r rt s t s r ts t r r t s t r t tr s r r 2 r t t t s ts t s r t 2 t r r rt s t s s s r 2 t rs r 2 r s 1 r ss s r ts t s rr s rs s t r r t s t r s st t s t t r s s r s t t t r t t r 1 s r s t t s r t s s t t 2 r 2 s r t s r t r t r r t s t t t ts s s t rr t t r t ts r t r t s t t t s s r r t t ss tr t s r rt s t ts t 2 2 s t q t s t str t r t s ts r s s t r t s t s rr r r s ts r r t t s r t s t t r 2 t 2 t rt r t t r 2 s s st t s rr s 2 s t t st t 2 s s r ts r 2 t s r t s s t t r s r s t t s t t s t s t s t s r s s t s r ts r 2 t ss s r t s st t t r t r ss s r rt s r t t t s r t s st s s t rt t t t s r s t s r ts t r st t s t 1 rt s t t s r t s s r2 t r r r t s t s s s s t 1 t r t t t r s 2 t t s r ts t r r s t t 3 s r ts t r t s t r s t st 2 s t t r t r ss s tr s r r 2 r t 2 r s str 2s s s t s r s t t 2 tr r q 2 s s t s r r s

7

8 s r s

9

10 r t s r r r q r r r rs s r s 2 s st s tí s 2 é s rt r r 3 st t t str í 2 ís s r r r s st s 2 t s s r s r s rr st tr é q r r r és r r r rt tr r st t s s st s t át st t s s P r r s s r s tr P r s s s r r r s r r r t 1t 3 r s tr s r s r r s 2 r s ó r r ñ r t t t r r st r s t 2 á 3 r 2 s st tr r q r t r s r r s 2 r s r st r s r 2á P r t 2 á 2 3 q s s r 2 st r r r s r t ír r r t 3 r r r ñ r t r á t s r 2 q s r s t t s r s r

11

12 t r s s r t t q st s t s 2 r t s t s t r tr tr t t s t st rs st t s 2 2 r

13

14 P t s r r r s rt ó 3 3 Pr t 2 tr s str r rs s r t s r rs r 2 r P t rt r 2 ó 3 3 3á 3 r r r t2 s t t r t 2 tr r q 2 str r rs t r rs st t 2 r 1 s r 2s s tt rt s r t r2 r t t 2 P t ó 3 rt t 2 st t t 2 r 2 r t 3 t s r str 2s r rt r rt P r t rt r tt t s rt2 t s r t t s t t t t s r s 2s s P 2s s s rr rt P r s r ss r r t s t s s r t 2s s tt rt r 3 str r t 2 tr s t s r s r 1 2s s P 2s s rt ó 3 3 t rt t s t t t r t r2 t r t s r t s r rs r 2 r 2s s P 2s s r ss

15

16 List of Abbreviations AB ASPERA AU BS CA CAPS DOY DRAP E/C ELS ER ESA EUV FGM FOV GCM GZ HT IC ICA ICE IM IMA IMB IMF IMS IN INMS Aerobraking Analyzer of Space Plasma and Energetic Atoms Astronomical Unit Bow Shock Closest Approach Cassini Plasma Spectrometer Day of Year Draping Energy-per-Charge Electron Spectrometer Sensor Electron Reflectometer Electrostatic Analyzer Extreme Ultra-violet Fluxgate Magnetometer Field of View Global Climate Model Giacobini-Zinner dehoffmann-teller Ion Cyclotron Ion Composition Analyzer International Cometary Explorer Induced Magnetosphere Ion Mass Analyzer Induced Magnetospheric Boundary Interplanetary Magnetic Field Ion Mass Spectrometer Inner Negative Ion and Neutral Mass Spectrometer

17 IP IPRL KSO LEF LH LMD LP MAG MAVEN MCP MEX MGS MHD MISCHA MOI MPB MPR MSH MSO MVA MVAB ON OP PCW PH PRL PSD PVO RH RHS Inner Positive Inverse Polarity Reversal Layer Kronocentric Solar Orbital Linear Electric Field Left Hand Laboratoire de Météorologie Dynamique Langmuir Probe Magnetometer Mars Atmospheric Volatile Evolution Microchannel Plate Mars Express Mars Global Surveyor Magnetohydrodynamics Magnetic field in Interplanetary Space during comet Halley s approach Mars Orbit Insertion Magnetic Pile-up Boundary Magnetic Pile-up Region Magnetosheath Mars Solar Orbital Minimum variance Analysis Minimum variance Analysis of Magnetic Field Vector Outer Negative Outer Positive Proton Cyclotron Waves Perihelion Polarity Reversal Layer Power Spectral Density Pionner Venus Orbiter Right Hand Right Hand Side

18 RPC RPWS SAE SC SD SEM SLT SNG SOHO SPO SSE SSS ST SW SWIA TIIS TOF UCT ULF UM VEX VHM VSO WH Rosetta Plasma Consortium Radio and Plasma Wave Spectrometer Southern Hemisphere Autumn Equinox Spacecraft Standard Deviation Solar Extreme Ultra-violet Monitor Saturn Local Time Singles Solar and Heliospheric Observatory Science Phase Orbit Southern Hemisphere Spring Equinox Southern Hemisphere Summer Solstice Straight-Through Solar Wind Solar Wind Ion Analyzer Titan Titan Ionospheric Interaction System Time of Flight Coordinated Universal Time Ultra Low Frequency Unstable mode Venus Express Vector Helium Magnetometer Venus Solar Orbital Whistler

19

20 r2 tr t P 2s s r t s s t r t s rt t t r s st t r s r t t s rt s s st t P s t s r t t 2 r 2 s t 2 r 2 s s t t rt r s s ts str ts t s 2s s s r t s r ts rs r 2 r ss ss ss tr ts r t r ss s t t r 1 1

21 s 1 r ss t t r s str t P t s 2s s t s r ts r 2s s s r t r r r s r r ss rr t t s r t s s r r 2s s é st t t 2 t t s r s t t t r t t r t r ss t P 2t s r t t t r t r t t tr t r t t t r s st t2 ts t P t P r r 2 t t ss s r t r st s t t t rt t s t r t s r t s r t 2s s s t r t r s ts t t str t r BXDRAP IMF s ss s s Pr t 2 tr s str r rs s tr t s r t r ss s s str r rs t s 2s s 1 s s r t s 2 s tr rr t P r 3 t P r 3 t r r tr 1 t t t rt s r rr r r t2 P s str r rs t s r rs st t 2 r 1 s r s str r s 11 P s s

22 s ss s s t s s r t t 2 s r s r t r ss s t t r t 3 s s r s t s t t r s r t r ss s s r t s P s r t P s t r t t é t2 r Pr rt s r 2s s t é st r 2s s s ss s s r s é r t r t r s 2 s s rs s r s 11

23

24 P tr t s s q s tr s r tr rt s 1 ts t r st t s s s r s r t r 3 2 1tr 2 s t s t rt r s r s r s2st s t s r t t s s t s r s s s s sts st 1 s 2 r rt s r 1 t s t s r t t t t 2 3 t s 2 s r t s tr s t t s r ss t r t t ttr t t s r s t t r s r ss r r t t t s r r t t rst r s s t ts 1tr 2 s t2 t s 3 t t r t t rt t s 1 t tr t r s s s t rt s r 1tr 2 r r r st t r t r t t s rr s r t s t r r 10 8 s r s t ts t t2 t ts t s r t s r s t t s s t t r t r2 t r t s r s s r tr t t s s t r st r r r t t 2 t (L D ). t t rt s r t t 2 t t s t r r t t s ss t 3 t rr s t r t t t t s s s rs s r s t t rt s r t r

25 tr t t r s st s t s s s r 2 r r t t s s t t rt r t r t st s t t t s ts t ss t t r t2 s s r rs s s r t t r ts r t 2 t t r s r s st s t tr s t s s s t rt ts t tr s t s t s r s r t 2 t r t t t t s r s r s t t s r 3 s s rt r t str t 3 s t r r t r ss s s st r ts r t s r s t s r s2st t ts rs s t r s r st s t t t s t t ts ss t s s 2s t t ts s r ts r s r s2st s t s t t ts ts t t t tr s t s r t st r r rs t t 3 r < ss t s < ss t rs < ñ t t < t rt t ts r t t2 s ts r s t t s r s2st t s s r ts s t s t s s r r 2 s r s ss s r t t s rs s t 2 s t s t r t t r t t t rs t r rt s t s s r 2 r t 1 r 2 t t t 1t r str t 3 s t rr s t s r t 3 st t r st 2 s t t r r s t s r s t s 3 str t t s t t s r t 3 st s rt r t str t 3 s s r 2 t s s st t t 2s r ss s r t r s r t s r rt 2 t r s t t r s s r s t t2 s r2 r t t t s t t s ts t 1t 1 s r s tr rt s s 3 t 1t r s r s t t ts r r s t t r2 r s t ss t 3 s t r ts t t s ts t s t t str t 3 s s r 2 t r s r t r t t s t s st t r P s s

26 tr t tr t st s r r r s ts rr ts t t s s r rr ts t r r t t 1t r str t t r r t t s t 1t r s s t t2 t s s r t t t s s t r s r t str 2 s t t r 2 s r t s rr s t s st s 1 s r tr t s 3 r 1 s r s r t s s s t s rs t s s r r t 2 t tr t s r 3 t t s s r r r s r r r t t t 1t r t s tt r t t r 2 t r t 1t r s s t t s s s t s s ss rt r r t r s 2 t 1t r t 3 s r s r s st t s s s t r 2s r rt s t t t s 1t r 1 s r s t r rt t r t st 2 t 1t r t r 1 s r r rt s r r t s t t s r t 3 t s t r tr t t t r s ts t s r t rt t s q s r ts t t t 2 t s rt t t str ss t t t r s s t t s t t s r t t t r s t t r t s r s t tr s r t r 2 t s s 1 t r t r s r t r s 2s s r t s rs t s r r r2 r t rt r r r t 2 r t r 2 t t str r 1t r r t t rt s t s 2 r t s tr s t s s 1 t r t t t t r t r2 t s t2 t s t2 t t s t s s t 2 s t rt 1 s r 1t s t t s st s r s r 2 r s 3 t s s r t r t s st t s t t r s t tr r q 2 s s s r s t 2 t s r 2 r ss r t t t r t s t s r r 1 t t tr ss t t t t t 1t r t rs s r s

27 tr t r s s t str r t 2 t t t r rt s t s r r r t r t s r s t st t s t t s t s s s t r2 t t s rs t t 3 s s s s s r t r r rt s t s rt t t t t s t s r t t t t ts t tr s t s r t r st t s s r t rs s t t R M r ts t r R M st s r r s rs 1R M = 3400 r t t r t r t t s r t s t t 2 s r r t t s t t R M r t t r rs t s t t r t t t t t s r r2 1t t t s 2 t s s rt s t 2 t s t r s r ss r t s r t r 3 2 str t t2 t str t r s s t r t t s r t s t2 r s s s r s t ss s s t t r2 P s r t s t r t 2 s r t t 2 t t r2 s t s r t r 3 2 s t s t t r 2 tr s tr t t str t r t t r r r t t r t ts s t s ts s s r t s t t R M r t t r rs r t t r t r s t t R M r t t r rs t s r t r t t P t s s s t r2 s t 2 t t r ss r s 2 t r s ss t t2 t t t s t r t t t 2 t s r r r t rt s r s s t t t t r s r ss r s t t s r t r 3 2 r r s t t r tr s t s s t t t r s s r t s t s t t 450 t t t 2s t r t t s r t t r t r s r t t s s r t r t r2 s t t r s ts r t t 3 t t r t s r tr s t rt t s t s r2 t s P s s

28 tr t t t t s t str r t P s t ts 1t s t t s t t r2 s s sts t t s s t t r t s rr t s s t s t r t t t r t rs s t t t s t r t t r2 s r P s r s r s t s r t s rr rs r t r t 2 t s rt t t t t t t t s 1 st t rs ss ss s r st t s r t t s t t s t t s r r t s t s r t s s r s ss t t t s r t rs s s r r t str t t st t t 3 s t s r t s r2 t t t s P t s s s t st 2 s r 2s rr t s rr s s s s s r ts r rs s r s

29 tr t 2 r s s ss s t r r t t s r r r t t r t s rt r s r 2s s r ts rs t s t t 2 s t s s s str t r s s t r r s t s r t r t s r t s s s t s r rr t s r ts t r t s t 2 r 2 s r t t s t r t r s t t 1 r s t q s t 2s s r q r t t r r t s r ts t 2 r t s r ts t t s t s t str ts r t s ss s r s s ss t r r ss s t t t 2 t s r rst 23 s r t r s t r s 2 2t 2 s t r r t 2 t t 3 s s r s r t 2 r s r r t t s t r t 2 s r 1 t2 t r t ss t tr t r st 2 st t s r t st t t t r 2 t r ts rs t P 2 s s r ts t 2 t t t rs r t rs r 2 r s r ts r s t 2 t r st 2 t r rt s t r t s s tr r q 2 tr t s s s r t 2 tr s r P s s r 2 s 1 r ss t str r s rs s r s t 2 P rt r 2 23 t r t tr r t t r r t r t t 23 r P s r t t s P r t r r s t t 3 s r t s rr t r s r st s t t t t r t r ss s s r s ts r t s rt r t s 23 t r 2 t ss P s tr t r P r tr s s t t t r t P s P r ss t t r r t t s r s t t r 2 t s t s t t 2 t r r s ts t s s t s t s s P s s

30 tr t s st t r r s t t s s t r s st r r s r s s ís s q t r s r r s 2 tr tós r s s r s r st s r st t s s s s s t r r t s r s rt r st t s s t ór s rt r s 3 str á s s tr t s rt t s 2 t 2 st t s s stá str t r s t r ít r s t s r s s r s t ór s s s s q s t 3 s r s r r st t s ó s q rr st s t r s tr tr s t s t rí t r á 2 stá t s st ít ít stá s rr r r s té s á s s t s s r s r t r r t r s r st s r st t s s s s s s t s 2 s s str t s r st s s s t é s s t s ít tr t s r t í ét tós r Pr r t 3 s st t s r t ríst s rr t ét r s ít t r q s t 3 r t t t r 2 r r s r t r r st t s r t s ét s r s 2 r t r s s s é tr s 2 ét s s s s r ó st r ás st s r í ét s t r s rt 2 t P 2 sá s s r st s r s tó tr s r s s s rs r 2 r 2 r s t t ít st s s r s 2 s s s r ó s tr ét s s tr r s s tró r tó s r s r 2 s 1 r ss s r s s rr rt 2 s r s t t rt r 3 s t s r st s r tó tr 2 r tó tr tr s r r P s s 2 t s r ét s P r rs s r s

31 tr t ít stá tr t r s t 3 q r tá s té t ás r t r 2 s r s s r ó s s ér q t r tr s tós r P r st t r rt r 3 s t s r st s r s tró tr P s r tr s 2 r t s tó tr 2 str t s P s 2 P r ss t r r t s s s s r s r í ét s rí r s t t tá t ít r s t s s s s r s r s t t s s P s s

32 P P 2s s r t s s t r t s st t s s s r 1tr 2 t s s s 3 rt s r t r s t r s r s t t r r2 s t2 r t t t 1tr 2 r t r2 t r r r2 s t rs t r rt s t 2 2 r s t t r s r s t 2 t r t s r s t s t r s t r t s s rt s t ts r2 r t rt s r t t r rt s t s r 2 r s s t r r 2 t t t r t s t rt s r rt t r r s t t t r t s s r r r s t 3 s t t r t s s t st t s t r s t s s ss t st 2 s s s t r s t s r t t s t r r s t t t r t ts r t t rt t s r t s s s s s t t r r t s r t s s s q t t rs

33 P 2s s r t s s t r t s rt t s s tr 2 tr s r s 2 r rt s t r s tr t r s r t r rst t r s t s s t s r t 2 s r rt 1t r tr E t B s r 2 2 t r ts st t r s ts r t r r t s r t2 rt s t t t t s t t t t s s r t r t s t r t r s st t r s q t t r r t st rt r q t2 v s t t t s E B s ts m dv dt = q(e+ v c B) r t t s E = 0 B st t t r t3 r r s t q v c B t s r s r r t t t2 t r t r s r t r t rt t t t s v s t r s s B v s s st t s s t t v B s s t s t t r rt t r r t B t t r r s r r t r s r L = mc q B v : Larmor radius or Gyroradius s r r q 2 s Ω cq = q B mc : Cyclotron frequency or Gyrofrequency r s t tr t r2 s 1 st t t r t s t r r r s t 2r r q 2 s t s s t rt 2r t 2 s t r r 1 t s t t s t2 t t t s rr t rt s r t s r r t s t2 r r r s 2 tr r q 2 t r s 1. P s s

34 P 2s s r t s s t r t s tr r r t tr s t 3 r t rt tr t r2 s t r s t t r s s t s r t t r F r tr r t B t rt r t t t r t t a = F /m. t s t s t tr str t 2 r r t B t s E B. t s s t tr t r2 t r rt r t r s t r s ts r tr s 3 r 2 s t r t3 tr s r t s t E B t tr t s s r r r r s t 2 s r r r r t r s t t t t2 v r s r r t st rt s v/c 1 s r 1 r ss s t rr t t rst r r v/c. tr t s t r r r r 2 t r t3 tr s r t s t rst r r r E = E+ v c B B = B v c E s t t t E = 0 t E = v c B t s B = B t rst r r 2 s t s tr s r t s r rt t t s s t t t B tr E B s s r t r t t 2 t t tr r r t B s r t r t t s t t2 v = V D t r s t t V D = c E B B 2 t r r s t tt r r r r s E B = E B+ V D c B = 0 t s r r r t t t r r t B r s t t 2r t t t t t r r t B s t t s r s t t 2r t t s r t t2 V D t t t t s t2 r t s t s r r rt s t s s s r s t t t r r s 2 s 2 r t t r qe q t 2 r r F t r s r t V D = (cf/q) B/B 2. r t t s r 2 r s s r t r t2 s t s t r st q t t 2r r s t t t E B s r r t B t t v. rs s r s

35 P 2s s r t s s t r t s r r t q t t rs t 2r r q 2 t t r 1 t 2 t 2r t s r r t s s 2 st t s tr 2r t s t tr t rt t s t s t r rt s 2r t r t t s t r t t r t t r s t t t s t2 ts s t rr r t tr s rs t r t r s s tr s rs r t r r t r st t s ts s r rr t 2 r r t t s rt s t r s s t r 2 s r t t rt s P s s s st t s r tr rt s ss s t st t t s s2st s 2 t s t r t2 v rt t t t t t s t r 2 t q t t r rt t s r t r t rt s rt s s s r s r st s st t st r t 2 rt s r s t t t2 s st r t t2 str t t r rt s s s r ts t r t q t t r rt 2 r t q t r t t2 str t t2 str t t r s s s f s (r,v,t), s s t t t r rt s t t [r,r+d 3 r] t t s t r [v,v+d 3 v] t t t s d 6 N s = f s (r,v,t)d 3 rd 3 v st s r t t st t t s s 2 s t s r t s t r s s s t r s t2 t r t2 t t r 2 r t r r r ts f s t2 s r s t2 n s r t t2 s rt s s n s (r,t) = f s (r,v,t) d 3 v V 3 r t2 v s s v s (r,t) = 1 f s (r,v,t) v d 3 v n s (r,t) V 3 t r 2 t s t r r r t t2 v s (r,t) s < 1 2 m s(v v s ) 2 >= 1 f s (r,v,t) 1 n s (r,t) V 3 2 m s(v v s ) 2 d 3 v P s s

36 P 2s s r t s s t r t s 2 r st t rt r ss r rt s s s s s r t t t r r r r 2 2 p s n s = 2 3 < 1 2 m s(v v s ) 2 > t s t r 2 q r t t r t r t t2 str t t s ss t r t t2 s t s s str t s t 1 t3 str t m f s (r,v) = n s ( )3/2 exp [ m s(v v s ) 2 ] 2πkT 2k B T s r k B s t t3 st t t s t 1 t3 str t t t r s s v th,s = 2kB T s m s t t r t sq r t r s s < v 2 >= 3k B T s /m s s t r t r 2 r rt t r r r t t2 v s s W =< 1 2 n s(v v s ) 2 >= 3k BT s 2 s st t t s r s t t r s t r r f s t r ts r t t s rt s q t r 2 t s s t s r t r s t t st s s r t r s s s r s 2 st t s s s t r rt s s s s s tr s s q s tr 1 ts t r r ss 2 r rt s t q 2 s s t rt s st r 2 t r r s r t s s r 2 rr t t r t s s t s s s s t r 2 t t r t t t rt s s r t 2 t r t r rt st < r > s s r t t t r t r 2 r rt e 2 < r > k BT < r > n 1/3, t r t r Γ t r t t r r 2 t t r t t k B T Γ n 1/3 e 2 k B T rs s r s

37 P 2s s r t s s t r t s st s r t t2 r t s t q 2 s s t s t s r s Γ r s t t r s 2 t tr st r t r rt s s t tr tr t2 t t r 1 s t rt s r 3 t s tr t2 t t t t ts t r s t s r s t t r t 1 t 2 tr t t s s t t t tr st t t t t st r r r q q r tr s s Φ(r) = q r e r/l D r L D t 2 t s kb T L D = 4πne 2 t st s r L D t tr t t r t r q s r 2 t r s t r L D t r s t 2 s 2 t r s t t s t t t st s s r r t s s q s tr t s s r r t L D. s r t r t s r t r 3 2 r s t2 n T 10 5 s r s t t 2 t t s r t s t s t t s rt t t t t 2 s r q r s t t r s 3 D t s r r rt s nl 3 D 1. t t t t Γ L D t tt r t s r s s (4πΓ) 3/2 1. t s t 2 t q r s rt r r st 2 t r rt r t tr t t r s r str t t s s s 2 t r st r t 2 s tr s r st r t t s t 2 s t t t s t s t t s s T = 2π me 4πne 2 2π w pe r w pe s t tr s r q 2 t r s t2 n t s r tr s t r q r t s t r st r t 2 s s t r st t t s s t r t tr s s tr s rt s t r t 2 r s t s t s r t 2 t s rt r r s r 2s t t t r rt st s r 6 r r r st t t t s t s r s t2 t s r s t s s r r t t r st t rt s t s t t t2 t rt s P s s

38 P 2s s r t s s t r t s str t tr t r s t 2 t t r t s t s s q t r t s t s s t t r t s t rt s r tr t t s t 2 r r r 2 s s t t s rt t r ts t r r t r rt s t t s r t rt s t t r s t t r ts t t 2 t r t r s tr t s t tr t s t st t st s tr t t s r r rt s t t s t t r r s s t s tr st t t tr s s t t s t t 2 3 s s s ss s t s t t s t r rt s r t r tr t r2 t t t s 2 t t tr t s 2 r r t t t 2 3 s s t s t s s t t rt t s r t t s t 2 t t s s t 2 str s t s t 2 s ss s t s t t t s r s s t s t r s t r t r rt tr r t r s s s λ mfp = [ 4π 3 nr2 l ln(1/γ)] 1 r r l s t s r s s q t r l e2 k B T s ss 2 3 s s r t t s r rt tr t r2 s 2 t r 2 t t tr t r s 2 t s s s s t s 2 t t t s r K n λ mfp /L s r r t t t2 t L t r t r st t s t r st 2 P s t s r t st s r r t t t s r 2 1 s q t s t t q t t tt r t r t t t f s (r,v,t) r t str t t r t s s s t t r s r r r s t s s r r q t 2 s r 2 t r 1 t 2 t s t r t r st t s r t t tr st t r s r2 t s r r t t rt r s t s t2 str t t r t t r 2 q r 1 r s st t s t t r 2 1 str t s r r s t rs s r s

39 P 2s s r t s s t r t s q t s t s t q t s t t 2 r rt ss t s r r t q t r t s t r t r s t st rt t s r ss s r t rt t r t s s s t t2 s t r r t s s s r r t s t 1 r 2 t s rt s 1 s t s r 2 1 r ss s r t 2 tr r s t s st t s r r 2 1 r rt s t t2 str t t r r t st s s t r r t t t3 q t s f s t +v f s r + q s m s (E+ v c B) f s v = f s t c r q s s t r t s s s rt m s s ts ss t r t s r r s ts t ts s rt r s s s t r s st t s r t s r t r t s q t t t t t r t t t t s t s s t r t t r2 s s s s r r2 r r t s r t s s t r t s r t r q t s t t s q t f s t +v f s r + q s m s (E+ v c B) f s v = 0 s s t t q t s r t r t t s t s s t st r q t s t r t t2 s t 1t s t r 2 s r t t 2 r 2 s t r2 r s s t 2 r 2 s r ss s t t t s s t s t r 2 q r q t s s r t s s t t t 1 r s tr t r s s r t r 3 2 r r rt s r t rt s s r q t t s t s ss t r 2 s r t t r r q t t s s r s s r s s t t s tr s r t s ss sm e m p r s t 2 q t s t t2 r t s t s s ss r t st s r t r t n i,e t + (n i,e v i,e ) = 0 P s s

40 P 2s s r t s s t r t s s q t s t t s r 2 ss t t tr s r t s r t r t r str 2 2 t st t 2 s 2 t r t r s 2 1 t t r t rr s q t s r r s t t r t r [ ] vi m i n i t +v i v i = q i n i (E+ v i c B) p i +R ie [ ] ve m e n e t +v e v e = q e n e (E+ v e c B) p e +R ei r R jk = m j n j ν jk (v j v k ) s t r ss t t s s t rt s t s s ν jk s t s r q 2 t s s s t s t t R jk = R kj. t s s ss t t t s s s t s s t q s tr t2 t r n i = n e = n r r 2 s t s ss t t t t t tr rr t s t2 s tr s r t s s J = en(v i v e ) t t s r t t t 2 r s s t s s t rst r 1 t s r t s t r s 2 s s r t r 3 2 ss s t2 ρ t2 v ρ = m e n e +m i n i m i n t t r ss r ss s tr r ss r v = m en e v e +m i n i v i m e n e +m i n i v i p = p e +p i r t r 1 t s r t t t t t t m e << m i r t r t t t t2 q t s r r t s tr s q t r t ss t t2 q t t t s ρ t + (ρv) = 0 s 2 t q t t r t s s t v t +v v = p ρ + J B ρc rs s r s

41 P 2s s r t s s t r t s t 2 1 s q t s t s2st r B = 4π c J B = 0 E = 1 c E = 4πρ c B t r ρ c s t r s t2 r 3 s s r t 2 r s s s 2 r r t q t t ts tr s t t s [ ] ve m e n t +v e v e = en(e+ v e c B) p e +R ei t t ss ss tr s t t r s s q t s st t s 2 s s t t r s t 2 t r s s s r ss s t tr s q r t t s r r t tr rt 0 = en(e+ v e c B) p e +R ei 2 s q t s s st t t t t2 t tr s 2 r t t t E+ v c B = 1 en v e = v 1 en J ( ) 1 c J B p e + 1 σ J r σ = ne 2 /m e ν ei s t tr t t2 q t s t r 3 s rst t t r s t t s q t s r t tr r ss r ts r s t 2 s ts r s s t r r r s ts t t s t r s r t r r r s t r t s s s r t t t t2 s t s s ss t t t r r st 2 tt r t r t s t ss t t t tr t t2 s r t s s s t r 3 s r s t E+ v c B = 0 P s s

42 P 2s s r t s s t r t s t t t E+ v c B s t tr t r r r t s r t r r t t q t s s st t t r t st r v << c r t s t t t r 1 c q t s t s r r v 2 /c 2 r t t r st t t r s t s t t q t s r r t t2 r s t j = 0 s s q t s rr t r s t t r s t s r 2 t t r t r 3 s s q t t t t t q t E t [( B t = v 1 ) en J B 4πη ] c J r η = c 2 /(4πσ) s t tr r s st t2 ss t t t tr s s t s 2 tr q t p e = p e (ρ) t r r ( 1 n p e) = 0 t t t r t2 q t s t 2 t r t r t t tr t rr t s t2 s st t 2 r r q t s s s r t r r r s ts r t t t q t s B t = (v B)+η 2 B s t s t s s rs s t t s r t 2 t rt 2 s t r t r t rt t s t ts st t 2 s t t 2 s r s R m = L ov o η r L o 2 v o r r s t 2 r t r st t t2 t t s s t t2 R m >> 1 t s t s r t t t t s t t t t q t rt r s B t = (v B) t s t t t tt r q t s t t t t s t t r t t s s t r t s é s s t t r t s t s t t s r r 3 t t r 2 t s ts t s r r t t t t s t r 2 t r t t s 2 t t s rs s r s

43 P 2s s r t s s t r t s 2 s s t s t r q t t t r r s ts t s r t r 2 t 1t s t s t t r 1 t s r2 t t s r t r t q t s s s s r t r t st t s t r 2 q r s s ss t tr s t s s r r t t L D t s s r r t t w 1 pe. r t r st t t r ss r st 2 st s 1 t t t s s t 2r r s T T coll,2πω 1 ci,2πω 1 ce t s t t t2 str t t s q t 2 t r ss r r s tr t s t s s r st 2 r r r t t r r r s t s t t t tr r ss r t t t t r 1 t t s t s t t s r s t s st t t t r t st s r 1 t t t r 1 c t r s E t st tr t t2 σ s t t r s t tr s r q 2 σ tr s q r t t s t E = v c B, t t s t r t s r r t L t t s s s r t s ss 2 s s s t q t r r s t t r 2 s r t t r 1 t 2 t s q t s st t t r r st 2 r ss ρ = st t 2 v = 0 s t r ρ p t pρ 5/3 = st t t 1t s t s r t r s s t s t r 1 t t t s P s s

44 P 2s s r t s s t r t s t 2 r 2 s st 2 t r rt s t r s r t t s st t t s rt t st t r t ts t t r s r t t t st r r r rst t 2 q r st t t s r st 2 t rt r t s t 2 s t t t t s ts 2s r s r s r t t r q r s t s s r r st t q r 2 ρ = ρ o = cte, p = p o = cte, v = 0, E = 0, B = B o ẑ t s s r s t s t s r s f = f o +δf r δf << f o f 2 t 2s r s ss t t t s s t2 s s t tr r s st t2 t s r s t 2 s s t t t rst r r r 1 t t r s t r 2 ss t t 23 t r t s t s ss t t t r r q 2 s r t t t t r 1 t pρ γ = cte, γ = 5/3 t t t t s st t s r 2 q t s q r s t t q t s 1t r 2 rt r t s q t s t s r t t t rt r t s s q t s r t t δρ = ρ o δv ρ o t δv = δp+ 1 4π ( δb) B o δe = 1 c (δv B o) t δb = (δv B o ) δb = 0 δp = c 2 sδρ, c 2 s = γp o ρ o s s t q t s s s r t t s δρ δu δe δb δp s t ts r st t s ss r q r s s q t r t s t t r δf = f exp[i(k x wt)] rs s r s

45 P 2s s r t s s t r t s t t ss r t2 s t ˆx 1 s s t t k = ks (θ)ˆx+k s(θ)ẑ. t t t t q r s s tr s B o s r t t ẑ 1 s t r s t t r s q t t t t s r s t t q t s t t s rs r t s w 2 = k 2 v 2 Acos 2 (θ), v A = B o 4πρo w 2 = k 2 [ v 2 A +c2 s 2 ± (v 2 A +c 2 s) 2 4 v 2 A c2 scos 2 (θ) ] q t s t s rs r t r t s é q t s s t s rs r t r t t st t s s t s t s t s t s t r st 2 t r s s r t s r t r t r tr st t ss tr s r 2 s s s r s t 1t t r t ss t t rs 2 r t s rs r t s q t s r t r t t s t2 t t r r s s v φ v φ = wk 1. r s s r t t s t2 t é t st s t s s st t t t s r s t r r t s s s t s t2 ss t t t r t θ. s s s r r t r t t B o = B o ẑ. q t s r r δb x Bv 1 φ cos(θ) 0 0 δv x δb y = 0 Bv 1 φ cos(θ) 0 δv y δb z Bv 1 φ sin(θ) 0 0 δv z vφ 2 v2 A c2 ssin 2 (θ) 0 c 2 ssin(θ)cos(θ) δv x 0 vφ 2 v2 A cos2 (θ) 0 δv y = 0 c 2 ssin(θ)cos(θ) 0 vφ 2 c2 scos 2 (θ) δv z q t s s t t t t t t2 rt r t t t B o δv z s t 2 t t t rt r t δb. t 2 q t s s t t δv y s t t δv x δv z s t s r q t t r t2 r t é s s (0,0,±v A ). t r r s t s r s t2 t t s r t t P s s

46 P 2s s r t s s t r t s A F S r P s t2 t t r r s r 3 t t é t2 s é st c 2 s = v 2 A q r t t s t2 q t v A r r ss t r t r t t rs t s 1 r ss s 0 0 δv = 1, δb = Bv 1 φ δv δb r r r t t t t B o t t r k. r r δv s r t δb. t rs r t r r s 1 r ss s s vφ 2 c2 scos 2 (θ) cos(θ) δv = 0, δb = Bv 1 φ (v2 φ c2 scos 2 (θ)) 0 c 2 scos(θ)sin(θ) sin(θ) t s s t t rt r t s r r t t t r s s 1 t r q t rs s r s

47 P 2s s r t s s t r t s s t r t rs t t r rt s t s r é s r tr s rs t t q r t r ss t s t r st r r s t t s ss t t t t s tr st t t t st t s s r r ss δρ 0 2 s s 2 t t t s r t B o r t s t r t t t str t t s r ss r r s s s r t st r t t s t s s s r s t r t s t t s t2 t t t s r ss r t s r t s rt r t s r t s t s r t s r t t t s s t t s s t s t t t st 2 s r t t s t q t s s r ts 2 s r s t q t s r t q t s s r t t t 2 r s s s t s t t s r s t2 r t s tr s q t s r t r r s t s s ss t t t s s s t s 2 tr r t t s s p i,e = p o i,e ( ) n γ s t t t 1 s q t s t r 3 s t σ s q t t s s ss rs t q t s n o n dv dt = ( B) B β (nγ ) E = (v ε n B) B ε n βe (n γ ) v e = v ε n B r t ss t ts r n o p o i,e L o B o v o = v A = β = po i +po e m i n ov β e = po A 2 e m i n ov A 2 ε = c w pi L o = v A Ω ci L o Bo 4πmi r n o P s s

48 P 2s s r t s s t r t s ε r t r s t s r t r s r s t r t rt t s t t t ε 0 r r t q t s 23 t r s s t r s s s t t r s s t s t 2 rt r r q r t s s ss ts t s q r s 2 n o = 1 p o = 1 B o = ẑ v o = 0. s r s t r tt s rst r r r 1 t n = 1+δn v = δv B = ẑ +δb p = 1+γ δn r s t s t q t s s s r t rt r t s δn δv δb s t ts t s q t s r st t s ss r q r s r s t t s t s t t s q t s t t r s q t t w δn = k δv k δb = 0 w δv = γβkδn (k δb) ẑ w δb = k [(δv iεk B) ẑ] ẑ 1 s s t ˆx 1 s s t t k = ksin(θ)ˆx+kcos(θ)ẑ r B o s r t t t rt r t δb r tt s δb = (δb cos(θ),δb y, δb sin(θ)) 1 r ss t t 2 s t s s q t t t r t t2 rt r t s r r s t t 2 δv = (δv cos(θ)+δv sin(θ),δv y, δv sin(θ)+δv cos(θ)) r q t s t v φ δn γβ v φ sin(θ) δv 0 0 v φ cos(θ) 0 0 δv y = cos(θ) v φ 0 iµ δb y v φ cos(θ) δv 0 sin(θ) 0 iµ cos(θ) v φ δb rs s r s

49 P 2s s r t s s t r t s r µ = εkcos(θ) v φ = wk 1 t t ts µ = 0 s t t r r t r s tr δv y,δb y rr s s t r 2 r 3 é s r s st t r s t r r t r 2 r 3 é s s t s r 2 t r r t s sin(θ) = 0 t r s q r t t s t s r t t r r t t st s t s s t s r t r r t B o t r s t s s(θ) = 0. t r st 2 t t s t t ts t t rt r t t r δb y,δb t t r r r 2 r 3 s t r t t t r t t tr 1 q t t s rs r t s t vφ 6 v4 φ (1+γβ +µ2 +cos 2 (θ))+vφ 2 (µ2 γβ +(1+2γβ)cos 2 (θ)) γβcos 4 (θ) = 0 r r t s 1t t s r r t k ẑ cos(θ) = 1 t rt r t s s t st s r t t r s s r t r 3 2 s ss s t2 v ± φ = ± (γβ) r r t s t2 s s 2 t s s v ± φ = ± ( γpo m i n o ) t t r t r r s rr s t st rs st t s r s r 2 tr s s t s r s t2 t s r s s vφ σσ = σ µ µ 2 2 +σ +1 4 r σ = ±1 σ = ±1 r t t s r r t µ = εk s t s s r r r 2 r 3 r s rs P s s

50 P 2s s r t s s t r t s r 2 tr s s r 2 tr r q 2 σ = σ s2 t t 2 s t t r t 2r r q 2 k. vφ IC = w k = σ [ εk 2 + εk 1+ 4 [ 2 ε 2 k 2] εk 2 + εk 2 ( 1+ 2 )] ε 2 k 2 = ± 1 εk w(k ) ε 1 r r t r q 2 t s s t s t t t rr s s s s w(k ) v Aw pi c = Ω ci r t t r t r r t s s s t r 3 t t r k t s s vφ IC 0 t s t r 1 t t s rs r t 2 v 2 φ (µ2 γβ +(1+2γβ)) γβ r t r s t s r v IC φ σ kε, σ = ±1 2 r t s 1 r ss r t s t2 t tr 1 q t t δb = (1, iσ,0) δv = (1, iσ,0) r ts r t r t s2st (ˆ k,ŷ,ˆk) 2 t t t q t s t s t t w > 0 σ = 1 δb = (1, i,0) r t t s t s s s s t r t t 2 t s t w < 0 σ = 1 δb = (1,i,0) s t s s s r t t s r r r t r s rr s t r r 2 r 3 t t r t t s r B o t t s s s s s t s s r s s t r 3 s w > 0 t r t s r t ẑ w < 0 t r t s t r t ẑ. st rs t s s r t st r σ = σ t t k s t2 t s t s t r 1 t s vφ WH = w k = σ[εk 2 + εk ] = σεk 2 rs s r s

51 P 2s s r t s s t r t s w(k ) σεk 2 r r t r q 2 t s t ts rr s s s s w(k ) σ v2 A k2 Ω ci st 2 t r 3 t t s k t s s vφ WH σεk t s 1 r ss r t s t2 t tr 1 q t t t t δb = (1,iσ,0) δv = (1,iσ,0) w > 0 σ = 1 δb = (1,i,0) r t t s t s s s s tr r t t t t r w < 0 σ = 1 δb = (1, i,0) r t t s t s s s r r t r s rr s t r r 2 r 3 t t r t t s r B o t s s s s tr s s r s s r t r 3 s w > 0 t r t s r t ẑ w < 0 t r t s t r t ẑ. s r2 t t rt r t s rr s t t 2 tr st r s r r s t 2 s t r t s s δb IC/LH = [cos(kz wt),σsin(kz wt),0] δb WH/RH = [cos(kz wt), σsin(kz wt),0] r δb IC/LH t s t 2 tr s r t r 3 s δb WH/RH t s t st r s r r t r 3 s σ = 1 r w > 0 σ = 1 r w < 0. r s 2s t s rs r t r t s r t r r t s ss r ss r rt r s s t t s t s r st s w R r t s s s s t r s st t s r r s t s s t s s s s r t 2 tr s r r s r t r t t 1t 1 s r s rs s t s s s t r st r t t s r s t r rt r s t t s t s s t r 2 r s t t s t s t s t s s r r rr t s r t 2 tr s 2 s t r r q 2 t r r r t s r t t t s r t s s t t r t 2 tr r q 2 P s s

52 P 2s s r t s s t r t s 5 4 WH 3 w (k) / Ω cp IC IC WH k c / w pp r s rs r t r t 2 tr t st r s t r r t r ss s r r s rt r s t t s r r tr r 2 ss t t r s r s r2 t s r 2 tr r s s r rt s r t st t r t r r 2 r 3 s t r t t s t 2 r s rr s 2 r t r 3 s t r t t t s s 1 t r r s t s s r t t r t t s t 2 r s t2 r t B 0 s t 2 tr r t r t B 0 t t t r s t t t r s s t t r 3 t st t t 1 r ss s δb LH = [cos(kz wt),sin(kz wt),0] rs s r s

53 P 2s s r t s s t r t s t w > 0 t t r t tr t r2 t s r v > 0 z +ion = v t r +ion = r L [cos( Ω ci t),sin( Ω ci t),0]. t Ω ci > 0 r r t r r r t t r s2st z = z +v t r +ion = r +ion t s r s δb LH = [cos(k(z v t) wt),sin(k(z v t) wt),0]. z = z ion (t) t r r z = 0 t rt t s s t r s t r s ts kv t wt = Ω ci t r t s st t w +kv = Ω ci r t s t s r s t 2 s r r s t r t t s t 2 r t r 3 r t st t r t r t t t s s s rst t r s t r t r t s r t r q 2 t t r 3 s s 2 t r rt t r s t t t 2 r r s t s q t t 2r r q 2 r t s r s tr r t r 3 r t t r s t r r s r s t s t s t s r t s s t t r t t t 2 r t t t2 r t B 0 r t r 3 s r t s r t B 0 t r r r t t δb RH = [cos(k(z v t) wt), sin(k(z v t) wt),0]. t v > 0 z = z ion (t) t z = 0 t rt t s s t r s t s w +kv = Ω ce r t t s r s t 2 P s s

54 P 2s s r t s s t r t s s r s t s s r rt s t r t r r t t s t 2 t t s s 2 tr r s t s s t s t 2 r s t r t t r t r 3 s t 2 r s t r t t t r 3 s ss s rs t s t 2 r s rt t s v > V ph t rt s s r t t s r t s 2 t t t s t t t s r t r 3 s s r t t t s s s s t t r 3 s t s t r t s t s t s s r t s s r t r t s t 2 r s r t r 3 s r r t t s r t r 1 t ẑ 1 s r r v > 0 t s r t r r r s δb RH = [cos(k(z +v t) wt), sin(k(z +v t) wt),0]. r s t s w kv = Ω ci r t t s r s t t s s t r s t t r t t s t 2 r r t r 3 t t 2 r t t s r t t 2 r s t v > V ph = w/k t r q 2 s 2 t rt s q t ts 2r r t r 3 t s r rs r t r 3 s s r t r r r t s t t t r 3 t s s r s rs t tr s t r 3 s v > 0 t s r t tr r r r r s ts δb LH = [cos(k(z +v t) wt),sin(k(z +v t) wt),0]. r s t s t w kv = Ω ce r t t s r s t r t s s t s rt t t str ss t t s t t r 3 s r q s t s r r r t r t 2 tr r q 2 r s t tr s r t2 2 r t st rs s r s

55 P 2s s r t s s t r t s ts s s t s t r t ss t 2 s t t t s ts t t r t r 2 r q t s s r 2 tr t r s t s s t s ss t t t r ss s r s r t r t r t t s t rt str t s r r t r t r s tr s r t rt t t st r t r ss s st t t t s r s s r 2 s 1 str t r 2 t 1 str t s t r t s ss q s tr t2 s tr t r t r s t t s t rr t t r s s r t st ts t r r s r r t r s t tr t t s r t rs s s t r t s t t r s s s r r s t s s r s t q t t r s str t r s t r r t 2r r s r t s t r r r rr t s s 2 p e s s q t t r s t st t s s r rt t r t rs ss t t s t r 2 ss t s s r s r s rs t t r t r ss t s t t2 t L t str t r s s r t t t t s t ss t s s s 3 s r t r s t t s r r rs s r + s t t s s t r s t r2 s s t t t r t ss t s t s t s s t r r = r ss s rs t L λ D /L s tr t2 λ mfp /L s r (c/w pe )/L tr s t (c/w pi )/L t r L /L 10 2 P rt t2 s tr s r s s r t s s 3 s t s rs t t t r2 r s 1tr t r t s s t r t t t 2 t t t r2 s s P s s

56 P 2s s r t s s t r t s λ D /L 1 t s t ss t q s tr t2 t s s s r s t r t s t t t r2 s s 3 λ mfp /L s s t t 1 t r t s r s t t s r s t s s s ss t s r r t s t s s t r r t 2 t s s t t t s s 1 str t s tr r ss r 1t t t s s (c/w pi )/L (c/w pe )/L r t r t r st t s s s t r q s r t tr s r q s t s ss t t t s t r q s t r r t tr s r q 2 t s t r r t s r q 2 s s 2 tr s s t t s s r rs t r s t 2 r s st r t t r L /L r s t r r r s s r t s r s t str r s rs s t t r t s r s t s r t t t 2r r s ts t s s t r s r 2 t rs t 2 t t 2 t s rt t t t t t t s s r r r s t t t + s t s r t t 2 s 2 s r t s r r s t 2r r s t r2 s r r t t s s t r r t str t t t t r t t r2 s rs s r s

57 P 2s s r t s s t r t s s st s s s s s s r t s s 1tr t t s st s rtí s 3 s q r t r t r s t s 1tr t s r q r t r í 2 2 s tr s r s tr rtí s r s 2 r r s r t s s r3 r s s q s t r r st s s r3 s r í q r s t r s s rtí s í s t st s t s rtí s 2 s r s tr s rtí s r q r s r s r s s r 2 r t t s s t r s t s s rtí s s rt t s ás ú q s t r s t s s r 2 q s t 3 ét r 1 s tr r s 2 st t s s s st r s s s s s tér s s r ó t r st ít r s t s t s t ór s t s r s t rtí s s sí t é s r s ét s 2 í s s s s s s tr s t rtí s r s s ét s st t s 2 r s r s r ó ét s r ó t3 2 s t rí t r á t rí s t s s s s rtí s s t ór s s rá t 3 s r t r r t r s r s s í t s s t s P s s

58 P str ts t s 2s s s r t s r ts s t r s r s t t t s t str ts t t r s t t r t s t s s r 23 t r t t t rs rt r 2 s t rs r 2 r t ss ss s s st t r s ts r s t r r rs t t s t r s s r 3 t t s 2s s s r t s t s r ts s t s t s s rs r 2 r ss rs r 2 r s t r t s str t s r t t r t r t r rs t r t r t r t r2 tr 2s s t s r ts r r2 ss r r t r 3 t s r t r s r ss s rs t r t s t str t 2s r rt s s r r s r s

59 str ts t s 2s s s r t s r ts t r t t r 2 t s r t t st s t t r t t s t ts t r t t t s r t r t r t t r str t r t t s r t 2 t r t s t rs s r t t s r s t r 1 s st 3 s r t q t s r r t s t str ts t rs r t r t r ss tr t r t rs r t s r t t r t 1 r t t t t r tr t t r t t s t s s 23 t r 2 t st t r s r t s t s r t r t tr2 t str ts t r t s r t s r t t ñ t r t tr2 r r t ss s st s s t t r t r2 tr t s rt t r t r rs t r r s t s r 2 r r t r ss s s s s t s s s t r r t r ts r t t t r s s t t s s t 2 s t t t r t s 2 t rt t s r s t s t 2 s t s r t r ts s s r t r r s t r r r t s t s s r r r ts t t r t r rs r t t t r r s t r s s r t P s t 2 rt r t s t s r t r t t rt r t s r s s r t r ts ttr t t t 2 t t s r s s s r s r r t r r r t 2s s t s st ss s t s s t s t 1 ss 2 r ss r s r t s r t r t t r s t t r t r 2 r st 2 t s t r r s s t t t r t t r t r r r t s st r t rr str 2 r r r t r s r r t t t t 2 s r t s s s t t st s tt r t st s r s r t 2 r s P s r ts P t r r s s s r t r s t t s s P s s

60 str ts t s 2s s s r t s r ts r r t r s t t t r s t t r2 r t tr2 t s t s st t s s r 3 t s s s t r t r t s r t s t rt s r ts t s r t 2 t t t rt r st t s s r t t t r r r t t r 2 r t r rs r r t 2 rs r r t r 2 2 rs t t t 2 t r s r t s t t t t t st t t t rt t r 1 r t t t r tr t t r r t r t t s r t r rs r s s t t t str ts r s t s str ts t r t t s r t tr 2 t t 1 t t t t rs s s s rs r t t t t r s t s r s t s t 1 r t r ñ t t r t t r t rt t rt t t t s r t r 3 t s t st s t r rs tr s t rs s r s

61 str ts t s 2s s s r t s r ts r str ts r t s r t t s r s r t t r st s r s st 2 t t r t t s r t t r t s r s r r t t t t t rs t t r 1 r t s st t tr 1 1 t t t rs t t r s t t r s r ts t t str t s 2 r ± t ± t t t t r r s t t t r r t str t t r t s t t t r s s s t t t r t s s s 1 r t r s t t t t t s r t r s t ss t tr2 r t ñ t P s s

62 str ts t s 2s s s r t s r ts t t t r s r t t 2 s t r t s r t t s r t t t r s tr t r t t ñ t s s t r r2 s r rt t2 t t s t s r ts r r t t s r t s t r s r 1 tr t s r t t s t t ñ t 2 s r t s r t P r ts t s tr t s st s s t s t r t s r 1 t 2 s s t r r t t r s s s 2 t t t t ss t r t t t s t r r t r s t s r t t r t 2 r r t s t s tr t t r tr r t t r s tr s tr t r s r t t tr 1 s t r 2 t t s st t t s r tr st t 23 r t π r s 2 s t rs ). str t s t t r s r s st s t s t t r t 2 s r 2 s r r t tr 1 t t s t r 2 s t r r s t t r r s r 2 r s t s E E = t 1 t r t r s t s s t t r s 2s s t t s str t s ts t t t t s r t s r t 2 t s s r ts r t r t t t t r t t t str t t tr s t r s r rt s r t r r s r t t t rr r t 1 t t str t tr s r t r r t t t r s t t str t t t t r t r r t t 2 r r t t tr s s t s s t str t t t r 2 s tr t tr s t s s r t t r t 2 23 t s t t t t t t ts tr s t t t r t r r t 2 t s r t t t r t t t t s rr s t t t t s r t s r t t s r tr r r t s r r s t tr s r s r t t r s s t t s r t t tr s s r t t t t t tr s r r s t t r t t r s 2 r2 s r r t t r t t r s s ss t t t rs t r t s r rs s r s

63 str ts t s 2s s s r t s r ts r t t tr r t t r s t tr s r t t s t t s t s s t t t s r t2 2 tr s st t R M. t s t s s 23 t r t 1 s r r r t s t r s r t 2 t s s rt t t t t t t str t s r r rt s t s r r r t rs s s t s r s t2 t r t r s t2 r ss ss ss 2 s ss s r t t t r 2 t t 2 s t 1 r t t r s2st ts r s s t s s t t r ts t r s 2 r r 2 t t r r t2 ss st rs ss t r t r t r t r 2 t t 1t s ss t t s r t r ts r t t ts s t t P s s

64 str ts t s 2s s s r t s r ts t s t t s ss t t r t t t r s str t r 2 r t r s t t s r t r s s r t r 3 t t s r t s r t t t tt r t s t st 2 t s t r t t t r s t s r ss s r 2 t r r t 2 2s t s t ss s 1t t t 2 r 2 2s t t t s 2 ss s t r t t 2 2s q t t str t s ss s t r t s r ts t s r t2 t s r t s t s tr r t ss s r t s r s t r 2 t r t r s st s st r q t r s r q t t tt t t st r t t s P t t s P rt s P t t t r s t str ts s s t 2 s Pr s t ts rr2 st t s t str ts t t r s t t r q t t s t s s s r t s t r s r str ts r ss 23 t s r t s r t 2 t ss t t r rt2 t t s t s r t r t r t ss P s tr t r P t tr r s t2 s r t t t r t r t P s r Pr str t P P r tt t t r s t r s r t t s str ts t t r ss t 1 r t s sts t r t t r 1 t t t r s r t t t r r ± ± r s t 2 t r s r ts r 2 t t r s t 3 3 r s t 2 rt2 t s t 2 t t t t r t s t t t t t t st r s s r ts r st t t r t s t s s s s r t r t s r ts rs s r s

65 str ts t s 2s s s r t s r ts r r t ss s r t 1tr t r tt s t r s ss P rt tr t r tr tr t r s r P ss P rt tr t r tr tr t r s r P s s r tr st t 23 r t t t ts tr s t r 2 r t r 2 r s t E/E = 0,17 r r s t P s 5,2 160 t t s t s s s tr s t2 st t s r r t tr str t t t t s s t ss P rt tr t r ss tr t r P P s s s t r s t rs s t s t r st t s 8 20 s s r s t 2 t r t t t rt t s r tr st t 23 r t r t r t t t r tr s r t s tr t t t t t ts s t t t 23 r s t t 2 P s s

66 str ts t s 2s s s r t s r ts rt s t rt r r r 2 r r r t rr r tr s tt t r t t t 23 r P t s s s t rr s t r 2 r r s tr r r t t s tr r s t st r 2 s s t s t q r t t r r tt t r 2 s s r str t s t r t q s t 2 s 2 r r t s t 2 sts s r r t P str ts t s t t s ss 2 1 t t r r t 2 t t t r s str t r t tr t 23 r r ts t r t s r t t r2 r ts tr s t s tr t s r r t s r t t t r s r tr s s t tr s t r t r t t r t str t t r rr r r t P r st rt t ts r r r t s r t t 2 r s s t 2 t r s tr s r t r t t r t s t s s r s r r t t r r t t t P s s s ts s t r 2 t st ss t s s s str t s s t r r t t s r t s t 23 r s s t r t s t 2s s s 2 r t 2 rs s r s

67 str ts t s 2s s s r t s r ts t t r s t rs r s t t r t r 2 st s r s t r 2 st s 2 sts s P s s rs r t r t t t r t t t P str t r 1 s r t t s r t 1 s t r t r t P r r s t t rt t tt r t s t s s r t s r s t r t r 3 t t r 2 r t t s r t ts s t t r t ts st t t s s P s P P s P st t s sts t r r t tr t s t r rt s r t t s r r P r tt t t r s t st 2 s t P t r q 2 r s r t s s t 2 r t t st t s r t tr r s t2 r t P s r t s t t t P s r ts r st t s r t tr r s t2 t r t r s r t t t P t t 2 r st t t tr r s t2 t r s r ss s t 2 r s t t s r r t r 2 tr s t s s str t r r s t s s s s t t t s s rr r t s t tr st t tr st t ss s r s r 2 t t s r t tr s t2 s 3 r r t P str t r s r s r ts r s r2 s t t 2 t s t t s ts r t r2 r t r t r 3 t t tr s t2 t s t2 tr ts r t r ss s t r r s r t t str ts s r t 2s s t r s r r t st 2 t t r 2 s rr t P 2 st t t r 2 t t t r r t s r t st 2 r rt s s s t 1t 1 s r s 23 t r t t t r t 23 r P s str t P r s 1 r ss P s s

68 str ts t s 2s s s r t s r ts t t r t ts t s r t s t s r t s r s s t rr2 r s t s t t r t t t P 2 r t s r ts r r rr r s t r t r r s t 2 t t s r t2 t t t ss r2 s sts t s t t 2 r t r t s 2 r r s t 2 t 1 r t t t r t r2 s r t 2 s r s st r s s r 1 t s2st s t t r s s rs t t t t s r s r t r s s r t t r s r s str ts 2 r ± s s t t2 r t t s t s s 23 r s t t s r ts 3 s 1 r ss t t r s str t P s 1 r ss ss r s t rst r s ss t t s t t r s r t s t t 2 t r r t r s s s s t r t r str ts t rr s t t r 23 r s s s r t t s t st t t s s r t t s 1 r ss t t r s sts t tr 1 1 t s s rs t t t 2 t t r r t 2 tt t t s r t s t s s s r s r ts t s ss t s r t t t t r t r t 2 t s r t r t t t r 2 t s r ts s s r q 2 t s r ts 23 t s t s s s 3 P str t r s s r s s rs t r t tr t s s rs t tr s tr t r t ss 23 r t ts s t r 2 r t q q t r r s r s s t r2 s t s t r s t s t s t s s 23 s r t rs r r r s 2 s 1 s 2 t s r t2 t r t s t2 r rr t 2 t s s 2 t t t t r 2 2 s r t r 23 t s t rs s r s

69 str ts t s 2s s s r t s r ts ss t r t t t t r r t s rr t s r t s t t r t r s t ts r r t t s 2s s t s r ts r 2s s t t r 2s s s t r s s r t t t r t st t r t r t r t s r r 1 t 2 s rr t 2 r r t r t r tr s t 2 r s 1t t t s t t r t t r t r ˆn r r 2s s t t r s r ts t 2 s r t s t s t r t str t r q st r st t ˆn t t t s t s t r t t r t t s t 4B (m) ˆn6 m = 1,...,M s t s st t r r s ˆn s t r 2 3 t σ 2 = 1 M M (B (m) < B >) ˆn 2 m=1 r t r < B > s 2 < B > 1 M M m=1 B (m) r t 3 t s s t t t r 3 t str t ˆn 2 = 1 r t r t r s t s t t r q t s r tt tr 1 r s 3 Mµνn B ν = λn µ ν=1 r t s s r ts µ,ν = 1,2,3 t t rt s ts t s2st Mµν B < B µ B ν > < B µ >< B ν > s t t r tr 1 r q t s t t t λ s r t s λ 1,λ 2,λ 3 r s r r Mµν B MB µν s s2 tr t s r r t rr s t rs x 1 x 2 x 3 r rt t r t rs r r s t t r t s 1 t r t r t t t r r s t 2 t t t t s s P s s

70 str ts t s 2s s s r t s r ts t t t rs r r tr r2 s t t r 1 x i kx i kx i i = 1,2,3 r t rs rr s λ s r r s t t t r s t s ts r t r r t r r t ˆn rst t r t tr 1 Mµν B q t t r s t s r t t ts t r s λ i t rr s t rsx i t rx 3 rr s s t t s st λ 3 s s s t st t r t t r r t t rr t s t r r t λ 3 ts r r s ts t r t t t t st t r t rs x 1 x 2 rr s t t 1 t r t r r t r r t t tr s t 2 r s t x 1 x 2 x 3 rr s r t rt r tr r s s t s s r rt r 2s s r r 2 r 2 s t t rs 4B (m) 6 t ss r 2 t r s r t r ss tr s t 2 r r r t t t r s t t r tr 1 M B µν r r t t r s t t r r t s2st t s 2 23 t t t s t t t tr 1 Mµν B s t t t r r r t s r t rs rr r st t s t t 2 r t rt t s t r t s t t rs (x 1 x 2 x 3 ) t r tr 1 M B M r st t 2 r r rt r t 2s s t t r q t r t s r st t s t 2 st r s (M + M) (x i + x i ) = (λ i + λ i ) (x i + x i ) r i = 1, 2, 3 rr s t 1 t r t r ss t t M r s t 2 r 3 rs t s q t s M x i +M x i = λ i x i +λ i x i q t s r tt t rt r s s M s r r t t t q t r s ts (λ j λ i) x ij = M ij λ i δ ij r x ij s t t t t t r x i. M M r t s2 tr tr s M ij = M ji s t s r q t x ij = x ji rs s r s

71 str ts t s 2s s s r t s r ts q t2 1 r ss s t t t t t rt r t rs st r r t r tr q t t r tt s x 31 = x 13 = M 13 /(λ 1 λ 3) x 32 = x 23 = M 23 /(λ 2 λ 3) x 21 = x 12 = M 12 /(λ 1 λ 2) x ii = 0 t t t t r r 1 t t q t t s x 31 x 32 s r r s t t r r t t s r s t t r x 3 t r s x 1 x 2 r s t 2 r 2 x 21 r r s ts t r r t t x 2 t r s x 1 t t s t t t rr rs t t r t t t rs r r t t r s M rt ss t r 1 r ss r M ij 2 r B (m) 2 B (m) + B (m) t t M r B (m) s t s t r s t t t s r ts t r r s t r r r r s r 3 t s t s t t s r r t t r s r r ǫ 2 [λ 3 /(λ 2 λ 3 )] 2 /(M 1) 2 r t t2 t r s t s ϕ ij = ϕ ji = << ( x ij ) 2 >> 1/2 =<< ( x ji ) 2 >> 1/2 = λ 3 (λ i +λ j λ 3 ) = (M 1) (λ i λ j ) 2, i j r <<... >> t s t s r ϕ ij r r s ts t r rt t2 t r x i r r t t t r r 2 r t r x j st t st rt t2 t t t r t t t r x 3 s s t r rts t rt t2 t r ss t t t rr s r λ 3 t t rt t s ss t t t r rr r st t s r x 3 ss t t t s rr rs r t r t t t t st t st rr r st t r < B > x 3 s λ 3 < B > x 3 = (M 1) +( ϕ 32 < B > x 2 ) 2 +( ϕ 31 < B > x 1 ) 2 r 1 r ss s r tt r t rt t s < B > x 1 < B > x 2 t t s rr r st t s r s 2 ss t r st P s s

72 str ts t s 2s s s r t s r ts t s 2 s t st t t r t r t r t ss t t t s r t t t s s t r t t t r k st 2 t r t s t t t 1 t r t r s t t r t r 3 t t s s 2 s r s t r s r t t s t r s s r t rs r t r t r t s2st s t s r t s r r s t t s r t s t 4B (m) 6 t r r r t s2st t t t r s s s ts t t t t r s q t 2 r s r s 2 t r t s t r r r s t rr s t t r r t k t r t t t s t tt r t r λ 3 λ 2, λ 1 >> λ 2 t r 3 t s q s r t s t r 3 t λ 3 << λ 2 < λ 1 t s r r r 3 t λ 3 << λ 2 λ 1 s s s t t r t t s t r t r s t t t t r t x 3 t ts t t t B 1 B 2 t r s t s s r 3 t t r r r t s r t r r s t r t t t r t r t t t t t t r k r ss t t t s t x 3 B o =< B > s t s θ kb s ) (ˆx3 B o θ kb = arcos B o r s 0 θ kb π/2 θ kb s t t r t s r r t r r r r q t t t t r r r t s r t s r t r r r s r r r tr s r s r t t s r s x(n) s s X(w) = x(n)exp( wni) n= r X(w) s s t x(n) ts r q t ts s t t t X(w) s r t r π. r t r st t r q t ts t t r r s t t 1 s t s r s r t s t t r r t s s ts t t rs s r s

73 str ts t s 2s s s r t s r ts r s tr s t2p(w) s t r r tr s r P(w) s s t r s t2 t s t r (w,w+dw) t s s P(w) = X(w) 2 t r r s P(w) s s t r str t t r q s t t r s st r q 2 t t st s t t t2 t 2q st r q 2 s s f Ny = f s /2 r f s s t s r q 2 t s r q 2 r s t t s tr s 2 t rs t r T r t s tr s t t r 23 s r ts s r r tr s r s t r s tr s t2 s t r t t t t r r q 2 t s s r ts 2 s 2 r r s tr s s tr r s s tr r s s st 23 t s r ts 2 r t t s t r s s r t r s tr s t2 s t t 2 r P(w) ss t t s t st 2 t t t s r t 1 s t r t s r t s s r ss rr t t s r t s s r ss rr t r xy (l) t t r tr r2 s r t s s x(n) y(n) t t N s s s N k 1 n=i (x(n) m x )(y(n l) m y ) r xy (l) = N 1 n=0 (x(n) m N 1 x) 2 n=0 (y(n) m y) 2 r i = l,k = 0 r l 0 i = 0,k = l r l < 0 l 1 s t r t r s t r t 2 m x m y r t s t rr s s r s s s r tsxy t s q r xy (l) t t s s rr t t r r r r 1 x r y t s t r t s q s s r t t r t s s t s q x(n) s t s t s q y(n) s s l s s s t t t s r t r r t tr 1 t s ts r 2 / s t r t r 3 t s t r s t t s s rr rs t t t r ss rr t r t r s t r t s s t t t s s rt t t st str ss t s t ss s t t t t s t x(n) y(n) r s t t s r q 2 s s t r t s r q s t t t r t tr r t t r r t ss r 2 t s r r t ss r2 t t r t t t s s t t t t r P s s

74 str ts t s 2s s s r t s r ts r r t ss t t t s s x(t) y(t) s 2 C xy (w) P xy(w) 2 P x (w)p y (w) r P x (w) P y (w) r t r s tr s t2 t s x(t) y(t) r s t 2 P xy (w) s t r ss s tr s t2 sp xy (w) = X(w)Y (w) s r t s r s t r rr t t t t s r s t r q 2 s t s r q t t r t t t t s s t r w 2 s t s t st 2 t r t s r t s t r t s r t r 2s s r r r t r r rr t s t r s r r r t tr s s r r r t r r 2 s s r 1 st r r t 1 r t t 1t r 1 t r t s t t r t q s st t r2 tt r t s t2 s s r rr t 2 r s r s t s s q t s r t r t t s ts t rst r r r 1 t t t st 2 t t tt r r t t t str t s r s s r t t tr s s r 12 r E t 2s s t s sts t r t2 HT t t st r s t s t s r ts t B s t2 v. 2s s s t t 2 t ss q s st t str t r s 1 st t t t r s r s s q t 2s s r 1 t r t 2 t r t t r t2 HT t t 3 s t sq r t tr D( ) 2 D( ) = 1 M M (m) 2 = 1 M m=1 M (v (m) ) (m) 2 m=1 r v (m) (m) r t s r ts s t2 t m s r t M M t r s r t s t r t t t r r st 2 s r t r t2 HT s s t r t2 s s r r r t 3 t t r D( ) s t t q t s t r HT HT = 1 0 < (m) v (m) > rs s r s

75 str ts t s 2s s s r t s r ts r K (m) µν = B (m)2 ( δ (m) µν B(m) µ B ν (m) B (m)2 ) (m) s tr 1 ss t t t (m) t t r ts ts K µν (m) r r t t t µ,ν t ts B µ (m),b ν (m) t t t t s t2 B (m) 2 t 1 r ss s q t δ µν (m) s t r r t tr 1 r ts <... > t t r t s q t t2 r t s t s r ts 0 < (m) > r t r 3 t t q t2 t t r t t r 1 t r t r t t r t D( HT )/D(0) t rr t t R HT t t t tr s c (m) = v (m) (m) (m) HT = HT (m) r r r é st t t s r s r 1 t t rt t r s r é str t r s s s r t t s t t s r rr t 2 rs r r s t t s str t r s t ts t s t2 t t t t s 2 rs r s s t t n r r n = ˆn ˆn s r t t s t t2 s st t P s r s r ss s str t r s s t s s t t = ± A r A r t r t s t s é t s r s t 2 q t s t s é r t s r t s s r r t t r r r r r r t s r r r t é r t r tt s s 1 r P s r = ± A r A r t s t2 t é t2 t r r s t 2 s s q t s s t t t 2s s t t r t é t st r r r s s 2 t st 2 s r t ts t r s s t t s r rr t 2 rs t st s t r t t t s r s t r t s t t r 2 t s s r s t t é t st s sts r 1 t r r r t tt t st t s t2 ts t r P s s

76 str ts t s 2s s s r t s r ts tr s r t t t r st t rr s ts t t é t s t é str t r t s tt r t s s rr t t s ± t r 23 ss s s r ts s t 2s s t é t st t t r t t s s r s s r t s s r t t r 2 t s t t t rs s r s

77 str ts t s 2s s s r t s r ts s st st ít s r s s té s s str t s q r 2 r s t s r r s t t s s 3 s r s s t s ít s s tr s r t s s s rs r 2 r 2 ss q 2 rí s r s t s r s t s r rt 2 tá st ít t é r s s s ét s á s s s s s t r st s r s s s s s t 3 s st t s s s t s ó rs r 2 r s s r r s s t s trí r t s rr s t s sí t é s s s tó tr 2 r tó tr tr s r ás s r s r t s t s s ó ss 2 t tó tr s tró tr tr s 2 r t s 2 str t s s 2 r q s r r st s r 3 s s s s s s 2 t 2 s r s s tó tr 2 str t s r s s 1 r ss 2 tó tr r s s ét s á s s q s s r t s s s s t s á s s r 3 í r s r r r s r t rr ó r 3 tr s ñ s s r t s r á s s r t st é P s s

78 P t t 2 t t s r s s t r s t t t st 2 t t t 2 t t r s ts r t t r t t t 3 s t s r t 3 t st r rt r 2 t r st t 1 r 2 t t t 1t r t t 2 t t t 2 s rr t s r t 3 t s 2 t r s t r ts t t2 t 1t r s r ts r t r t s q t r ss s t t t t ts t s 1 s2st t s t ss t s t 3 rt s t s r r s r ss s t r s ss t t t r s rr ts t st s t t s r s rr ts s s t r s 2 t ss s s t t 3 s r t t st t s r t s ss r s t str t r 3 t t s s r t t st t r t t t s t t t s r str t t r t t rt r t 3 s s t str s 2 r t 2 r s t t t r s s s q t r t t 1t r t 3 s

79 t t 2 t t s r s t str t s r r r t st s str 2 s t t t 2 t s rr s t s r t 3 t ts t s t r st 2 t r t 2 r t t r t s r t ts r t t r t s 2t s s t t r t tr t ss t t r t 2 t t 3 s t r t t s r t 2 r st 2 st t t s t s r t s r t r 3 t t r 2 s r t t t s r s t t P 2 rs s s r ts t 2 t s r ts r s t 2 t t t r t é s r s s r t 2 r s R t t2 σ t r ts t t 3 s t t2 V w rt r s t s t s r t rs s t s 2 t t 4πσRV w c 2, t q t t s r t 2 s r R m 1. t s t t t s t t r t 2 s r t t t r t t 3 s t s st t t r r t str t t tr t t t s s r 3 t t t t st s t 2 st st r t s t s s s t t s r t t 2 t t t s t t s 2s 2 t rt r t t s r t t t r t t str s s r t s r t s st s r t t t r t t t t 2 s r t 1 t r t t r2 s t s r s t r t r t r t t r2 t s s t r r t t r s s s t s s s r t t s t s 2 r t s s t t r r r t t r t st t r2 st t s s r 1 t t s s r tt s V = V(x)ˆx B = B(x)ŷ t t 1 1 s t r t t rt r t2 t x t st t t r t t 2 t s rt r s t r 3 t q t 2 s V(x)B(x) = constant r r s t 2 s r t t t t r s s r s t t st s s t t 2 s t r 3 r 1 t r s P s s

80 t t 2 t t s r s r t t t r t r t 2 t t s r s r t t tr t t 2 r t s t s rt s 2s r s t t s t t r s str 1 1 s r rr t t t 1t s t r t V w t 2 1 s s r t B w. t r s t t s t 2 é r 1tr t r 2 r r t t s s s s t s s t s r 1 t t st rt s t t r t t t t t s s s s s t tr rr t J r r t t r s r s rr t s r 2 t tr t r t 2 2 t t t t 3 s E = Vw c B w. r t t t str t r r t t t s rt t t str ss t t t 2 t r t t 1t r t t t s sts t s s t t r t2 r t 2 t t t rr s s s r t 2 r t2 r rs 2 r P s t t r t t s r rt s s r t s r ts t r s t r ss s s r rt t ts s s rst t t 3 s s s rs t t st t t r s r t s s t s s s s t t t t r s t s r2 s t t 1 t t s t2 r t t 2 r s t r s 1 t s s s t t t s r ss r s t st s t rt t t r t r ss r t r ss s t t s r t s r s r s2st s t t t t t2 r q r t t st t t 3 s r t s t 3 s s r 2 t r s r s r t r t 2 t s t s s rs s r s

81 t t 2 t t s r s r t s t r s s t t s r t 3 ts ss ss 1t 1 s r s t s s s s t r tr st t ts 3 r r t r s r s s s s t s r s r r t t 2 r r t 2 t str t t tr s r ss s t r 2 t r t 1t r s s t t t 3 s s s s r s t s t 1t r s s t 2 ss t rt s t s r r s t s rt r 2 rt t t s t ts s rs s t r 2 s r t s s r ts t s r s2st s t t t t r t r t 2 t t P s s t r ts t t t s r s s t 1 s r t s st s s t t s t rs t s t r r t t t 2 r t s ts r s t s s s t t t t 2 r t s ts r s t r t str t s s s q t r ts t s t2 t 2 t str s t r t tr s rs t t t t s r r s t r t r r s t t r t t s t 2 t t t t 3 1t r t r r s s s s t t t t t 1 t t r 2 t t t s r t s t r t t r r t s r ts r r 2 t t r t t r2 1 r r s r t t r r ss t t t t t t r t s t r t s s 1 t s t r t r s 2s t t s r s t t r r s s r t s s t s t t s r r t t r t t 10 4 tt r t t s t t s s t s s t s 1 r s t t r 2 t rt r t r t t t r r s r s s t t str t r rs s tr s r t t t s r t t s r t st rts s s s t P s r ss r t r2 r t s r s s r 2 s t r2 r 2 t s t r s t t s tr t s r t r t s r s s t s r t r2 rt s r2 P s s

82 t t 2 t t s r s r t s r t s r t t r ss t t t r t t r t r t t t t t t t r s s str t s t r t t r t s s t r t s r 1tr t r 2 r r t r t r rt s t tr t s s s t s rt s s s t t s rt r t t r2 2 s 2r r r r t t t s 3 t t s s t s t P t s r ts r s t s t t r r s t r t s r t r t r s s t t s r s s r r t str t s t t s t t t t r t t t2 r r t s s str 2 s r t str t t r s t s r t r s st s r t r s t r s t r s r ss t P r t ts rs s r s

83 t t 2 t t s r s Magnetic pile-up Magnetic pile-up r t s r ts t s rr rs t 2 rs r 2 r 2 t t r t r ss t P s r ts 2 t t t r r t rs r 2 r s r t ñ t s t t rs s t s t tr s t ñ t s r s t t r s r t t r t t t t 3 s r t t s r s r t t s s r t r s t t r t t s t 3 s tr 3 t r r t s s s rt t s t r t t t s r rs s s t t s r 3 s s s s t 3 t r 1 tr t s t r s r rr t s2st s t r t s rt r t s t str t r t r2 t t ts r r t rt t t s r r t tt r t rt t t s r st t t t r t t t P rs t t s r r 2 s rr t t q t t s t ts s sr t t s r ts s r s t s r tr st t t r r r ss r t t s t t r s s str rr t t t t ts r tr st t r s t t t2 s s sr t t s t r 2 r t t t t r t t 1t r s rr t t t r 2 r t t s r t P s s

84 t t 2 t t s r s t r2 st s s s t P s r ss t t s s 2 r 3 s t t t s t t s t t P t r 3 t s s s s r r s q t ss tr t s t t 2 s 1 s r r t r r t r t t s r s t t r2 st ts s r t r t rt r st t s t r st 2 t t r s t r s s s r r s r ts r r ss t r s r st t s r s t str t t r t t t t s t2 t t P t s s rt t t s t q t t P r t s t s P r s r t r P t t r t r s ts s r st t t r 2 t r ss r2 t P t s 2s t t r t s P s s s t s r2 s r ss t t s 2 s r 3 str 2 r s s t r s s t r t r t t str r t s st s r rs t s t ss r 2 ss t t str 5 5 t t t P s t rs 5 5 r s s t 2 t r r t t t r2 st s ss s s s t t P 2 tt t t P 2 r r s t t t r r r t t r s r ts t t r t r t r r s t r s s s r t t r r P r ss t 2s 2 tt r t t t r t t 2 t t tt r s t t r s s t ts r r t s s t t s t r2 st t t r t r s r t t t s t t t t P t r t t 2 s r t s r t r t r2 s 2 r t r r t s r r2 r t P 2 r t r 3 2 s r r s t t str t r t tt t r st s tt t t r t tr t t tt r rst t r r t rs s r s

85 t t 2 t t s r s t s sr t t s t q t tt s r ts t t t P r ss t 2s s r t s t t r2 t s t r t r s s t r r t P t str 2 r s t r s r ts 2 t 2 r t t r t s r s t 2 tr st t t tt t s t t P s t s r 2 t t t r s t t s s r s t r 5 5 t r P s r s t 3 t 2 s t r r s s 2 t t q s r sr t s st t st 2 t rr t t t B x t r ss B rad ts t t r t t s t q r s t rr t t B x B rad s 2 r s r s s t t str t s r 2 t t t t 2 t t t t tt s t t t s r t s t rst s t t str t r t2 s s r t r t t t r 1 t t s rst s r s s s r s r t r s s r s t r s r s 2 t t t r t s r s s r t r s t r t r tt r s t t r s t r r t r r r s ts r t t t t s r s t 2 r t t s ss t t t P ts t t t s r r t t s t r t rr t ts r t r r t t r s r r r t t t r t r t t t2 r ss t 2 ttr t t t P s t r t s t r s r t s r t r s t t t s t2 r s s r r r st r 10 5 t t 9, t t t t t tt t r r2 s r r s +20 r st 10 5 s r rt r t s t t s t t r s t t t t t t t t s t t s r s 2s t t rr t r s t r t t s s rr t P s s

86 t t 2 t t s r s 80 B CSE, VEGA 1 flyby at Comet Halley, 1986 Mar 06 Bt CSE [nt] R CSE [x 10 5 km] :20 CA 0 05:00 05:20 05:40 06:00 06:20 06:40 07:00 07:20 07:40 08:00 08:20 M1 C1 C2 r t s r s r s t t str t t t t s t r s st r r r t t t s r s t 2 r t r t r rs r r t t t r s r s r 1 t t 1t r st t t t t t t r s s r t 1t t r t t r t r s t r s r rst s r t s r 1 t 2 s tr s t s t r t t t s t t2 s r ss t t t t r r t t t r r t t Bz CSE s s r s s t r t rr t 2s s r r t t str rr t s t t t r t t 2 s s s t s t s r t t tt s s s t s t s t s t s r s str t t t s t st 3, s r t t s t st 1, r t r t2 st rts r s s t t s t r s t r s r r t t r t t rr t t t B x B rad t s t str t t r s t t str t r s s r r t t t r t P r t t t rs s r s

87 t t 2 t t s r s :00:00 to 07:09:59 y = 0.70x r c = 0.91 ns = 578; 1 av /(1 s) :10:00 to 07:15:59 y = 0.96x r c = 0.99 ns = 360; 1 av /(1 s) 40 Brad [nt] 35 Brad [nt] Bx [nt] Bx [nt] etween and, for four intervals around closest approach, the color refers to the respective time interval in Fig. 7. For the inte r rr t t B x B rad r r t r s r s st r r t t r t rr t s t s t t t r s s t r t t t r r tr s t r t r rt st rt rr t r2 s t r 3 t t t 2 tt r r r s st r r t str t s t t t s t t t r t t t2 tr st t t r t r s t r t t t r t P t st t 3, t t t r t s t str rr t ts r t s r s t r ss t P t ts s2 tr r t t r s t t t t t P s r ss s rt r st t t s t r s t t 2 t t r s rt t t t t t t 2 ss t t t s r P s s

88 t t 2 t t s r s t 3 t r2 s t r t t t s s r t ts t t t2 s s r r r t t r r s s t t r t r t P t 2 s t s s 2 s r t rs t t t r r2 r tr s t r t r s t r s r t s r t 2 t r t s r ss s t s s r t tt t r st r t r r tr s t r t P t t P t t r 2 t t s t r2 2s s r r t t t 2 t s s t r rr s t t s r s s r ts t s r t r s ts t r r 2 t t t t str t r t r t t r s s r ts r 2 r ss t t t t r s s t t t r t str t r t s s t t t r t r t t t str t t t r rts t s t tr t t s r ts r t r r2 t s rs t s r t s r s t 2 t t t r r P s q r r r ts t rt r s t t t r t t t s sts 2 t r s t r s t 2 r s r t r t t 1t r r t q st t 1 st tr s t s r s t t t t t t rr t rs t r t t s tr s t s r ts r s t r t r 3 t r rt t r r t r s ts t t s 1t s 2 st 2 P s 1 r ss s r ts s t rs ss t rt r s t t r t r str t r s t t t r t s r R V, t R V = 6052 str r t t r P t t r s r t s s t rs t t t t t str t r s st t s t t s s r t 2 2 r s t s r t t t t r t t r P r r s r tt r t 2 t r rt s2 tr s t s t r s t t t r t t t t r t r2 t tr t t ss t t r s r t s r t r s r t t t P s t P t s t ts r t t t t r t t s s s r r t s r 2 2s t r t r st s r t rt rs s r s

89 t t 2 t t s r s t r r t 2 t s r s 2s s t r t 1t r str t r s t r t s t t r t t 1t r t t r st 2 t t t P t t rs s t st r r t s r t t t t P t r s t t t t t t r t 2 t t s r t t r t 2 t str t t2 ts t t t s s r t s t t r t t t 3 s s t ts s st 2 s r s t s r s r s 1 s s st s r rs P r r t t r t r t r r s r t r r 2 t r t r s t t tr t t r 1t r r t st t r ss rs P r r r t 2 2t 1 s t rst r t t rs r s2 t t s t s r2 s r2 r r t s r t t r t 3 s r t s r st 2 st t t s 2 s t t r s st t2 s t t r s r t s r r 2 r r2 t s t t t ss t t s s O(η 1/2 ) r η s t t s t2 r tr r s st t2 t s r t t rs 2t r t st 2 t 2s r ss s rr t r 3 t t s s r s r 23 t r t r st s t t r t s r t 2 t st s r r str t t t rt r s r t r t s r r t t t2 tt t t st 2 t s r rt s t s r rst r s t t t s r str t r r r t r 3 t t t t 2 t t r s ts r t t r t t t 3 s r s r t 2 r r tr r2 t t str t2 t str t t s rst r t 2t s t r t tr t s ss t t t s r r st 2 st t s r t 2t s r t t t r t s s r s t r 3 t t s s t2 V(r) rr s s t t t r s r r sr r st 2 P s s

90 t t 2 t t s r s st t t s rst t s rt t t t t t t s r s r t 2 t r s t 1t r s s t t 3 t r st s s2 tr2 t t 1 s r s r r tr r2 t r t r 3 t t t s s2 tr2 s st r 3 t t s r st t r ts r t r st s t r r2 t 2 s rs r r t rst r 1 t t t tr t s t t ts r s st t2 s t r t2 t s ss t r st 2 s r t s tr 2 r s st t2 s t t r t t tr s s t r t q t s t t s r t r st 2 st t t s r (V B) = 0 B = 0 E = V c B s t s s t q t s ts t s r r st t r2 t2 s ss t t rr t t V = 0 r ss V = 0 r t s r r s t2 t 2 t tt r s 2 t r t t t s t r r r t s2st t t t r t s r t 1 1 s t r t t t2 t t2 ss s t B 0 t t2 s t r r t t t2 V 0 ts t r s t s t 3 r t 1 s r s s t t r t s2st s t t2 s r r t s s 2 t 1 r ss V = (1 R 3 /r 3 )V 0 cos(θ)ê r +(1+R 3 /2r 3 )V 0 sin(θ)ê θ r r θ V 0 r t r st t r t t s t2 t t2 t t2 r s t 2 t t r t r p t t s t st p str r t 1 1 s r r s p = 1 R 3 /r 3 rsin(θ) rs s r s

91 t t 2 t t s r s Z B 0 Y R X B 0 r t t r t s2st r θ s t t t 1 1 s rt r s t r t t s s t π 3 t φ s t t 2 3 t s s t 2π r φ = 0 rr s s t t r t t 2 1 s q t s s t 1 r ss t tr t r s t tr st t t t Φ E = Φ t r r V Φ = 0 q t s t t t tr t t s t r2 t str s t r2 t s ss t t q t r t t t s r t s r s q t t s r t t t r st s r t t t tr s t s2 t t r r s ts t t 2 1 s s q t r r t s t s t t r2 t Φ(r ) = E 0 rsin(θ)cos(φ) r φ s t 3 t r t t t s r r t s2st s r t s st 2 s t t q t s st t t t st t r2 t q t s Φ = E 0 r 1 R 3 /r 3 sin(θ)cos(φ) = E 0 pcos(φ) s ts 2 s q t t t tr s r r t s r P s s

92 t t 2 t t s r s E r = E 0 [1+R 3 /2r 3 ] 1 R 3 /r 3 cos(φ)sin(θ) E θ = E 0 1 R 3 /r 3 cos(φ)cos(θ) E φ = E 0 1 R 3 /r 3 sin(φ) q t t t r t t t2 t tr s t t r t t ts r r t V t t r r r t t t t t t t t t t q t s s t s 2 t r t t t t r t t t 2 r 2 ss r t r t t s t r t t s r t tr t s t r t t t r t B 0 t t2 t t2 V 0 s 90 t r t t B 0 V 0 t t2 s 0 s t r t2 t 3 r t r s t t B 1 t t2 V t r s t r 2 ss t t s s s 2 r t t t s t s t s s t t t t2 s B 0 = B 0 +B 0 rst s r t s r r t t t r s t s t ẑ r t s2st 1 s B 0 s r r t s t s r tt s (B 0 ) r = B 0 sin(θ)sin(φ) (B 0 ) θ = B 0 cos(θ)sin(φ) (B 0 ) φ = B 0 cos(φ) s r ts t r t q t s r rs s r s

93 t t 2 t t s r s [ (V B)] r = θ [sin(θ)(v rb θ V θ B r )]+ φ (V rb φ ) = 0 [ (V B)] θ = r [r(v rb θ V θ B r )] 1 sin(θ) φ (V θb φ ) = 0 [ (V B)] φ = r (rv rb φ )+ θ (V θb φ ) = 0 B = 1 r 2 r (r2 B r )+ 1 rsin(θ) θ [sin(θ)b θ]+ 1 B φ rsin(θ) φ = 0 r t t2 V q t r q t r t r t q t r B φ B φ r + V θ rv r B φ θ = 3B φr 3 2r(r 3 R 3 ) t t r t t r B r B θ t 2 q t 2 r q t t 2 sin(θ) t t K r + V θ rv r K θ = 0 r K = rsin(θ)(v r B θ V θ B r ) r s t r s rst r r rt r t q t s s 2 t t r t r st s t s s r r s r t r t r t r st q t s 1 r ss t r s θ φ t r s r r r str d dr = r + V θ rv r θ s V φ = 0 s q t s str t t r t r p t t2 q t r r t db φ dr = 3B φr 3 2r(r 3 R 3 ) q t s dk dr = 0 P s s

94 t t 2 t t s r s t r t q t s t r2 t r t t t t2 q t r r B φ = B 0 cos(φ) 1 R 3 /r 3 r q t t t t K = pv 0 B 0 sin(φ) t t t q t s r t t 2 r t t q t s t r s ts r r t tr t s t t 2 t r B φ K t E r = V θ c B φ = (1+R 3 /2r 3 ) V 0 c sin(θ) B 0 cos(φ) 1 R 3 /r = E [1+R 3 /2r 3 ] R 3 /r cos(φ)sin(θ) 3 E θ = V r c B φ = (1 R 3 /r 3 ) V 0 c cos(θ) B 0 cos(φ) 1 R 3 /r 3 = E 0 1 R 3 /r 3 cos(φ)cos(θ) E φ = (V rb θ V θ B r ) c r E 0 = B 0 V 0 /c K = crsin(θ) = pv 0B 0 sin(φ) = E 0 1 R crsin(θ) 3 /r 3 sin(φ) q t s t t ts B r B θ 2 s q t s 2 t t r t r st s str s t t r t q t s r B r B θ s s rs P r r r s r r t [ db r 2 dr + r 2r3 +R 3 ( )] 1 2r(r 3 R 3 1+ ) cos 2 B r = B 0 sin(φ)sin(θ) (θ) r 1 R3 cos r 2 (θ) 3 [ db θ 2 dr + r 2r3 +R 3 2r(r 3 R 3 ) + 9r 2 R 3 ] (2r 3 +R 3 )(r 3 R 3 B θ = 2B 0 sin(φ)(r 3 +2R 3 ) ) r 1 R3 cos(θ)(2r r 3 +R 3 ) 3 rs s r s

95 t t 2 t t s r s r s t r s rst r r r r2 r t q t s r s 2 t r t t r s t r t s q t s 2 t t ts B r B θ r B r = (r3 R 3 ) r 3 r cos(θ){c 1 B 0 sin(φ) pr 4 dr (r 3 R 3 p 2 r) 3/2 r 3 R3} B θ = (2r3 +R 3 ) r r 5/2 r 3 R {C r 3 (r 3 +2R 3 ) r 3 2 ±2B 0 sin(φ) 3 R 3 dr (r 3 R 3 p 2 r) 1/2 (2r 3 +R 3 ) 2} r t r s s r r t t r 0 θ π/2 t r s t π/2 θ π C 1 C 2 r t r t st ts t r t s t s 2 t r2 t s str r t t t t t r t ss t t t r r s q r r t t t2 s r t s B 0 = B 0 t r r B 0 = 0 t t t B = V = 0 (V B) = 0 t r2 t s s t t2 B 0 = B 0 V = V 0 r s t t r t t s t t 1 1 s r s t 2 s t s s s r r str t t r t t t2 t 1 r t t V B s r r t r 3 2 t s t 2 t 2 t s r r t r s t t ts t s s r B r = (1 R 3 /r 3 )B 0 cos(θ) B θ = (1+R 3 /2r 3 )B 0 sin(θ) B φ = 0 s r s 2 t t t r s t r 2 ss r t t t t t t2 s s 2 r t t t t s t s r s q t θ 0 s t t t r t t 1 1 s s r t B 0 = B 0 cos(θ 0 ) B 0 = B 0 sin(θ 0 ) r s s t t s r t s r st t 1 3 r t s r B 0 V 0 B 0 r t t 3 1 s s r t r rt s r s r s t t t s t2 t t s r t s r s t str r r t r st s r r t s rr s t Z = 0 P s s

96 t t 2 t t s r s Z(R) PRL V 0 X(R) r Pr t t s r t s r r B 0 V 0 s t t str t r s sts t rr r s2 tr t s r s s r t 2 t r t2 r rs 2 r t t Z = 0 t t r r s t r t2 t t t t s s t r s t t str t s t t s r t s r r t r s ss t t r r t r s s t t s r t s r st t 2 3 r t s θ 0 = 60. r r r s s t t t r t t t s2 tr2 s r r s t rs r t2 r rs 2 r P P s r r rr s s t t s t ts r B x = 0 r t t P r r t s s s t r r t 2 rs r t t t t r rs s ts r t2 t s 2 rs t P s t t Z = 0 st s t s s r t str t 2 r r B 0 s str st t t s t t s t P r s t θ 0 t 1t s t r r r t 2s s t r rt s t s 2 rs rs s r s

97 t t 2 t t s r s IPRL Z(R) PRL V 0 B 0 θ 0 = 60 X(R) r Pr t t s r t s r r θ 0 = 60 s t r s st t2 ts t P t P r s r s ts r t r t ss t t t r s st t2 ts r t r s st t2 ts r r 2 rt t t s rr s t P t 2 r t 1 t t t t t s t P s t 2 s r s t t t t t t t s t2 t t s t t t s s t P t r 1 t2 t P t r s t r s r t r s t 2 P r t2 r rs 2 r ss s t t t r t r t t rt t s s t t s r s st t2 ts t r r t t t t 2 s t t t tr st t t t r s t t t s s s t t p/r > O(Rm 1/4 ) r R m s t t 2 s r r r t 2 t r2 2 r t t 2 t t t r s t r s st t2 ts r r t s s t r s s t t s s t s r t P s t s 2s t t Z = 0 r r t r st P s s

98 t t 2 t t s r s t 2t t t t t t s r t t s s t2 ts s r rr t ss rs r t2 r rs 2 r t r s st t2 ts r t ss t t r r t P t r ts s t s r r t s θ 0 s t t r t r r s t t r s s t r s s t t tr2 t P t r θ 0 = r s s t 1 r t 1 s t t 1R < X IPRL < 2R t P s r r t st r s t s rt r str 1 < 3R t P s t t t 2 t str rt t P t s 2 r s r 2 s t t r r st s r t Z = 0 r r r s t θ 0 r s s t 3 r t rr s t t t t P t str r rt r r X IPRL = 3R r θ 0 [ ] s t s t t 2 t r r s t r r r θ 0 s s r r θ 0 s ZIP RL(R) X IPRL (R) r t t rs r t2 r rs 2 r P t 1 3 r r t s t t r t t r t s s t t t r θ 0 = t r r 2 t t ss s r t r st s s r2 r r s ts s t t t 1t r t s str t 2 r r t t r t t t t t r str r t st s sts t rr r s2 tr t s r s s r t 2 rs s r s

99 t t 2 t t s r s ZIP RL(R) ( ) θ 0 ( ) r st t P 2 r r t Z = 0 t 3R s t θ 0 t t P s r t t r t t r ss t B 0 s s rs P r r r t s rt r s r t B 0 s 3 r t rr r s2 tr2 r s r s t t P s t s t r t t t r t rt r r s t t t P s t B 0 r t B 0 r s t t r t B 0 r s t B 0. t s r r t t t t s t ss t t t P s t s r s st t2 t t t t t s t r t t s t r s t t s t t r 2 r r t r 2 r s s s s t t t s t tt r tr s t r t t s t t t s r r s t s r s st t2 ts t r t rr r s2 tr2 s r r str t 2 r r s t s t t P r t r t r t t s r 1 t2 st t t s r t t t t t P t r r s ts s t s r s ts r t s r t r t t t r r t r t t s s t t r ss s r s t t r r r s t 2 s s r P r t s2st r t 1 s s t r t t 1t r t 1 s s r t B IMF s t t X DRAP < 0 t s s r P s s

100 t t 2 t t s r s B IMF XDRAP = BIMF = 0 t B XDRAP s r r str t t t Z DRAP > 0 s t r rs 2 s t B XDRAP s t t s r Z DRAP < 0 BXDRAP IMF = BIMF > 0 r2 t t Z DRAP < 0 s 2 s t B XDRAP r r s t Z DRAP > 0 s 2 t s t t B XDRAP s BXDRAP IMF = BIMF < 0 r2 t t Z DRAP > 0 s 2 t B XDRAP r r s t Z DRAP < 0 s 2 t s t t B XDRAP s st t t r t s rr t t t s t str t t t s t r t t s s r t t s r rs 23 t t r t ss s r r ts P t s r s t s r t r r t r ts r t s t t r s t t t r s 2s s r r s t t 1t s t t t t rt t s t r t s r t s r t 2s s s t r t r s r s r ts r t t rr t rs r r t r t s2st t s r q s r t s2st s t r rs t t X MSO 1 s t s t t t s r r t t t r r r ss rr t 4 Z MSO r r t rs s r t s t t t t rt Y MSO t t r t s2st r r2 r t t s st 2 1tr t t s t t t s t P str r t rt s t t r s s t P ts 2 s t t t t r t t t t ts r st t s s t r s r s r ts rr s t P r t X MSO r t s r t 1,5R M st t r t s r t r s s t r 2 r t s t rs s t t t t r st t s t rs r t t s t 0,41R M rs s r s

101 t t 2 t t s r s Z DRAP (b) southern lobe B IMF PRL X Titan B X= 0 X DRAP B X IMF =0 SW Z Z DRAP B0 (a) current sheet B IMF IPRL PRL PRL B X = 0 SW X Titan X DRAP B0 B0 B IMF X >0 B X = 0 X Z Z Z DRAP (c) northern lobe B IMF SW PRL PRL IPRL Titan X DRAP B IMF X <0 r t s r r r t r t t s s r t P r t s2st s t s r s t r t t 1 s t t t s s t P s t t t t s r B XDRAP = 0 r r s rr s t BXDRAP IMF = 0 BIMF XDRAP > 0 BIMF XDRAP < 0 r s t 2 P s t t Z = 0 t rt r t s t r s r r s t 2 t P s s

102 t t 2 t t s r s t r t str t t r r t rst t s r ts ts t t s t t t s t r r r ts t t st t s r ts t 2 st t t r s r t s 2 t t s s r r s r s t t t s t r r r r t r2 t s s t2 2 tr s st t r r 1R M r r t t X MSO 1 s r t r r s s t r t t r 1 t 2 t s s t r s r r ts t s r s t t r t t s t r s t t t r t t s r t s t str r t rt s t s s r t rt t t rt r r t 2s s t s ss t t s r t t t s t r2 s t 2 r ss s t t t str t r t s r r r ts t t t st t s r tt r s t t t st t st t r t2 t t t s t 2 st t s t s t r ts t t r 2 r t st t s r t r st t r s r r r 2s s t t t s t t t t s s t s r s t t t r ts s t s 2 t s r t r r t st t s r 2 t s s s t t t r r t s r ts s t s t 2 t t t s r s t t r ss t t s r t s s t P r s s t tr t r2 t s t r ts t rr t 2 r r t s2st t r s rs t str r r r2 t t s t s r t t rs t rt t r t r s t t t s t X MSO r t s r t 4,5R M 3,7R M. t r t s s r ss t rs t t s t r s t P r t r s t s t s r2 r s t s r ts t rt t s r t t t r s st r s r r ss s t r s r t r s t t str r r t st t s t t 3 t P r t s2st 23 s r t s t t t r s r r t st t s t s r r r r t t t r t s2st s r t s2st r 2 r rr t s t P r t s2st r t rt t s t t t t r t s s t t2 s s r ts r rt s ss t t t s r s t rr t rs r t P r t s2st s rs s r s

103 t t ② t t s r s [Y2MSO+Z2MSO]1/2(RM) XMSO(RM) r tr t r② r t s t r ts s t rr t ② r r t s②st s r t s②st t r t rs s ts XM SO ① s t s t t t s r r t t t r r r ss 4 rr t ZM SO s r r t rs s r t s t t t t rt YM SO t s t r t s②st t t r r s s XDRAP = XMSO [0, BYMSO, BZMSO ] ZDRAP = q B2YMSO + B2ZMSO P s s

104 t t 2 t t s r s Y DRAP = Z DRAP X DRAP r B YMSO,B ZMSO r t Y Z ts t r t t t str r rs t s r ts t t st t s t t r t t t rs 2 r t t t P r t s2st s r t t t r t s t (X Z) DRAP t P r t s2st B IMF ZDRAP B IMF XDRAP 3 r s 2s s t s q t t t X t t BIMF YDRAP s t t t r t t t P r t r r r r q r s t t r t t t s t t t t s t2 t r t r 3 t rt t t str t r s s r ts t r r t r ts t r s t r t t t r s t t t t X DRAP r t r t r t t t 2 t s r t t X DRAP 1 s s θ t s r t t t s t2 s r t t t t t s s rs ñ t t B 1 t θ t t s rt t s θ = ± s[ 1+B ] t s 1 r ss 2 t t s r ts r r 3 t s s t rt t2 t t t r t r2 t s t θ IMF ± θ IMF t 2 t 1 t t r t t t = BZDRAP IMF s α = t (BIMF ) 1 t r r t t X DRAP 1 s B IMF 1 r ss B IMF r s 2s t s t t r r t t P r t s2st rt r t r r s ts t r t t t t (X Z) DRAP t r s s t r t t t (Y Z) DRAP 2 t B IMF s 2s r t t +Z DRAP r t t r rt t2 t t r t t s r t α r t 2 t s r t s s r r t s t Z DRAP t t r s t s s r s s r r 2 s 2 t str t s Z DRAP = Y DRAP /B IMF Z DRAP = Y DRAP /B IMF. s ss s t t t t 2s s r r t t t t s r s t t 1t s t s t r ts r t t s s r ts t st t s t t θ IMF ± θ IMF s t t t s t B IMF XDRAP t r s r t s s r r ts t r t t B IMF XDRAP s s s t r r s t r r t r t t t s r st t s t rs s r s

105 t t 2 t t s r s AL.: DEPENDENCE OF THE MARTIAN MAGNETIC LOBES LOCATION ON TH IMF r s t t P s2st r r t t t (X Z) DRAP t t t X DRAP 1 s s t 2 θ IMF. r r t t t (Y Z) DRAP 2 t t P r t s2st B IMF s t t +Z DRAP r t α = t (B IMF ) 1 t B IMF s t rt t2 t t r t t s r t t P s s

106 t t 2 t t s r s 1 r ts r t 2s s t t s r s t t t r r t s t s t rt s t s 2 r s t s t t s t t st t t s r r t s r t t t s t r ts r r st t st 2 s t s t t t st 2 t t t t rt t s t r t t t t t t t r t s s rt r t s s t r r s r t s t t ts ts t t t 2 s t r t t st t st r s ts r s t t 1t s t s ts t t str t r B IMF XDRAP r t r t r r s t t r s s t t r t r 3 t t s t r ts r t t θ IMF t r t t t P r t s2st t r s t rr t t t 1 r t rt t2 θ IMF rst ss 2 t s r ts t t r s t θ IMF ± θ IMF r t s t s s t 0 < θ IMF ± θ IMF < 90 t t r t s t s s t 90 < θ IMF ± θ IMF < 180 rst r s s r ts t BXDRAP IMF > 0 r s r t s r ts s r t s r ts t BXDRAP IMF < 0 t t r s t r t s r ts s r 2 st t t r s s t t r rt t2 α t t t r t t t rt t s s 23 t t s t P t s r t t s t r t 2 t str t s Z DRAP = Y DRAP /B IMF Z DRAP = Y DRAP /B IMF t r 2 r s t r r t t 2 s t t r2 r s 2s t tr t r2 s t P r t t t (Y Z) DRAP t (X Z) DRAP r t r r r s s r t t s r ts r s t t B IMF XDRAP t s r s t 2 t r r s ts s s r t s r r t t s θ r s ts ss t r rt t2 θ < 20 s r t t t r r t s t 2 s 1 r t rr rs rs s r s

107 Z DRAP (R M ) B X IMF >0 t t 2 t t s r s OP IP IN Z DRAP (R M ) BINS T A % 48.56% % 80.76% % 5.59% ON % 100.0% 0.00% Y (R ) DRAP M X (R ) DRAP M B X IMF < OP % % Z DRAP (R M ) IP IN Z DRAP (R M ) % 90.20% 93.50% 93.65% 6.50% ON % 9.59% Y DRAP (R M ) X DRAP (R M ) F igure 4. MGS locations inside the MPB projected onto the DRAP coordinate system. θ ( ) r tr t r2 s t P r t t t P r t s2st r r rr s s t r ts t BXDRAP IMF > 0 BIMF XDRAP < 0 t r t s 2s t r t t tr t r2 t (Y Z) DRAP (X Z) DRAP s s r t ts t t r t r s s t P r t r t t r t 2 r t P P r s r t rs s t t r t rr s t s r t t s st t r r r t t s rr s t s r ts r 0 < θ± θ < < θ± θ < 180, r s t 2 t P s s

108 t t 2 t t s r s st t t r t r s r t s t t s t str t t rt t s t r t t tr t r2 r t s t 2 r r s r t Z DRAP rst t r s r t s t s r t r s t P r t r s t 0 < Z DRAP < 1 1 < Z DRAP < 0 r s t 2 r t r s r t ts t t st t t P s r t t r s t P t r t r s t Z DRAP > 1 Z DRAP < 1 r s t 2 t r s r r 2 t r t s ts rst t t st t s r ts t r s r Z DRAP < 0 r r t t r t t s 2 s r ts r t 2 r rs t t r s r Z DRAP > 0 s s s t t s r ts r q t t r t t t s s r s t r 2 t s 3 r t r r r r s r t t r t t t t t P P r s r Bx IMF > 0 Bx IMF < 0 r s t r st t r s rt r s r t rr s t r 2 r t 2 r θ ± θ = [ ] t r t t r r θ ± θ = [0 25 ] t t r t t t t r 100% t t s r ts t t t r r s t B IMF XDRAP t s t r 10% t s r ts t t 2 r t B IMF XDRAP t s t P r 100% t s r ts t t r t B IMF XDRAP t s t P r 50% t t s r ts t t t r r s t B IMF XDRAP t s s st t st r s ts r s 2 t r t r t rs t t r t r t r st 2 t s r s ts s st t 2 s t 1 st s t t rt t s t r s r r s Z DRAP t r s t t t s t s t r r t B IMF XDRAP t s r s t 2 s t r t 2s s t rr t t P r s r s t s r s t t tr s r t s s r s t s s r t t r r s t P r t t r 2 s r ts r s r r s t BXDRAP IMF t s 19%, 81% t s s t 1 s ss t t t P r t st r 2 s s t r t rs s r s

109 t t 2 t t s r s s r ts t t t rt r s r r s s 1 s r ts t r Bx IMF < 0 93,5%, 6,5% t r s s r r 1 r t t r r t s r r t t r t ss t t t r t t t r t Bx IMF < 0 s rts r s r s ts r 2 t s r 100% t ts t t t t P r s Bx IMF < 0 t r s Bx IMF > 0 r s t 2 r s r r t s r t s s 90,2% r t rst s 94,41% r t tt r s s r 100% t s s t 1 t s s rt r 2 r t Z DRAP = 0 Z DRAP > 1 t s B IMF x < 0 Z DRAP < 1 t s B IMF x > 0 s ss s s r s ts r t s t r r t t t t t rt r t s t t r s t r t t r t t t s r t 3 ts r t ts t r r 1 t 2 t s t r t t t s t s s ss t t t tt r ts r r r t t t s t r 2s s s r t s r t P 2 s s st t t t P s t 1t r r2 r t r s s r t t s t t s r t 2 s t s s rs r s s r r r t t t t r 2 s r t t r r s s t rt P s t t r s t r t s t t t 1 t t s t r r s r s r 2 s r s st t t t s t t s t t r s t t rr r 2 s t s s s ss 1t rst s r s t r rt s t s r s s str t s r t r t s r t t t s t rs t s t t t t rs r t r s t P r t s2st r t t t r s t t t rr t r t s2st s t r t t s s t s s t t t r t 1 t tr t t st rt 2 t r s t t t t t 2 t t rs s ss s s r t t t r r t s t 23 t r 2 2 s r t t s t ss t s r t s s t P t s r r t r r r st 2 t t 23 r ts t t P s s

110 t t 2 t t s r s r t s t t t s r s t s t Bx IMF t r ts t r t t r r t s t t 2 r t s r s t ss s r t s r rr s t t P t r r t t t t t s r s s t t s t r r t s t s r r r s t s s t s st t t t t s t q s q r r t ss t t r t t r 1 t 2 t s t r st 2 t rr s 2 r s t t t r s t t t t r s 2 r t r t r t r rt r t r t 2 ss t t t s s r rt r s r t s 2 t s s r s t r t t s r t 1 t tr r t s t2 t r t t t s t t t rt t s s t t t t r s r r t s s t P r Bx IMF > 0 t t Bx IMF < 0 s t s r t t ss r t r s s t 2 r r t s s t t r Bx IMF < 0 t t Bx IMF > 0 s r r t s rr t s s r r r r s r r s st t st st 2 t t r s t t r s s t r t r r s θ± θ = [0 45 ] θ± θ = [ ] t 2 s t r t r s s t t t s s r t s t r s t t t 2 t ts t Bx IMF > 0 t P Bx IMF < 0 r s t t s t t t r s r t t r r s ts t r s t r t s r s t r r t t s r t t r s 2 s st s r rt t t r t t t t t t P t P t t t t t s s t 2 t s t r st t t t t t s t t t s t r t t t s s s q s t t t r r t r2 rt r t s 1 t r r t s t s t t t t s t r st t s r t t r2 s s r t t st s t t r2 rs s r s

111 s st t t 2 t t s r s r s t ít stá st t í ét q r s t t r ó tr s t 3 2 stá t s ér t 3 st s rt r t t r s s t r r í 2 t t tr 1t r 2 t t r t t í ét q r t t s ér t 3 s r t r s t r s r t s 1t r s r t s s s 3 s s r s s q s s t s st s st s s 2 ó rtí s 3 s r t s ér s r s r s s r s r r3 s r s rr t s r s t s s r t r t stá st s rr t s sí t é 2 ó s r t s t 3 r t stá s r s ré s s á ét s s r t r ó st t s t s í s ét s st r s r ó t 1t r tr s s t r t st ít st s t í ét s r r s t s t s ér s t r s t 3 s s t s st t ór s 2 s r s s t st t ór s rr s ít q r t t r r tr ét s s t 3 r t t t r t r t s r t r s st r s s t st s r r t r 3 s r í ét s r tr s tós r s s t 2 2 rt sá s s r s t s r s s s s s 2 r s t t s tr s r 3 s r t st t s s r r s s t s s rt s r t r2 r t t 2 P t ó 3 rt t 2 st t t 2 r 2 r t 3 t s r str 2s r rt ó 3 3 t rt t s t t t r t r2 t r t s r t s r rs r 2 r 2s s P 2s s r ss P s s

112 P Pr t 2 tr s str r rs s s t r s s t st 2 r q 2 tr t s s s r t 1t 1 s r s rs s r t r 3 t r r r t s r q 2 r 3 t r t s ss t r t t t t t t r2 1 s r s s t2 t r t r t r t r s t r t r ss s t t r r t t s t 1t t r r s s s t s 3 t t t s r r t rs r t r 3 t s s r t r t s t r t t t t2 t t2 str t t s s t t r s r t t r t r rt s s r2 rt r 1 s r ss s t s t str r t ts str r t r r s t s s 1 s r tr rt s r t 2 3 s s q t 2 2 t s r s s r s s t st r s P s s t rt t s t t t r t t rs r s s t t s t t s t 2 r t 1 s s rs s r t t t r t t r2 s r r s t 2 t

113 Pr t 2 tr s str r rs s t r t r s tr s r r 2 t t t t t r2 rt s t t s 1 s r t t s s s t rt s r t r q t t r r t 2 t 2 s t r t 2 s t s2st t s t tr t t t s t t s s t rt s s s t rt t s t r s t t t t t r t s st t s t t s r s s t r s r s rs r t 3 s ss t tr t s s r t 1 t s r t str r s rs s s t ts tr t s r t r ss s r ts t t tr s t s s s s r rs t 1 s t tr 1 s r s t t 1t 2 t r r s t s s s r t s r t t r t r ss s t t t t t 3 t t t r t t t s r t st rts r 2 t r rt s r t 1t 1 s r 2 2 r t t r t r s t t t r2 t s r s r 3 s r t r2 r 2 r t t r 2 t r t r2 tr s r 3 2 t 3 t r 1 tr t t t s rs t s rt s r 3 st 2 t r t rst t r ss s t s 3 t s s s t r 2 t t s t r s t t t r r t tr s s t tt r r r 1 t 2 t r st t r s t t t t t s r t t s t2 s s 1 r rs t t tr t s t s r s s r s t t r t tr s 3 t r r rt s t t t r t t2 s t V SW t s s r s tr t r2 r t t r t r2 t t r r t2 V SW sin(α V,B ) r r t V SW cos(α V,B ) r t t t t2 t α V,B t t t t r s t t t t r s t s s t s s r s t s s r t s t t2 str t t t r t r2 s r t ss t r t r s r r str t s s2 t t s s r s s r t t rt s s s r t t t r2 r r t t r t r s t 2 t P s s

114 Pr t 2 tr s str r rs s r r str t s r cos(α V,B ) = 0 r str t s rr s t sin(α V,B ) = 0. + r P r r r t2 r 2s s t r2 t 2 s r r t s s 1 t 2 t s s t r s 2 st t ts s r st 3 r s r t t s r t r2 r r s t r r t r s t r2 s s r s rt s t t r r t2 r s 2 t 2 st str t s r t r2 s 1 r t r t r t rs ss t t r tr t s st t2 t t r s ts r t t r t t r t 3 s str t s s st 2 s t r t s t s 2t s t t s s t r s t s t2 r t s 2 st r t t r r t r2 str t t s s tr t st t s r2 t r r 2 r t r t str t t t s t t t s r r s r t t s r t t s s t t t α V,B s t r s t t r s t r t 2 2 r t t r s t r q 2 t r t r t 2 st t t st t2 r 3 t t α V,B t t t s r 3 s s V SW s r t t t r s r t s r r t tr t rs s r s

115 Pr t 2 tr s str r rs s r t r s t st t2 r t r2 t t r V SW s r r t t t r r str t t r t tr t t st t r t s α V,B t st t2 s st r t r s r t t t t 1 r t r t t st t2 s r r t t t t st t2 r α V,B > 75 r s r t r2 r2 s s r2 t s t s α V,B = 90 s 3 t t s ts r t s st t s t t st t s r rt t s t t r 2 tr r s t st t s s 1 t r 2 tr r s t st t2 rs t t s r s t t t r rt s s s t s s t r s s 1 r tr t r q 2 ω t r k t r s t r q 2 s t t r 2 tr r q 2 Ω ci r t t s r q 2 r 2 tr r s t r tt ω k v ion ±nω ci = 0 r v ion s t r t2 t r t B Ω ci s t 2r r q 2 t s s + t r 3 t t s + r r s t 2 tr r r r 2 tr r s s r ss t t n = 1 n > 1 r s t 2 r r t r s rs t s s s t s t r r r r s t r 3 t t s t tr r t t t s s s s t r 2r t t t r t s st s s str rt t r t t t r 2 1 t t t r s t st t s 1 r t r t s t k B = 0 r k s t r t r r s r t t s s 2 t t 2 tr r s s ss 2 n = 1 s t s r q t r t t t t st t2 r r t r t B s t s s t 1 r ss ω k v ion +Ω ci 0 r r t α V,B r s ω k s t t s t 1 r r t r t s r2 t r t t t t t r ω ion = ω k v ion s t r q 2 t tr t s r q 2 ω t r k t r s r t r r r r t s s r ts s r s r rt s r rs r s t tr t s r t t t P s s

116 Pr t 2 tr s str r rs s t t 1 r ss s s ω sc = ω k v sc ; where vsc = [V sw ˆk]ˆk r ω sc s t r q 2 t s t r ˆk = k/ k s t s t rs s t t t2 t r t t r2 r s s t r s t t V sw t s s s ω sc Ω ci r r s r t 2 t st t2 tr r t r 2 t 1 s r s t r t t t s r r t r 3 2 r q 2 t r st s t t r 2 tr r q 2 t t r 3 t t s s s r t r r t st t2 r s t r rr t s r2 s t r r t s s r t t r 3 t t t s r s t t r 2 tr r q 2 s t s sts t t t rr s t t 2 tr r q 2 rt r s s t r ss t t t rr t s s t s s s t r s s s s r r t 1 st 3 1 s r rt s rt t st t t r 2s r rt s 2 tr s r rt t rs ss t r t 3 t rt t t s t t r t t ts s r t t st t ss r t s r t 3 r t s rs t rst s r t s t t r t 2 tr r q 2 str t s 2 t P s s r t ss t s s s t s t 2 r t t 2 r 3 t r r t t s t t t P s s s r 2 r t 3 t r t r r st t st 2s s t r rt s t s s r t r s s t t s t r q 2 r 3 t r t t s t t r s r t t s t r r P s s r t s r t s r r t t s r t r t tt r t t s 2 rs t r ss 23 ts r t s s ss t r t s s t r st s s s t ss str t s t r t t t tr s t r2 2s s t t s 2 ss r 2 t t P s s r str r t s rs s r s

117 Pr t 2 tr s str r rs s s t s st 2 t t s r ts rr s t r ts r t 2 t str t t s t r rr2 t st 2 t P s t t 2 t r str r t rt s r t r s s 23 t r q 2 r t r 3 t r rt s t s s t ss t rr r t s ss t r t s s t r r t s t t tr s t s t t 1 s r rs s 23 t s t str t t s s t tr r t s2st t r rs t 2 s st 2 t r rt s tr t s s s r 2 P t str r s s ss t t s r r s ts r t t r t st s s str r rs t s st s r ts t t r s t s 3 t s r t s s r s r t str t t s q t r r r t s s r t r 1 s r r t s t r s r t s 1 t r s t s s t s r 2 t tr str t t s t 2 s r t t tr s 2s s r r t s sts r t r 3 t t r s tr r rt s t r r 3 t t r r r t r t t t rs s t r s t str t tr t r t s2st r t s r t s t s 2s s s t t q s r t r 2 s tr rr t r t 2 r r s tr t t ts t r t s2st r t r s t t t r rt s t s r P s s t t r ss rr t t t t t s r s t t tr 1 s r ts r s r 2 s t t t t ts P r 3 t r t r tr 1 t t r r 3 t P s r t 2 2 t 1 t r t s r t r r r r P s s

118 Pr t 2 tr s str r rs s t t t t 2s s s t t t r tr 1 t t r 3 t r r t r t 2 tr r q 2 r tr t s r t s r t P rr t ts t s tr 1 r r t t t r s r t t r 3 t t t2 t t s t r q 2 r s r t rs r 1 t 2 t q t s rt3 r s t 2 t 2 s t t s 2s s t t t2 t t rt s t r t s t t s r t s t r s t t t rt r s s t s st 2 s s r t r t s s s r t r r 1 s r s 3 t r t s r s s st t t s s t r t rs t t t t s 2 t s r t ss r t str t s s r t r t st s t s st t s t str t s t t tr E st t s r tt r s t str t s 2 ss V SW = 400 s 1 ˆx MSO st 2 t s t str t s t r t t r s t t t r t t t tr E = V SW c B 2 tr tr t r t s2st s t r t rs t t Z MBE 1 s s r t E X MBE s t r t V SW Y MBE t s t r t tr s s t s 2s s t s t s s t t t r s t str t t r rt s t s s t t r t r s t st 2 s t r rt s t s s t tr t r2 r t t s s ts s s s 2 t t s t r r t 2 tr r s 1 s s r t s r s s t2 1 s t t2 r s t s r ts r str t s 1 P s s 2 str r t rt s t t r s s t t ts t r r r t rst t s t s s r q 2 rs s r s

119 Pr t 2 tr s str r rs s r t s t r r t s t r t r t B o s q t st 2 ts t s s t 2 ts r t t s 34 t r s t t t rs r t r s s t r t tr 1 s r ts 2 r r s t t r s t s s t s s r t t s s r 2 s t 2 r s r r 2 s ss t t t 2 r s r s t t t t tr s t2 Bx (nt) By (nt) Bz (nt) Orbit P216 B (nt) :37:00 10:37:30 10:38:00 10:38:30 Universal Time (hours) r t s r ts r rt t r t P r t s r t 2 s tr rr t s t s s r ts r r t t t t t t r t B o t r t tr 1 s r r t r s r s r s s t t t s t r t t r t tr 1 t r r rt t r t P r ss rr t t t t s r s s t s s 2s t 3 r s t t rr t t t ±2 s r t t s 2s s r t r ts r r t r 2 s t s r r s ts s s st t t t t s r s s s r P s s

120 Pr t 2 tr s str r rs s 3.10^4 Orbit P233 Flux (part/(cm 2.s.ster.eV) 10^4 314 ev 191 ev 116 ev 10^3 17:33:00 17:34:30 17:36:00 17:37:30 17:39:00 Universal Time (hours) r tr 1 s r ts r rt t r t P r t rr r ±2 s ss t t t t str t s t t st t s s r 2 r q s t r t t r t 2 tr r q 2 Ω cp t ±1 rt t2 r s s 2 r r s tr t Y MSO t t t r rt t r t P t r q 2 t s t s s s2st t 2 s t t t r t 2 tr r q 2 r s r rs P r 3 t s s t t t s r r r t st r t t r t t r r r 3 t t r t r s t t B o r s s 1 t r s ts 2 tr r s t t s s 2 s λ 2 /λ 3 r t t t t t s r r s t 2s s 2 s s t k B o θ kb = 8 s t t t r r t s q s r t r s t t t r r s r t 1 t r t r ts r 2 s s t r 3 t s t t r t s t r ts t t t rs s r s

121 Pr t 2 tr s str r rs s 0.5 Orbit P232. δb par and δflux (E = 116 ev) δb par (nt) δflux (part/cm 2.s.ster.eV) Time displacement (seg) 6:40 6:41 6:42 6:43 6:44 6:45 6:46 6:47 Universal Time (hours) Cross correlation function r t t s t r t t t t tr 1 s r ts r rt t r t P r t s s r t r t r rt s t s r r s r rs s r s t st t θ kb r r t 2 tr r s r λ 2 /λ 3 > tt r t 2 s θ kb 9 s st t 2 t s r s ts t t t s s t2 2 r r t r t r r t t r t t t t t t t t r k s s t r t t t r t P r 3 t r r tr 1 r t r t s s r s r t st t t r t r 3 t r r t r t 2 tr r q 2 r s s 1 s r t s s t r s r r 3 t 70% r t r r t t2 t t s t t r 3 t < r 2s s t t r r ts 2 s r r rt s r r r s t t2 2 r s s t t t t s r s t r st r t t P s s

122 Pr t 2 tr s str r rs s r r r 2 s tr B YMSO r t P r t r t 2 tr r q 2 r t s tt r r r t s t t s s rr s t t rr r rs ss t t t s r t s t P s t r s tr s t2 t r s rt t t t rs s t s r t s s r str t s t s s r r t P s r r s s r r t r r ts t t t rt s r rt s P s r t s s ts t rt r s r s ts r s r 3 s s t r r rt s P s r s t r ts t t r s s t r rt r 2 s r 3 t r r 1 r ts P P s r r rt s t 2 t r r t r 3 2 r r 3 t r r t t t2 θ kb s ss t 15 t r s r r 1 t 2 8 rt r r t s s t s r s r t s r r 1 t 2 t R M R M r t s r r s P t t s r t t t s t s s t r P r r s s s t rst s B o s r 1 t 2 t s str 2 s st rs s r s

123 Pr t 2 tr s str r rs s 2 Orbit P216 April 3, :37:11 10:38: B 2 (nt) B (nt) 1 r r rr s t 2 tr r t r r r t P t ts t t B o = [ 1,02, 0,18,8,27] r ss t s t st rt t t s r s 23 t t t t s r t ss t t str s 2 r s t t t rt r s 3 t r rr r t 2s s t r rt s s t t rt r ts r r t st 2 t rr r t t s ts t r s s s r t s t str t r t r t P r r q r t 23 t P r t str t s r t t s t s P s s t s s t t r q 2 s t t t r t 2 tr r q 2 ±1 ts t λ 2 /λ 3 10 ts t r t t2 r r 3 t % P s s

124 Pr t 2 tr s str r rs s Degree of polarization Ellipticity Coherence Orbit P204 15:30 15:45 16:00 16:15 16:30 15:30 15:45 16:00 16:15 16:30 15:30 15:45 16:00 16:15 16:30 Universal Time (hours) r Pr rt s t tr r q 2 s s r 2 t s r t r rt t r t P r t s 1 t st 2 t t r r t t r t r rt s r t s r s t t r r t s ts r s s t t rs s t tr st str r t r P r ts t s st t r t r s tr s t2 t r t r t t r t 2 tr r q 2 t t 3 2 r ss s rr s t t P s s r r s t P ts r s 2s t r t s r R M s s r r s t s t r s st ss t t t s r r t s s r 1 s r r t s t t r s t s t 1 t r t st t r s s t s t2 r s s t st r s r t t s s r t t r s t 2 r t str 2 t r s s t t t s st t t s 2 s r s t t s r r P r ts t s t2 t r s r ts α V,B s t ss t tv SW s r t t rs rt r r s r s r t t t r t s t t2 t s t s t r s t t r t2 str t t 2 r ss s rr s t P t r rs s r s

125 Pr t 2 tr s str r rs s 0.35 Orbit P δb/b o Altitude (R M ) r r t t s r s t r st r t t r t P r 1 t t y = A 1 ( r a ) 2 s s t a = ( ± R M t r s t P t r s 2s t r t s r 10 s s r s t s 2 st t st s t t t s t t s 10 r s s s t s t t r s t s s t r s s s tr s s r t t r t s t r t t t st t2 s t r t s st t t t s t r t s t 2 t r t str r rs s t ss r 2 t s r t s s r 2 r s t s 2 t s st t2 t α V,B str t t α V,B st t rr rs r t s r s s r t r s r s r t r s ts t t r r r s ts s t str t r r s 23 t s t str t t r t s ts r s r s t r t s2st r s s t t s r r t r t t tr t r2 t Y MBE,Z MBE r P r ts r s s t α V,B st t r s s r s rr s t P P r s t 2 2s s t s 2 r r t s t str t t s t t s t s s s P s s

126 Pr t 2 tr s str r rs s r t P λ 2 /λ 3 θ kb 5 5 α V,B t s s s t t t s s s st s t r ts r t r r rt s r t t r t r r 3 t t t2 r λ 2 /λ 3 θ kb 5 5 α V,B t t t rt s t s s t t s r t Z MBE = 0 r t t s r t s t t s r s r s t t s t str t P s tr st t t s t str t s s t s t t 2 t s t tr t t s t rr t t s t α V,B r t t 2 t tr t r r r t s s r s r E s r t 2 t r t r st s t t s st 2 s t r r t rr r t t s t P P r s P s r r s t t P str s r t s t 2 2 r t t s t 2 t str r r P s t s r P st r r r r 3 t r t t s s r P s r t rr P s s r t t s t α V,B s t str t s r t s s s t r 60 P r r s s r t rs 55 t rs s r s

127 Pr t 2 tr s str r rs s Amplitude (nt) Altitude (RM) r t t P s s t t t t r P r ts r t r st t t t s t t 2 r ss s rr s t P s r t s r r s rr s t P ts st r t 19 s st t t t tr2 t t s t 2 r P t P t r t rr t s t P P t r t t t r s t r rt s t rt 2 r 1 s r r 3 t r t s t t t r t s t s t2 r t s s rt r 2 t s s s st t t 1t s t r r t2 P s str r rs t s r rs st t 2 r 1 s r P s rr r t r r t r t t r r r r s st 2 23 t t P r ts s r ts t r t r r s r r s t Ω cp s t r t r t st str s ts r2 P r t t t t R M s t s s P s s

128 Pr t 2 tr s str r rs s Amplitude (nt) Cone angle α V,B ( ) r t t P s s t t r P r ts r t r st t t t s t t 2 r ss s rr s t P s r t s r r s rr s t P ts s 2 t s r s t t r t r t t r t r s str rt s r t s t t r s t s s st s t t t s r t st r t t t r t r s t t 2 t t s r t s t s s t r r r s tr s t2 P t tr s rs t t r s t t t δb P δb s t r t r s ts r t r s tr s t s t ts δb st s r t P s st t r s t t r s t s r r r r s s t s t t r s r t t t s t Ω cp r t t t r P t t r q 2 f cp ± r Ω cp = 2πf cp 3 s t rr r f cp ss t t r s r t s s r r t t r P r r q s f > f cp s ts st r t t 2 st t f N t 2q st r q 2 rs s r s

129 Pr t 2 tr s str r rs s 6 4 Amplitude (nt) Z MBE (R M ) Y MBE (R M ) 0.1 Z MBE (R M ) Y MBE (R M ) α V,B ( ) r r t r2 t s r t P r ts t P s r t r r r 2 t t t s r 2 r 2 t ss t t t s r ts r t s s r P s s r s rr s t P P r s t 2 t P s s

130 Pr t 2 tr s str r rs s 3 r t t r q 2 s s r t s t s t s < PSD(f) > fcp+0,015hz f cp 0,015Hz > k{< PSD(f) >f N fcp+0,015hz + < STD(f) >f N fcp+0,015hz } s s 2 r 2 s t s r r ts t t t r s tr t Ω cp t t = s t s s t r ts s s t r s t Ω cp t r r s q t r st t st r s s r r t r s r ts t r s s 1 s t t t s t t r t 2 tr r q 2 t s s t P δb s t t r q 2 f r t t r r s tr s s t f cp = t r r t t 3 s s r t t r r t t r r q s r 2 s s ts r 2 s t q t 2 t t r r t2 t P s rst str rr r t ss t t r t s s t r t r s t t r t r 2 t t t r t r s r ts r t r s t t r2 t rs t r t s r r t st t t t r t r r t2 t s r t r t t r r2 r ts t r t r r rr r t s t s tt r s t t r t P s rr r t r s rt s s s s r s t t r t r r 1 t 2 rt 2 r r s r t s rr s t t P tr s t t t r r2 r t s r t t s t r 2 t s s r t r t r r t s t r s r q 1 t r r s s t 1 t t r t r r t rr t r 2 r r s str r s s r rs r r2 r s r s r t t t r r2 t r s t t ts t rst t r t t r P s r r s r t r s r t r r r s s s r P t s r r r 2 s t r t r r s t t t t r str t t r t r rr r t s r s st t t st t s t t r s s t s 2 r t r r t str r rs s r s

131 Pr t 2 tr s str r rs s f c r P δb r r r s s t t t s t Ω cp s t t r q 2 r rr s t t rr r t st t f cp t s r t s ñ t r r s t2 r r q s r t t r t t t r s t r 2 s s r 2 s s s t r s t tt r s t s s r t t r t t r r Ω cp rt t r r ts t s r tr2 t s st t t tr r t r t r s rts t 2 t s s t t 2 r t2 t rr t Ω cp t t t ttr t t t r ts t s r t rt 2 r 1 s r 2 t t r t r t r s rr t t t s r s < R > t st t t st t rt 1 s r r q r t r 2 t r 2 r rt s s s ts r s t2 t r t r s s t 3 t r t s r ss s t s rt t 2 t r r r t rs 2 s r t t t s t r r t t s r s ts t 1 s t s r s t t rs s r 2 r P s s

132 Pr t 2 tr s str r rs s r rr str s t Ω cp t t r t r t r t r t s r r t r 2 ts r t r ts r s 2 s t2 rs t P 2s r s t2 t t t r s r t t2 r st t t r rs r P r2 s t r s r s r q 1 t r s t r s r s r s st r r2 s t r s r t q 1 2 r t rt t t r r s t str t r t r t s r 2 st t r r t s r t s r r s t s st t r s s r r s s t r q r r t rt r t 1 s r r s t2 s r s 1 t s s t s t t 1 s t r t r s t2 r 2 s r s r t s s 1 s r s t s t t r t s s r r t r r t s rs s r s

133 Pr t 2 tr s str r rs s 2 r tr t t t rt t r s r s r s t s r 2 s s s r 1 t r t 2 t 3 t s s t t rt 1 s r t t s rt t t t t s t t t r t 3 t r 1 r t s t s r t t2 r t r s s t2 r r t s s sts t t t 3 t r t s t 1 r r t r t s r t st r r t t t s st s s t r t P s t rs ss st t 3 t r t s t t t t s r t t2 t s r st s rt t r 2s s t t t t r t r t t r t s r 1 t rs t r2 s t 2 ± 2 s 1 s st t t tr s t ts s s t r t r2 r ss t s r r t t t s t t r r t2 s r t r rr t s r t s t t s t t r r r s t t t r s s t Ω cp s r t tr s t2 r t s t t s sts t t r s t t s t Ω cp s t r s t r s t s t2 t t r t str t s r t t r ts t 1 s r tr s t s t r ts t r s t2 t t r t s r rr r t s t Ω cp r t 1 t t s s t 1 t rs s s r ts t r t s tr t t t t r s s r2 t s t r s t P s r t t s t 2 r 1 s r s t s t r 2 ss t s t t r t 2 s t s t2 t t t 3 t r t s r st t r t s r ss 2 t t t t s 2 t s s t r t rt 2 r s t s r s r t t2 t s 2 s 1 s r r 2 t s r r t s r s t s t r t r s t t 1 s r r t r été r 2 q t 3á 3 t s t 2 s t s r t r t rt t t s r s r s 2s t r 1 s r s t2 t t t t rt t P t s t2 r r t t r 2s s r t t s t t t st t r s t t s s s t r t t r t s t s t r t s t r s r rt s P s s

134 Pr t 2 tr s str r rs s t 2 r t s t s r s t s r t t2 r s t tr t t r s r s r t tr st s st s t2 r s s 2 1 r rs r s t r s r s st r r2 r s r s r t s t s r t s2 tr r t r 1 s s r 2 t tr st ts r rr r2 r r s t 2 t t t s tr t r ts s t s s t2 t s s t s t t s s t s s s r r t 2s r s r 2 t s s t s t s t t r t r t s s r t rs t2 tr 1 s r s t2 3 t r t s t s r r t2 < R > r t t t s s s t r r t 2 r 1 s r rst t r rr t s t2 r s s 1 r r s t r s r s st s 2 r s r t q 1 s s st t t t rr s 2 t 1 s r tr t t t s 1 s r r s s t s s s s r t rr s t2 r s s 2 s t s t s s t r r t s r t s s t t s s t s t2 s t s r t 2 t 1 s r s t r r 2 ss rr t r s t s r t t P 2s s s r rs s st t t t t s t t s s t2 t t 2 rr r s s t t r t r t s s s 2 t ss s r t t2 r s s s s r s 2 st t t r t2 t 1 s sts t t s r ts t t r s r t s r r t r s t t t t s 2 t r t r t t st t2 t s r P s t 1t s t r r t 2s s t r 2 t str r s rt r P str ts r s r t t s r r rt s t s r t str r t s s t str ts t r r r t t t 1t r t s r r t r s t s tr r q 2 s s rs s r s

135 Pr t 2 tr s str r rs s s str r s t s t st 2 t P s rr r t str r t s s t t r s rt t r r t t t t s s t r s s t t P s rr r t t rs rs t rr t t t rt tr st r r t s r t t2 t t ts t s t ss t q t 2 ts s s r ts r t r s r t s tr st t t s s t t tr st ts s r t 1 t t s s t s t rt s t tr t2 t rt r t s t tr t2 t s r t s r t r r r t s r t t2 r s t r r t ss ss t st 2 t r r t ts t s s t 23 t P s t r s t t r t ss r t s 2 rs 2 st r s r t s t s 2 rs t r s s t r 2 r 2 r t s s t s r 1 s s t t s t t r t r t r r r t s t 2 t P s r t s s r t t s t t 3 s r rt s t t r t r t r s t t s r t t2 r s t t r t t s r r t r r r t s r q 2 3 r r r s t r t s t t X VSO 1 s t t r s t s t t t t2 V SW s t t r 2 t r r t t Z VSO 1 s r r t s r t s t t t rt Y VSO 1 s t t r t s2st s t s rs s st t t s t t t r t t s s t t str r s s t t r t r t r t r ss t t r s tr s t t s r t s r s ts t r s st s t 2 P s t t 2 s t r r q 2 t r r t r t 2 tr r q 2 s t t s t s rst t 2s s t t P s t s r ss s s t P s t rs r t 2 r s r t st s r t t r s r rs s r s t 2 P s s

136 Pr t 2 tr s str r rs s r 1R V = 6052 r t s t t s r t t2 r s s s r s t r t t t r s t t r P s r r s r 1 t s 2 P s ts t s s t s r t s t t s r r t rr r s s t q st t r t t rs t t P s t s t r r q t 2 s r t s r 1 2 t r r 1 t 2 t t s r t r r t 2s s t s r t s t s t s tr2 t rst t r t 2s s s t s s r r s r t t s t s rst t st t2 t t st r s r s 30 s r t s r 1 t t 1t r t s r r r t t t t s r t t2 r s t s r t r st t 30 t r r r t t st t s r r r r s t s ss r P s r s r r q s t r t s t t s r t2 s 1 t r t r t s s r s t t s s r t s r t st t2 r t t r P s r s r s r tt t t r s ss s t s r rt s t s t r s r t s r t2 t s r r t s t2 t s r 2 P r t2 t s t s s r t rt s ss t t t t2 s r 2 t r r t r s t P str t r s t r t r t s r s t str t s r t r 2 st r s V SW r s t r s t s r r t r s r 1 s t t V SW s t s 1 r r s r 1 t t r t s r s r 2s t P rr r s r s 2 st r s t r t rr P s s t V SW s t s s r P s r r r q t 2 r r t r V SW s 1 r s r 1 s r r s t r s s 1 t t s s t r s tr r s s t r r r 2 rr s r V SW r t s 1. rs s r s

137 Pr t 2 tr s str r rs s to (2006 DOY 130 to ) to (2011 DOY 60 to ) No. of occurences [%] PCWs (ns=153) Vsw (ns=452) No. of occurences [%] PCWs (ns=439) Vsw (ns=457) Vsw [km/s] (1 val/day) Vsw [km/s] (1 val/day) r st r s r s r s P P t r s r s t t s r s r s r t s r r t r s r 1 t s r s t t t r r ss t s r t t2 P s r r r q t 2 s r r s t s r s s s 1 s t r t r s r s t s t s s t t t r t r t t s r s s t r s r t t2 t t r s t t t r s r2 t P s r t s t s t r t t t s r t r t s 2 t r s t t t r s t r r s t s 2 r s t t st t2 s t s t r t 2 s t s r t s r r V SW r t s t r ss t t r r r s tr t t t r r r 2 t t r st t2 r r t 2 ss t t s r s r s t r t r t s s t 2 r t r t s r P s r s t2 t s t s r t r t s t2 r r P s r ts 2 r s t s t t t t t t str t t t s s s r t rts t s t s r t r t t r s t2 st t s t s s t s r r t r t P s s

138 Pr t 2 tr s str r rs s t s t r st s t s r r st t 1 t t s r st t t r t r s r 1 t s r s s t r rr s t r s r 2 s t t P s r r t s t2 n p r t s t s t s r r t 2s t t P s s 2 n p s r t 3 r r P s r 2 r s t s r t 3 r s r 1 r r t t r s r r t r s t2 r t s t t P s r s r t 3 tr r r P s r r s t s n p 3 s s r 2 s s s t t s t t P s r r r 2 r r r s r s t2 s s s rts t t t t t r t s t2 t r t r2 r t s t r s t t t r r t s 2 s t r t s t t P s r t s s t s r r t s t2 r s r 2 r r s r 1 2 t r t r r P rr s s r t t t s r s t r s r r P t r s r 2 s t t r t r s t2 P r t s r r t r s r 1 r t 2 r P s r r s t2 s s t s s t rs s r s

139 Pr t 2 tr s str r rs s t t s 2 r 1 s r 2 r r s t s s t t t r2 s t s s s t s r r t s t2 r s t t r s r 2 tr s t r r t s 2 r s r st t t s s t st r r t r s r t s t r s r t s r t t str P s s r t t t r t t t r2 r t s t2 t t r s r r t s t2 t s s t s rt r t t s r t s r r 2 r st t r t s t s s s t q st t s t t r t r s r 1 r t t t r r st 2 t t 1 s t r r t r s r t rt s2 t r r t 3 t r t t t s 1 s r r s s s s 1 t t rt t t t r s t2 r r t s t 1 s r s r t t r s r s t t r s t2 2 r t t t r r t s s r t t2 r t r r s r 1 2 t t t s r 1 t s s t s t r s r r s ts t r t t t 2 r r t t r2 + s t2 t t t R V t st rt r r 2 r t r s r s t2 r s r 1 t r s r 1 s t r s 3 t r t t t 2 r s r s ts s t r r s t2 r + t r t t s t r t s t r t s r s r r s t2 2 t r t s r r t s t r s t2 1 s r r t s r s 2 t r r t r s r s s r t t2 t 1 t t t r t t t s t2 t r2 r t s t t s r r 2 t r r r r t r2 s r st t tr2 s 2 r r 2 t t r s t r rr r t P s r s r 1 s rt r str P s t s r s r 1 r t s r r t r s 2s s t t t t t q s t r t s t t t2 r t t r r t s t2 s 1 s r r t s t r s t t t r r t s t2 s t 2 r t r r t r r s r r t 2 tr s r s r 1 P s s

140 Pr t 2 tr s str r rs s s ss s s rst t t t t s t t r s 2s s s t t t s t r str t rt s s s r s r t r t t r t 2 tr r q 2 r t t 2 r 3 r s r s s s t t r r t t s P s s t r s t r t r ss r t s r t 1 s r 2 r rs s 1t 2 t r s s ss t s r st s r s r t s t t r str t s r 2 s r s r s s st 2 r q 2 s r t 2r r q 2 t s t t r2 r r rt r r st s t s s t s r r t t s v ion r2 s t t t r q 2 s r s t 2 t r t t t t t r t t Ω ci. s r t r 3 r t t r t v ion st t r r t r 3 t s s r t t2 str t s r t r t r 3 r t 2 tr t r s t t t st st t r r s r s t t s s t t str t t t r t s t r s t t r s s s t s s s t st tr t r r r r s r 2 t t t r 2r t t s r t s rt t r t t s r s t t r 3 t t st s r rs t t t s s t r r t s t t 2s s r r t t t s rs t t s t r V SW s ss t t rs r t t s t t r t s r s t s r t s t s s r ts t s ss t t r t s t2 t s s rt r t t k V SW t t s ss r2 t t t r rr t t t r 3 t s r s r t r t r s ts t ss t t t s s s t r r t t V SW s t t r 95 t t s st t s s r t rr s t t s s r t t r r r t r s r 90 t r r s t r t 2 2s s s s t t t P s s r t rs r r r t st r t B s 3 r θ kb t r s t r ts rs s r s

141 Pr t 2 tr s str r rs s t r ss t s st 2 3 t s r s s r s r ss t2 t2 2 δb par /B 0,25 r ss t2 t s s s st r t r ss rr t t t t t tr 1 t t tr 1 s t s r 12 t tr s t2 t r t t 1 s r t r ss rr t t t t t s r s r ss t t s s ts t s q t2 t s r s t s t 2 t t t rs t t t s r t 2 t s r t t t r s t t str t s s t s r s rr r s tr r t t t st ss r ss rr t t t t t s r s t t s t t r ss rr t r s r t r s t t s t r t s s s r t r s ts t 1 t rr t t t t s r 3 r t s s t t t r s s2st t rr t t t t t s ts t t rr rs s 2 t s r t s t t r s t t s t s r s ts t t t t rr t s t ss rr rs r t s s r t 2 tr r 2s s s r ts s s s t t t r q 2 r 3 t r t s s t s t t r t t rt r t t t t s s t s t t s r r s t t t s r s r t ss t t t r s r r t s r t 2 str s t q s r t t r r q 2 t r s r r t r t 2 tr r q 2 3 t t t t t t s r s s s r s s t t t r st r t t r s tt r t s rts t t t rs s t s r t s s t r st t r t s r P s t rs s t r r t t r s t t s r r t s t r r s r st s t t s st t t t s t r s t r rt t r t r 2r t str t s str r t rt s s s s r t t rt s r s 3 t 3 t t r t 2 r t s s s st r t s t r r r t s t t tt r s r t s t 2 t s r s t t 2 r t s t r q 2 s t t 2r r q 2 t r r s r t str t s 3 t t 2r tr str t s t s r t t s t P s s

142 Pr t 2 tr s str r rs s t t tr E t s t str t s s t t t P s s r t str r rs s sts t t t t t s t str t t s t s s t s t t t t s t ss st t rr t r s s r r r r t t t s t t t t tr 2 s r t t t P s t r st s ts r s t r ts t B > 5,6 r t r tt t 2 r t 2 t s r r E ts 2 r t t s r r r t 1 t s r t t rs r s s r 1 s r 2 r t s 3 t r t 2 t t tr r 1 s t tr s r t t st tr t r st t r s t t t t t tr s 3 r t s 2 tr s str t t t s r tr st t t s r s t t t r P P t s t str t r st s s r t rt r s t s t t r t t t t tr t r r r str t r t r rt r r s r E s r t 2 s s r P s r 2 t t s r t t r s s t s t s st t tr 1 t t t s s t t t str t s t ss r 2 t t s t s rt t t t t t s r t s s t s r t r2 s rt s t2 s t 2 t s r s r s t st s r t t r s ts 2 ss t s r s t r t t t t t s r t r s r P t t r t s s rt t t t t t t t rr t t t s t str t t P s t t tr s s s r t s t 2 t 2s s r r t t s t r st r s ts r r t rr r t r t2 t P s s r t str r s rs s r s t 2 t s rs r2 r r t s r t s s t r rt s P s r s r t s t r t P P s s s r r st t st st 2 t t s 2 s t r t t r s t s s st t t t tr2 t t s t 2 r P t P t t 2 t s s r t s st t t r r t2 t s s r t s t t t r 2 rt rt r r rt2 s r t t r t r 1 s r t 2s s t rs s r s

143 Pr t 2 tr s str r rs s rr str tr s rs t t s t Ω cp t s t r t t s s s t t t t s s r s t t s r t s s t t t s r t s s t 2 r r t rt r r s t r s r t r t s r t q 1 s r r t s r t2 s t s 2 s r t r tr s t s t s t s 1 s r t r s t t t t r s r t 2 s r r t t t r r s t t 1 t2 t s r t t r ss s t s r s ts s st rr t t t rr t s s t t r t t st t rt r ss t t r t 2 s t s t2 t t 3 t r t s r st t r t r st r t s r s ts t s s rt t t t t t t t s r ts r r r t r s r t s s t t ss ss ss s r t t2 s t rt 1 s r t r r t P s rt t 2 t s s t t s r s r ts t r s t t s r 1 t s s r tr st ts t P s rr r t r t 1 t t s s t s t rt s t r t t r s r 1 t 2 t s r t r t rs t t t s r t 2s s r r P t r rr P s r t t t s r ts r t t s r 1 r t s r s r s ts s s st t t t t q s t r t s t t t2 r t t r r t s t2 s 1 s r r t s t r s t t t r r t s t2 s t r s s r t r t r r s r r t 2 tr s r s r 1 P s s

144 Pr t 2 tr s str r rs s s st st ít stá tr st s tr ét s s r s r s s 1ós r s 1t s rt 2 s s í t r t r 3 s s s r s r r 3 ó r t 2 s t s s 1 ó q s s 1ós r s t r s s t r t r 2 s r t s r s s t r ó r s ó s q r s r ó st t 1t r r s ó s t 3 r t 3 r q r r s rá tr s r t r 3 st s s t s r t t s t r ó t ó str ó s s s r s s s rtí s r s t r t t s r2 rt r st s r s s t r r ó s rr s t s s r s rr s s r s t s s q rtí s 1 s ér s tr s s t 3 s 2 s s t t t r s r t s r q r s s r s s r s t st s r s s r tró r t s s t t rt t s tr t t r ó tr t s r 2 rt s 2 q q s t t s s r s tr és 2 r s s tr s r r í 2 t t tr t s r 2 s rtí s t r s st s t t s 1 s ér s s s s tr rtí s s r t s 2 r t t t r s t á s st s tr s r 3 s r t st t s s r r s s t s s rt 3 3 Pr t 2 tr s str r rs s r t s r rs r 2 r P t rt r á 3 r r r t2 s t t r t 2 tr r q 2 str r rs t r rs s t t 2 r 1 s r 2s s tt rt r 3 str r t 2 tr s t s r s r 1 2s s P 2s s s 1 s s rt 2 s stá 3 s 2 tr 2 t t r s t t t r r tó t r rt 2 s s r 2 r r t rs s r s

145 Pr t 2 tr s str r rs s P s s

146 P t s s r t t 2 s r s r t r ss s s t r s t t t st 2 t s r rt s s rr t r s r st s t t t t s r s r t r ss s t ts t t r t r ss s r t rt st t t t t t s r s t ts t r t t ts s r t s ss t s t 2 2s t t r ss t s t t 23 t s r s r r s s r s r s t t r 2 t s s t 2 r r s r t s r 1 s 2 r t r t s 2 2s t t r t 3 s t t r st t r s r s t st 1 1 t t r t t t s r t 3 t ts s r t r s r s2st s 2 t t t t s r t r t r ts t r st t r r R s t r r s r t r t t s s t t 2 r 1t r t s rt

147 t s s r t t 2 s r s r t r ss s t s s rt 2 t r s t t r r r t2 t t r r s t s s 1 r rt s + t r r s + s t r r t t r t s r t rst r r r 1 t r t t s t t t s ts t t s t r s t t 2 t r s t t t s t s r t r t t s r t r t r t t r t t r t t2 s 1, t r s t t s r t s r t2 s 1. r 2 t t s s rs s s t ts rr ts s t t s 2 t s r ts s st t t s t t t 1 s r ss tr s t 2 t r s t r t tr st t t t t r t s r t 3 ts t r s s s s s s r str r t s t t s t s st t r s t t r t r t r t t s r t r st 2 t t r t t r s t r t t s t t t s t ts r t s s r s r s t t r t t t r t r s t r t r t t t t s r r t t s s s r t s r ts r t s t t s r r s t r t t r t t s t t r s t t t r t r r s r r t r t s r t rt r t r t r t s r r t 1 s s s t s t r t s 2 r r r t s r t rs s ts t r r s t s s t s r t r t r s t s t s r t t r t t s s r t t r s t s s ts r r ss t 2 s t s t t s st st r t r s s r 2 str t t s t R s. r r s r s 2 t t s st t t t t t t s r t r rt t st t t t t s s t s r t t t r t s r 2 r ss r s s t 2 r t s t 2 s t t r t s t rt t r t s r s rt t t r st 2 2 t tt r s t r s t t s t s t t t t rt t s r t tr t2 s t r t s r s r t t t t r q t r P s s

148 t s s r t t 2 s r s r t r ss s s t s s r E = (v B) r t r t s rr t r t t s t r t t s r t s r t r s ss t t t r s t r s t 2 s ss t t t s r r t r t r 1tr t r t s t s t t 1t r t r t r 3 t t s t r t s s s r rst t t r rts t r s t s r t t r t q t r s 2 str t r s s str t r rr t s 2 t r t s t s t t t s t 2s tr s t s t t t t t t s r t s t r t 2s t t s r s r ss 2 t s r s st 2 s t t s st s s r t R s s t t ts s t t s r t t s s 2s r s t t s s t ss t t t t r t s r s ts s t 2 t r t s r rr t r r s s t t s str t r s s s r s t r s 2s s str t t st rs t rs s r s

149 t s s r t t 2 s r s r t r ss s r s t s r t t r t t s r t t r s t s t s s t t s t rr t s t t t r t r s ts t t r s str t r t rr t s t t t r t t s r t t s s t s r st ss rr r t r s rt r s r t r s r ts t t s s t2 t r t t t s s t t s r rt t q t r r t t r t s s s t r s s t s t r s t s r s 2 r ss t s ts r t r r t t r2 r t t s r s t r t r s t r t s t r s r 2 r t t t s t r2 r t t s t t s r str t r t t r t s r r t r ts ré t s s r t t t t t t s r t r s t t r s s t t t r2 r r t t r s t s r t s r r s s t t r s t str t s t t s t t r rt t 23 ss t str t t t t r t t t t str r t r2 2 t r t s t r t r s t s r rr t s t r t s t st t t t rr t s t r t t r s t t s r s t s t t r t t t rr t s t t r s t t t r t t q t r t s r t rr t s t t r t r t t ts 2 r r t r s t r r s t 2 t s t rr t s t t r t s s t 2 r t r t t 1t r s s tt r t r t s r t t r s s st 2 t t s t q t 2 t r t t t rt r ss r s t t s t s r t s t t t t 1t r r t s t ss s s 1 t s r s r str2 r t s t s r s r2 s t s r r ss r s r t t s r r ss r rt t r t2 t s 2 s r t rt t r s r 1 t 2 t t s r s r t r t s s r t t rt s s r r t t t s r s sts r tr 2 r r s r t t t t t r t t ts r t t 1 s s ss t r r t t t s s r r s t r r t s 2 t r s 1 t t s P s s

150 t s s r t t 2 s r s r t r ss s r t s str t t st rt t r s t s r t st rt s rr t s t t s t t r r t t r s t s st rt t r s t s rr t s t rr s t t r t t r s rt r s r r ts t 2 r r s t t t 2 r r t t s t r 1tr t r rr t 4 s r t t s r t r 2 r 2 s t ts tr st t s st t t s str 2 s t 3 t r t s r r t r t tr s t r s t s r t tt r r rt t r t ts t s t s r 3 t r rts t s t s r r t ts s r s s q t t t r s t 1 r t ts t s t r t t t s r t s r t r st 2 t t r t 4 t r t s r t t s tr t t r t s r s 2 r r s t r 1 s st t s s t r t s r r t t t t t t s r t t t t s s r r q 2 r r s r r rs r t t t 2 r r 2 r r s t tr r t r s s s 2 r r 2 t t r t t r s r 2 rs t r t s 2 rs t s r t 2 t t s s r t t r2 r t r 2 r t t 12 t s rt t t t s t s rs s r s

151 t s s r t t 2 s r s r t r ss s r r s t t s r t t st t r s t s r str t r 2 r ss t s ts s r s t t r r t r s t t s t t t r 1tr t r s t 2 r tr r r s t t s t s r r t s t r s rt s s r t t t s r t P t 2s s t s t r t rst t 2 2 s st t r s t ss tr t rt t r 2 t t t r t s r t 3 ts rr ts s t t s s r tt t t r t t 1t r t r s t r tr t t r t rt r s t s t 1t r s s s r 2 s s r s t ss 2 t s 2 ss s r r t r t s r s t s s t s t t t t t t s t st t s r r s t t s rs rt t s s q t s r t t r t 3 s t s r rt s r 2 t t r s s t s r st t s s rr ts s t t s s r r t s t 2 str t st t t 3 s s r s t t 3 s r s s 2 s r P s s

152 t s s r t t 2 s r s r t r ss s t s t s r 2s s t r s s r rt s str r t r s 2 st 2 t s t t r 2 t s t s r s t r t s t r t r ss t t s r r r t t s r r 2s s rt s s t t r s r ts r 2 ss r s t t 2 2s r ss ts t t s r s t s t t r s r t r ss s r s r t s t s t s t t s r s t s r tr s rt str r t s r s t t t r t t t r s r tt t st t str t r t s r 2 r s r ts s st t t t s s r t tr s t s r t t t s r t r tt t s st t t t t t t ss r t s r s s t s s 1 r r t 2 t 23 t s r t r t r t rst s r t t r t r r ss s r t s t s s s t t t s s 1 t s t 3 t r rt t r s s r s t s r t r t t r r ss 2 2 t st t ss t t r t s s 1 tt r t st ss t r t 2 2s st t t t t s r 1 2 r t r t s t r t 2 2 s s 1 r t 23 P s r Pr s r t s r s t s r ss t 2 2s 2 r t 3 s s t s t t ts t t t s r r ss 2 rt r t r ss t ss 2 s r t r r s ts s st 2 str t r s r s s r t t r t s st t r ss r t s s tr t t t s s r t t 2 t s s r s s r t s r r t ss P s tr t r tr s r t s t t s st t t r 2 2s s st t 2 t s t 2 t t r s s r s t t r t tr s tr t r t t t t t s 2s s r s r t s r 2 q s s t q t s str t rs s r s

153 t s s r t t 2 s r s r t r ss s t 2 s st t t t r tr 2 t r r t s 2 st t t t s ss r t s r t t r r s s 1 r t t r 2 2s t t t r s st s t r t t ss r t r t s s 1 s s r ts r s t rs ss t t s 2s s t s r s t r 2 2 s t t st t s ss tr ss tr t r s r t s t t t t s r t t t rs s t s t s t t t s s t s s t t s t 2 s st t t t s s st r t t 1 s tr s rt t t t t t t 2 t t r r ss r t r s 2 s t t t t t s t r t t r t t 2 s r t t r st t t st t t r t t t s r s t r t s r s t t s s t r t s r s r 1 t t rt t r t s s s t s s r s r é str t r s r r s t r r t s str t r s t ts t s t2 t t t t s 2 rs r s s t t t t s r s s t s 2 t é r t t s st 2 23 ss s s r t s t r 2 2s s t s s s ss s tr t r2 1 r t s t t s t r t r 3 t s s t r s 2s t tr t r2 ss r t t r 2 2s t s r t r t r t s t s t t r r t s2st t X TIIS 1 s ts t r t r t t t Y TIIS 1 s ts t r s t r t Z TIIS 1 s t s t r t s2st s t s ss s t t s r t t t s r 1 t 2s s 1 s r str t ss s t r 2 s tr s t st t t s t2 t s s r t t tr r s t2 t s r t s 2 s t é s t s r 1 s 2 r t t r r 2 t t t r s r t s r t s ts r r é t st t 2 r r t t s r ts t t r t 2 s 2 s t r s t 1 s t rr t 2 rs t t t s r s r 1t s t r s ts ss s r t s 2 st 2 st s r t t t s r t t 1 t t t 2 s rr t t s r t r P s s

154 t s s r t t 2 s r s r t r ss s 2s s rt r t s st t t 2s s r r s t r t 2 2 t s r st s r r r 2 2s data1 T1 T4 T1 4 2 T17 T19 Z TIIS (R T ) Y TIIS (R T ) 2 4 T X TIIS (R T ) 2 4 r r t r2 ss r t s r 2 2s s r t s ss s t 2 2 t r2 t t s st r t t t t t r t s s r s t t t t s ts t s r t t s s t r s s P P P s r t s r t s 2 2 t t t r t s s t r t P s s s r t s s 2s t tr r s t2 r 2 P t t r s P 2s s r r s r t r 2 r r q 2 r r s tr r s t2 r t t t r t r t s tt r s ts t t ts s r 2 r t s r r r s s t Bx TIIS By TIIS Bz TIIS t ts rs s r s

155 t s s r t t 2 s r s r t r ss s r s t 2 t r s 2s t t t s t2 B TIIS Magnetotail r P P s r t s r 2 2 s s t s r t P s r t s s 2s t tr r s t2 r 2 P t t r s P 2s s r r s r s r t s r r s tt r s ts t t ts s r 2 Bx TIIS r By TIIS r r Bz TIIS r r t t t s t2 B TIIS r t ss s t t r s t s r t s s r s r t r 3 2 tr r s t2 r t 3 t t ss t rs t s t s r t tr s t2 r s s t s r t r s t s s r t t s r r 2 t s s t 2 r s s r t t t s t s r ts s t t ss s t 2 Bx TIIS > 0 t s t t tr2 t t t s r t r t r t Bx TIIS t t r t ts r s P s s

156 t s s r t t 2 s r s r t r ss s t t t t s t s r s r t t t r t t X TIIS t t s t s s t r t t 1t r s ss r s t 2 t s t t t t r rs t Bx TIIS t t t t 2 ss s t s t s r t t r t s st 2 t st t s r s t t r 2 t s r t ss t t t t s r s r s t r t s t t r s 1t s t s s r t 2s s r r P P s r ts r r t st t t t2 t s t é t2 t s t r r t r s s t 2s s r rr t t r tr r r t r t s2st s r t s2st s t r t t r t t X KSO 1 s t t r s t t Z KSO r r t t t r s r t t t rt t t Y KSO t t r t s2st P s r t t r t t r t s t r t P s s t s s t st t s P t t t r s t t s r t r t t r s ss s r t t t t t 3 t r t s s t r str t t r str t r t t r s t str t s t r r r t ts tr t s s t t t 2π st r s r 1 s r t r t t s 2 s 2 t str t s r tr 3 2 t r s r r t s δ θ t t δ s t t t Z KSO = 0 t s t r t r s r 90 t +90 t θ s t t X KSO Y KSO t s s t r θ = 0 rr s s t t r t t X KSO 1 s t t t tr s r t t 23 r t t t r t t s r t r t t r t s t r t q s t t 2 s t 2 t r t r r 2 s st t t t t r ts r r t t t P tt t s r t δ θ r s rt t t r s 2 t t r s s t r str t t r str t t s t s r t r t r t s2st r t s t r t r t str t t s s r t t s s δ θ rt t s t s r r t s r δ = 20 θ = 20 r s 2s t s 1 s s r 2 P r rs s r s

157 Normalized ion flux t s s r t t 2 s r s r t r ss s r 2 2 s t δ θ s ts t t s t ss t t t r t t s s t s r δ = 35 θ = 130 s r t s t r r r t t t r s t s s t t str t s r s ts r s r 3 s E a) a) b) T40: CAPS SNG 2008/005 21:09-21:12 hs F 10 8 T40 : 2008/005 21:10:30 hs 10 7 Flux [cm 2 sr 1 s 1 ] Energy [ev] r r 3 s 1 s r s r 2 P r s s t δ θ r s t s t s t ss t t t r t δ = 35 θ = 130 r 2 s tr t s 1 s s r 2 t s P t s r r t s t r r t 1 t s ts st t P s t r t s s r q r s r t s s t s s t t s r r 2 t s r t t t rt t 2 s r ts t 2s ss t r t s t 1 t t t s t s t s t t t 2 t t r s r t r ss t t t r t s s r tr t t s t2 v t s ss t s t t r2 2 t s s r t s t r 2 s tr r t t r t s t t s r st 2 st P s s

P P Ó P. r r t r r r s 1. r r ó t t ó rr r rr r rí st s t s. Pr s t P r s rr. r t r s s s é 3 ñ

P P Ó P. r r t r r r s 1. r r ó t t ó rr r rr r rí st s t s. Pr s t P r s rr. r t r s s s é 3 ñ P P Ó P r r t r r r s 1 r r ó t t ó rr r rr r rí st s t s Pr s t P r s rr r t r s s s é 3 ñ í sé 3 ñ 3 é1 r P P Ó P str r r r t é t r r r s 1 t r P r s rr 1 1 s t r r ó s r s st rr t s r t s rr s r q s

Διαβάστε περισσότερα

rs r r â t át r st tíst Ó P ã t r r r â

rs r r â t át r st tíst Ó P ã t r r r â rs r r â t át r st tíst P Ó P ã t r r r â ã t r r P Ó P r sã rs r s t à r çã rs r st tíst r q s t r r t çã r r st tíst r t r ú r s r ú r â rs r r â t át r çã rs r st tíst 1 r r 1 ss rt q çã st tr sã

Διαβάστε περισσότερα

ss rt çã r s t Pr r Pós r çã ê t çã st t t ê s 1 t s r s r s r s r q s t r r t çã r str ê t çã r t r r r t r s

ss rt çã r s t Pr r Pós r çã ê t çã st t t ê s 1 t s r s r s r s r q s t r r t çã r str ê t çã r t r r r t r s P P P P ss rt çã r s t Pr r Pós r çã ê t çã st t t ê s 1 t s r s r s r s r q s t r r t çã r str ê t çã r t r r r t r s r t r 3 2 r r r 3 t r ér t r s s r t s r s r s ér t r r t t q s t s sã s s s ér t

Διαβάστε περισσότερα

Radio détection des rayons cosmiques d ultra-haute énergie : mise en oeuvre et analyse des données d un réseau de stations autonomes.

Radio détection des rayons cosmiques d ultra-haute énergie : mise en oeuvre et analyse des données d un réseau de stations autonomes. Radio détection des rayons cosmiques d ultra-haute énergie : mise en oeuvre et analyse des données d un réseau de stations autonomes. Diego Torres Machado To cite this version: Diego Torres Machado. Radio

Διαβάστε περισσότερα

r r t r r t t r t P s r t r P s r s r r rs tr t r r t s ss r P s s t r t t tr r r t t r t r r t t s r t rr t Ü rs t 3 r r r 3 rträ 3 röÿ r t

r r t r r t t r t P s r t r P s r s r r rs tr t r r t s ss r P s s t r t t tr r r t t r t r r t t s r t rr t Ü rs t 3 r r r 3 rträ 3 röÿ r t r t t r t ts r3 s r r t r r t t r t P s r t r P s r s r P s r 1 s r rs tr t r r t s ss r P s s t r t t tr r 2s s r t t r t r r t t s r t rr t Ü rs t 3 r t r 3 s3 Ü rs t 3 r r r 3 rträ 3 röÿ r t r r r rs

Διαβάστε περισσότερα

Alterazioni del sistema cardiovascolare nel volo spaziale

Alterazioni del sistema cardiovascolare nel volo spaziale POLITECNICO DI TORINO Corso di Laurea in Ingegneria Aerospaziale Alterazioni del sistema cardiovascolare nel volo spaziale Relatore Ing. Stefania Scarsoglio Studente Marco Enea Anno accademico 2015 2016

Διαβάστε περισσότερα

P r s r r t. tr t. r P

P r s r r t. tr t. r P P r s r r t tr t r P r t s rés t t rs s r s r r t é ér s r q s t r r r r t str t q q s r s P rs t s r st r q r P P r s r r t t s rés t t r t s rés t t é ér s r q s t r r r r t r st r q rs s r s r r t str

Διαβάστε περισσότερα

r t t r t t à ré ér t é r t st é é t r s s2stè s t rs ts t s

r t t r t t à ré ér t é r t st é é t r s s2stè s t rs ts t s r t r r é té tr q tr t q t t q t r t t rrêté stér ût Prés té r ré ér ès r é r r st P t ré r t érô t 2r ré ré s r t r tr q t s s r t t s t r tr q tr t q t t q t r t t r t t r t t à ré ér t é r t st é é

Διαβάστε περισσότερα

Efectos de la cromodinámica cuántica en la física del bosón de Higgs Mazzitelli, Javier

Efectos de la cromodinámica cuántica en la física del bosón de Higgs Mazzitelli, Javier Efectos de la cromodinámica cuántica en la física del bosón de Higgs Mazzitelli, Javier 2016 07 22 Tesis Doctoral Facultad de Ciencias Exactas y Naturales Universidad de Buenos Aires www.digital.bl.fcen.uba.ar

Διαβάστε περισσότερα

P P Ô. ss rt çã r s t à rs r ç s rt s 1 ê s Pr r Pós r çã ís r t çã tít st r t

P P Ô. ss rt çã r s t à rs r ç s rt s 1 ê s Pr r Pós r çã ís r t çã tít st r t P P Ô P ss rt çã r s t à rs r ç s rt s 1 ê s Pr r Pós r çã ís r t çã tít st r t FELIPE ANDRADE APOLÔNIO UM MODELO PARA DEFEITOS ESTRUTURAIS EM NANOMAGNETOS Dissertação apresentada à Universidade Federal

Διαβάστε περισσότερα

Robust Segmentation of Focal Lesions on Multi-Sequence MRI in Multiple Sclerosis

Robust Segmentation of Focal Lesions on Multi-Sequence MRI in Multiple Sclerosis Robust Segmentation of Focal Lesions on Multi-Sequence MRI in Multiple Sclerosis Daniel García-Lorenzo To cite this version: Daniel García-Lorenzo. Robust Segmentation of Focal Lesions on Multi-Sequence

Διαβάστε περισσότερα

Physique des réacteurs à eau lourde ou légère en cycle thorium : étude par simulation des performances de conversion et de sûreté

Physique des réacteurs à eau lourde ou légère en cycle thorium : étude par simulation des performances de conversion et de sûreté Physique des réacteurs à eau lourde ou légère en cycle thorium : étude par simulation des performances de conversion et de sûreté Alexis Nuttin To cite this version: Alexis Nuttin. Physique des réacteurs

Διαβάστε περισσότερα

E fficient computational tools for the statistical analysis of shape and asymmetryof 3D point sets

E fficient computational tools for the statistical analysis of shape and asymmetryof 3D point sets E fficient computational tools for the statistical analysis of shape and asymmetryof 3D point sets Benoît Combès To cite this version: Benoît Combès. E fficient computational tools for the statistical

Διαβάστε περισσότερα

Multi-GPU numerical simulation of electromagnetic waves

Multi-GPU numerical simulation of electromagnetic waves Multi-GPU numerical simulation of electromagnetic waves Philippe Helluy, Thomas Strub To cite this version: Philippe Helluy, Thomas Strub. Multi-GPU numerical simulation of electromagnetic waves. ESAIM:

Διαβάστε περισσότερα

Couplage dans les applications interactives de grande taille

Couplage dans les applications interactives de grande taille Couplage dans les applications interactives de grande taille Jean-Denis Lesage To cite this version: Jean-Denis Lesage. Couplage dans les applications interactives de grande taille. Réseaux et télécommunications

Διαβάστε περισσότερα

Assessment of otoacoustic emission probe fit at the workfloor

Assessment of otoacoustic emission probe fit at the workfloor Assessment of otoacoustic emission probe fit at the workfloor t s st tt r st s s r r t rs t2 t P t rs str t t r 1 t s ér r tr st tr r2 t r r t s t t t r t s r ss r rr t 2 s r r 1 s r r t s s s r t s t

Διαβάστε περισσότερα

ACI sécurité informatique KAA (Key Authentification Ambient)

ACI sécurité informatique KAA (Key Authentification Ambient) ACI sécurité informatique KAA (Key Authentification Ambient) Samuel Galice, Veronique Legrand, Frédéric Le Mouël, Marine Minier, Stéphane Ubéda, Michel Morvan, Sylvain Sené, Laurent Guihéry, Agnès Rabagny,

Διαβάστε περισσότερα

ss rt çã r s t à rs r ç s rt s 1 ê s Pr r Pós r çã ís r t çã tít st r t

ss rt çã r s t à rs r ç s rt s 1 ê s Pr r Pós r çã ís r t çã tít st r t ss rt çã r s t à rs r ç s rt s 1 ê s Pr r Pós r çã ís r t çã tít st r t FichaCatalografica :: Fichacatalografica https://www3.dti.ufv.br/bbt/ficha/cadastrarficha/visua... Ficha catalográfica preparada

Διαβάστε περισσότερα

Transformations d Arbres XML avec des Modèles Probabilistes pour l Annotation

Transformations d Arbres XML avec des Modèles Probabilistes pour l Annotation Transformations d Arbres XML avec des Modèles Probabilistes pour l Annotation Florent Jousse To cite this version: Florent Jousse. Transformations d Arbres XML avec des Modèles Probabilistes pour l Annotation.

Διαβάστε περισσότερα

Émergence des représentations perceptives de la parole : Des transformations verbales sensorielles à des éléments de modélisation computationnelle

Émergence des représentations perceptives de la parole : Des transformations verbales sensorielles à des éléments de modélisation computationnelle Émergence des représentations perceptives de la parole : Des transformations verbales sensorielles à des éléments de modélisation computationnelle Anahita Basirat To cite this version: Anahita Basirat.

Διαβάστε περισσότερα

Consommation marchande et contraintes non monétaires au Canada ( )

Consommation marchande et contraintes non monétaires au Canada ( ) Consommation marchande et contraintes non monétaires au Canada (1969-2008) Julien Boelaert, François Gardes To cite this version: Julien Boelaert, François Gardes. Consommation marchande et contraintes

Διαβάστε περισσότερα

Solving an Air Conditioning System Problem in an Embodiment Design Context Using Constraint Satisfaction Techniques

Solving an Air Conditioning System Problem in an Embodiment Design Context Using Constraint Satisfaction Techniques Solving an Air Conditioning System Problem in an Embodiment Design Context Using Constraint Satisfaction Techniques Raphael Chenouard, Patrick Sébastian, Laurent Granvilliers To cite this version: Raphael

Διαβάστε περισσότερα

Modèles de représentation multi-résolution pour le rendu photo-réaliste de matériaux complexes

Modèles de représentation multi-résolution pour le rendu photo-réaliste de matériaux complexes Modèles de représentation multi-résolution pour le rendu photo-réaliste de matériaux complexes Jérôme Baril To cite this version: Jérôme Baril. Modèles de représentation multi-résolution pour le rendu

Διαβάστε περισσότερα

Forêts aléatoires : aspects théoriques, sélection de variables et applications

Forêts aléatoires : aspects théoriques, sélection de variables et applications Forêts aléatoires : aspects théoriques, sélection de variables et applications Robin Genuer To cite this version: Robin Genuer. Forêts aléatoires : aspects théoriques, sélection de variables et applications.

Διαβάστε περισσότερα

Transfert sécurisé d Images par combinaison de techniques de compression, cryptage et de marquage

Transfert sécurisé d Images par combinaison de techniques de compression, cryptage et de marquage Transfert sécurisé d Images par combinaison de techniques de compression, cryptage et de marquage José Marconi Rodrigues To cite this version: José Marconi Rodrigues. Transfert sécurisé d Images par combinaison

Διαβάστε περισσότερα

Vers un assistant à la preuve en langue naturelle

Vers un assistant à la preuve en langue naturelle Vers un assistant à la preuve en langue naturelle Thévenon Patrick To cite this version: Thévenon Patrick. Vers un assistant à la preuve en langue naturelle. Autre [cs.oh]. Université de Savoie, 2006.

Διαβάστε περισσότερα

Annulations de la dette extérieure et croissance. Une application au cas des pays pauvres très endettés (PPTE)

Annulations de la dette extérieure et croissance. Une application au cas des pays pauvres très endettés (PPTE) Annulations de la dette extérieure et croissance. Une application au cas des pays pauvres très endettés (PPTE) Khadija Idlemouden To cite this version: Khadija Idlemouden. Annulations de la dette extérieure

Διαβάστε περισσότερα

LEM. Non-linear externalities in firm localization. Giulio Bottazzi Ugo Gragnolati * Fabio Vanni

LEM. Non-linear externalities in firm localization. Giulio Bottazzi Ugo Gragnolati * Fabio Vanni LEM WORKING PAPER SERIES Non-linear externalities in firm localization Giulio Bottazzi Ugo Gragnolati * Fabio Vanni Institute of Economics, Scuola Superiore Sant'Anna, Pisa, Italy * University of Paris

Διαβάστε περισσότερα

UNIVERSITE DE PERPIGNAN VIA DOMITIA

UNIVERSITE DE PERPIGNAN VIA DOMITIA Délivré par UNIVERSITE DE PERPIGNAN VIA DOMITIA Préparée au sein de l école doctorale Energie et Environnement Et de l unité de recherche Procédés, Matériaux et Énergie Solaire (PROMES-CNRS, UPR 8521)

Διαβάστε περισσότερα

Contribution à l évolution des méthodologies de caractérisation et d amélioration des voies ferrées

Contribution à l évolution des méthodologies de caractérisation et d amélioration des voies ferrées Contribution à l évolution des méthodologies de caractérisation et d amélioration des voies ferrées Noureddine Rhayma To cite this version: Noureddine Rhayma. Contribution à l évolution des méthodologies

Διαβάστε περισσότερα

❷ s é 2s é í t é Pr 3

❷ s é 2s é í t é Pr 3 ❷ s é 2s é í t é Pr 3 t tr t á t r í í t 2 ➄ P á r í3 í str t s tr t r t r s 3 í rá P r t P P á í 2 rá í s é rá P r t P 3 é r 2 í r 3 t é str á 2 rá rt 3 3 t str 3 str ýr t ý í r t t2 str s í P á í t

Διαβάστε περισσότερα

Ax = b. 7x = 21. x = 21 7 = 3.

Ax = b. 7x = 21. x = 21 7 = 3. 3 s st 3 r 3 t r 3 3 t s st t 3t s 3 3 r 3 3 st t t r 3 s t t r r r t st t rr 3t r t 3 3 rt3 3 t 3 3 r st 3 t 3 tr 3 r t3 t 3 s st t Ax = b. s t 3 t 3 3 r r t n r A tr 3 rr t 3 t n ts b 3 t t r r t x 3

Διαβάστε περισσότερα

Langages dédiés au développement de services de communications

Langages dédiés au développement de services de communications Langages dédiés au développement de services de communications Nicolas Palix To cite this version: Nicolas Palix. Langages dédiés au développement de services de communications. Réseaux et télécommunications

Διαβάστε περισσότερα

Jeux d inondation dans les graphes

Jeux d inondation dans les graphes Jeux d inondation dans les graphes Aurélie Lagoutte To cite this version: Aurélie Lagoutte. Jeux d inondation dans les graphes. 2010. HAL Id: hal-00509488 https://hal.archives-ouvertes.fr/hal-00509488

Διαβάστε περισσότερα

ON THE MEASUREMENT OF

ON THE MEASUREMENT OF ON THE MEASUREMENT OF INVESTMENT TYPES: HETEROGENEITY IN CORPORATE TAX ELASTICITIES HENDRIK JUNGMANN, SIMON LORETZ WORKING PAPER NO. 2016-01 t s r t st t t2 s t r t2 r r t t 1 st t s r r t3 str t s r ts

Διαβάστε περισσότερα

Mesh Parameterization: Theory and Practice

Mesh Parameterization: Theory and Practice Mesh Parameterization: Theory and Practice Kai Hormann, Bruno Lévy, Alla Sheffer To cite this version: Kai Hormann, Bruno Lévy, Alla Sheffer. Mesh Parameterization: Theory and Practice. This document is

Διαβάστε περισσότερα

ss rt t r s t t t rs r ç s s rt t r t Pr r r q r ts P 2s s r r t t t t t st r t

ss rt t r s t t t rs r ç s s rt t r t Pr r r q r ts P 2s s r r t t t t t st r t Ô P ss rt t r s t t t rs r ç s s rt t r t Pr r r q r ts P 2s s r r t t t t t st r t FichaCatalografica :: Fichacatalografica https://www3.dti.ufv.br/bbt/ficha/cadastrarficha/visua... Ficha catalográfica

Διαβάστε περισσότερα

Network Neutrality Debate and ISP Inter-Relations: Traffi c Exchange, Revenue Sharing, and Disconnection Threat

Network Neutrality Debate and ISP Inter-Relations: Traffi c Exchange, Revenue Sharing, and Disconnection Threat Network Neutrality Debate and ISP Inter-Relations: Traffi c Exchange, Revenue Sharing, and Disconnection Threat Pierre Coucheney, Patrick Maillé, runo Tuffin To cite this version: Pierre Coucheney, Patrick

Διαβάστε περισσότερα

QBER DISCUSSION PAPER No. 8/2013. On Assortative and Disassortative Mixing in Scale-Free Networks: The Case of Interbank Credit Networks

QBER DISCUSSION PAPER No. 8/2013. On Assortative and Disassortative Mixing in Scale-Free Networks: The Case of Interbank Credit Networks QBER DISCUSSION PAPER No. 8/2013 On Assortative and Disassortative Mixing in Scale-Free Networks: The Case of Interbank Credit Networks Karl Finger, Daniel Fricke and Thomas Lux ss rt t s ss rt t 1 r t

Διαβάστε περισσότερα

Q π (/) ^ ^ ^ Η φ. <f) c>o. ^ ο. ö ê ω Q. Ο. o 'c. _o _) o U 03. ,,, ω ^ ^ -g'^ ο 0) f ο. Ε. ιη ο Φ. ο 0) κ. ο 03.,Ο. g 2< οο"" ο φ.

Q π (/) ^ ^ ^ Η φ. <f) c>o. ^ ο. ö ê ω Q. Ο. o 'c. _o _) o U 03. ,,, ω ^ ^ -g'^ ο 0) f ο. Ε. ιη ο Φ. ο 0) κ. ο 03.,Ο. g 2< οο ο φ. II 4»» «i p û»7'' s V -Ζ G -7 y 1 X s? ' (/) Ζ L. - =! i- Ζ ) Η f) " i L. Û - 1 1 Ι û ( - " - ' t - ' t/î " ι-8. Ι -. : wî ' j 1 Τ J en " il-' - - ö ê., t= ' -; '9 ',,, ) Τ '.,/,. - ϊζ L - (- - s.1 ai

Διαβάστε περισσότερα

Hygromécanique des panneaux en bois et conservation du patrimoine culturel. Des pathologies... aux outils pour la conservation

Hygromécanique des panneaux en bois et conservation du patrimoine culturel. Des pathologies... aux outils pour la conservation Hygromécanique des panneaux en bois et conservation du patrimoine culturel. Des pathologies... aux outils pour la conservation Bertrand Marcon To cite this version: Bertrand Marcon. Hygromécanique des

Διαβάστε περισσότερα

Analysis of a discrete element method and coupling with a compressible fluid flow method

Analysis of a discrete element method and coupling with a compressible fluid flow method Analysis of a discrete element method and coupling with a compressible fluid flow method Laurent Monasse To cite this version: Laurent Monasse. Analysis of a discrete element method and coupling with a

Διαβάστε περισσότερα

C 1 D 1. AB = a, AD = b, AA1 = c. a, b, c : (1) AC 1 ; : (1) AB + BC + CC1, AC 1 = BC = AD, CC1 = AA 1, AC 1 = a + b + c. (2) BD 1 = BD + DD 1,

C 1 D 1. AB = a, AD = b, AA1 = c. a, b, c : (1) AC 1 ; : (1) AB + BC + CC1, AC 1 = BC = AD, CC1 = AA 1, AC 1 = a + b + c. (2) BD 1 = BD + DD 1, 1 1., BD 1 B 1 1 D 1, E F B 1 D 1. B = a, D = b, 1 = c. a, b, c : (1) 1 ; () BD 1 ; () F; D 1 F 1 (4) EF. : (1) B = D, D c b 1 E a B 1 1 = 1, B1 1 = B + B + 1, 1 = a + b + c. () BD 1 = BD + DD 1, BD =

Διαβάστε περισσότερα

Résolution de problème inverse et propagation d incertitudes : application à la dynamique des gaz compressibles

Résolution de problème inverse et propagation d incertitudes : application à la dynamique des gaz compressibles Résolution de problème inverse et propagation d incertitudes : application à la dynamique des gaz compressibles Alexandre Birolleau To cite this version: Alexandre Birolleau. Résolution de problème inverse

Διαβάστε περισσότερα

A 1 A 2 A 3 B 1 B 2 B 3

A 1 A 2 A 3 B 1 B 2 B 3 16 0 17 0 17 0 18 0 18 0 19 0 20 A A = A 1 î + A 2 ĵ + A 3ˆk A (x, y, z) r = xî + yĵ + zˆk A B A B B A = A 1 B 1 + A 2 B 2 + A 3 B 3 = A B θ θ A B = ˆn A B θ A B î ĵ ˆk = A 1 A 2 A 3 B 1 B 2 B 3 W = F

Διαβάστε περισσότερα

P t s st t t t t2 t s st t t rt t t tt s t t ä ör tt r t r 2ö r t ts t t t t t t st t t t s r s s s t är ä t t t 2ö r t ts rt t t 2 r äärä t r s Pr r

P t s st t t t t2 t s st t t rt t t tt s t t ä ör tt r t r 2ö r t ts t t t t t t st t t t s r s s s t är ä t t t 2ö r t ts rt t t 2 r äärä t r s Pr r r s s s t t P t s st t t t t2 t s st t t rt t t tt s t t ä ör tt r t r 2ö r t ts t t t t t t st t t t s r s s s t är ä t t t 2ö r t ts rt t t 2 r äärä t r s Pr r t t s st ä r t str t st t tt2 t s s t st

Διαβάστε περισσότερα

Conditions aux bords dans des theories conformes non unitaires

Conditions aux bords dans des theories conformes non unitaires Conditions aux bords dans des theories conformes non unitaires Jerome Dubail To cite this version: Jerome Dubail. Conditions aux bords dans des theories conformes non unitaires. Physique mathématique [math-ph].

Διαβάστε περισσότερα

La naissance de la cohomologie des groupes

La naissance de la cohomologie des groupes La naissance de la cohomologie des groupes Nicolas Basbois To cite this version: Nicolas Basbois. La naissance de la cohomologie des groupes. Mathématiques [math]. Université Nice Sophia Antipolis, 2009.

Διαβάστε περισσότερα

Coupling strategies for compressible - low Mach number flows

Coupling strategies for compressible - low Mach number flows Coupling strategies for compressible - low Mach number flows Yohan Penel, Stéphane Dellacherie, Bruno Després To cite this version: Yohan Penel, Stéphane Dellacherie, Bruno Després. Coupling strategies

Διαβάστε περισσότερα

Pathological synchronization in neuronal populations : a control theoretic perspective

Pathological synchronization in neuronal populations : a control theoretic perspective Pathological synchronization in neuronal populations : a control theoretic perspective Alessio Franci To cite this version: Alessio Franci. Pathological synchronization in neuronal populations : a control

Διαβάστε περισσότερα

A hybrid PSTD/DG method to solve the linearized Euler equations

A hybrid PSTD/DG method to solve the linearized Euler equations A hybrid PSTD/ method to solve the linearized Euler equations ú P á ñ 3 rt r 1 rt t t t r t rs t2 2 t r s r2 r r Ps s tr r r P t s s t t 2 r t r r P s s r r 2s s s2 t s s t t t s t r t s t r q t r r t

Διαβάστε περισσότερα

Note: Please use the actual date you accessed this material in your citation.

Note: Please use the actual date you accessed this material in your citation. MIT OpenCourseWare http://ocw.mit.edu 6.03/ESD.03J Electromagnetics and Applications, Fall 005 Please use the following citation format: Markus Zahn, 6.03/ESD.03J Electromagnetics and Applications, Fall

Διαβάστε περισσότερα

ITU-R P (2009/10)

ITU-R P (2009/10) ITU-R.45-4 (9/) % # GHz,!"# $$ # ITU-R.45-4.. (IR) (ITU-T/ITU-R/ISO/IEC).ITU-R http://www.tu.t/itu-r/go/patets/e. (http://www.tu.t/publ/r-rec/e ) () ( ) BO BR BS BT F M RA S RS SA SF SM SNG TF V.ITU-R

Διαβάστε περισσότερα

ITU-R P (2012/02) khz 150

ITU-R P (2012/02) khz 150 (0/0) khz 0 P ii (IPR) (ITU-T/ITU-R/ISO/IEC) ITU-R http://www.itu.int/itu-r/go/patents/en http://www.itu.int/publ/r-rec/en BO BR BS BT F M P RA RS S SA SF SM SNG TF V ITU-R 0 ITU 0 (ITU) khz 0 (0-009-00-003-00-994-990)

Διαβάστε περισσότερα

Logique et Interaction : une Étude Sémantique de la

Logique et Interaction : une Étude Sémantique de la Logique et Interaction : une Étude Sémantique de la Totalité Pierre Clairambault To cite this version: Pierre Clairambault. Logique et Interaction : une Étude Sémantique de la Totalité. Autre [cs.oh].

Διαβάστε περισσότερα

Profiterole : un protocole de partage équitable de la bande passante dans les réseaux ad hoc

Profiterole : un protocole de partage équitable de la bande passante dans les réseaux ad hoc Profiterole : un protocole de partage équitable de la bande passante dans les réseaux ad hoc Rémi Vannier To cite this version: Rémi Vannier. Profiterole : un protocole de partage équitable de la bande

Διαβάστε περισσότερα

m i N 1 F i = j i F ij + F x

m i N 1 F i = j i F ij + F x N m i i = 1,..., N m i Fi x N 1 F ij, j = 1, 2,... i 1, i + 1,..., N m i F i = j i F ij + F x i mi Fi j Fj i mj O P i = F i = j i F ij + F x i, i = 1,..., N P = i F i = N F ij + i j i N i F x i, i = 1,...,

Διαβάστε περισσότερα

Points de torsion des courbes elliptiques et équations diophantiennes

Points de torsion des courbes elliptiques et équations diophantiennes Points de torsion des courbes elliptiques et équations diophantiennes Nicolas Billerey To cite this version: Nicolas Billerey. Points de torsion des courbes elliptiques et équations diophantiennes. Mathématiques

Διαβάστε περισσότερα

Three essays on trade and transfers: country heterogeneity, preferential treatment and habit formation

Three essays on trade and transfers: country heterogeneity, preferential treatment and habit formation Three essays on trade and transfers: country heterogeneity, preferential treatment and habit formation Jean-Marc Malambwe Kilolo To cite this version: Jean-Marc Malambwe Kilolo. Three essays on trade and

Διαβάστε περισσότερα

Łs t r t rs tø r P r s tø PrØ rø rs tø P r s r t t r s t Ø t q s P r s tr. 2stŁ s q t q s t rt r s t s t ss s Ø r s t r t. Łs t r t t Ø t q s

Łs t r t rs tø r P r s tø PrØ rø rs tø P r s r t t r s t Ø t q s P r s tr. 2stŁ s q t q s t rt r s t s t ss s Ø r s t r t. Łs t r t t Ø t q s Łs t r t rs tø r P r s tø PrØ rø rs tø P r s r t t r s t Ø t q s P r s tr st t t t Ø t q s ss P r s P 2stŁ s q t q s t rt r s t s t ss s Ø r s t r t P r røs r Łs t r t t Ø t q s r Ø r t t r t q t rs tø

Διαβάστε περισσότερα

! " # $ % & $ % & $ & # " ' $ ( $ ) * ) * +, -. / # $ $ ( $ " $ $ $ % $ $ ' ƒ " " ' %. " 0 1 2 3 4 5 6 7 8 9 : ; ; < = : ; > : 0? @ 8? 4 A 1 4 B 3 C 8? D C B? E F 4 5 8 3 G @ H I@ A 1 4 D G 8 5 1 @ J C

Διαβάστε περισσότερα

Déformation et quantification par groupoïde des variétés toriques

Déformation et quantification par groupoïde des variétés toriques Défomation et uantification pa goupoïde de vaiété toiue Fédéic Cadet To cite thi veion: Fédéic Cadet. Défomation et uantification pa goupoïde de vaiété toiue. Mathématiue [math]. Univeité d Oléan, 200.

Διαβάστε περισσότερα

Measurement-driven mobile data traffic modeling in a large metropolitan area

Measurement-driven mobile data traffic modeling in a large metropolitan area Measurement-driven mobile data traffic modeling in a large metropolitan area Eduardo Mucelli Rezende Oliveira, Aline Carneiro Viana, Kolar Purushothama Naveen, Carlos Sarraute To cite this version: Eduardo

Διαβάστε περισσότερα

Traitement STAP en environnement hétérogène. Application à la détection radar et implémentation sur GPU

Traitement STAP en environnement hétérogène. Application à la détection radar et implémentation sur GPU Traitement STAP en environnement hétérogène. Application à la détection radar et implémentation sur GPU Jean-François Degurse To cite this version: Jean-François Degurse. Traitement STAP en environnement

Διαβάστε περισσότερα

Stéphane Bancelin. Imagerie Quantitative du Collagène par Génération de Seconde Harmonique.

Stéphane Bancelin. Imagerie Quantitative du Collagène par Génération de Seconde Harmonique. Imagerie Quantitative du Collagène par Génération de Seconde Harmonique Stéphane Bancelin To cite this version: Stéphane Bancelin. Imagerie Quantitative du Collagène par Génération de Seconde Harmonique.

Διαβάστε περισσότερα

Pierre Grandemange. To cite this version: HAL Id: tel https://tel.archives-ouvertes.fr/tel

Pierre Grandemange. To cite this version: HAL Id: tel https://tel.archives-ouvertes.fr/tel Piégeage et accumulation de positons issus d un faisceau pulsé produit par un accélérateur pour l étude de l interaction gravitationnelle de l antimatière Pierre Grandemange To cite this version: Pierre

Διαβάστε περισσότερα

Ó³ Ÿ , º 6(155).. 805Ä813 ˆ ˆŠ ˆ ˆŠ Š ˆ. ˆ.. ³ Ì μ, ƒ.. Š ³ÒÏ, ˆ.. Š Ö. Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê. Ÿ. ʲ ±μ ±

Ó³ Ÿ , º 6(155).. 805Ä813 ˆ ˆŠ ˆ ˆŠ Š ˆ. ˆ.. ³ Ì μ, ƒ.. Š ³ÒÏ, ˆ.. Š Ö. Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê. Ÿ. ʲ ±μ ± Ó³ Ÿ. 2009.. 6, º 6(155).. 805Ä813 ˆ ˆŠ ˆ ˆŠ Š ˆ Œ ˆ ˆ Œ ˆŒ ˆ ˆ ˆ ˆ ˆ Ÿ Œ ƒ ˆ ˆŠ ˆ.. ³ Ì μ, ƒ.. Š ³ÒÏ, ˆ.. Š Ö Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê Ÿ. ʲ ±μ ± ˆ É ÉÊÉ Ö μ Ë ± μ²ó ±μ ± ³ ʱ, Š ±μ, μ²óï Œ É ³ É Î ±μ ±μ³

Διαβάστε περισσότερα

Interaction hydrodynamique entre deux vésicules dans un cisaillement simple

Interaction hydrodynamique entre deux vésicules dans un cisaillement simple Interaction hydrodynamique entre deux vésicules dans un cisaillement simple Pierre-Yves Gires To cite this version: Pierre-Yves Gires. Interaction hydrodynamique entre deux vésicules dans un cisaillement

Διαβάστε περισσότερα

Solutions - Chapter 4

Solutions - Chapter 4 Solutions - Chapter Kevin S. Huang Problem.1 Unitary: Ût = 1 ī hĥt Û tût = 1 Neglect t term: 1 + hĥ ī t 1 īhĥt = 1 + hĥ ī t ī hĥt = 1 Ĥ = Ĥ Problem. Ût = lim 1 ī ] n hĥ1t 1 ī ] hĥt... 1 ī ] hĥnt 1 ī ]

Διαβάστε περισσότερα

Développement d un nouveau multi-détecteur de neutrons

Développement d un nouveau multi-détecteur de neutrons Développement d un nouveau multi-détecteur de neutrons M. Sénoville To cite this version: M. Sénoville. Développement d un nouveau multi-détecteur de neutrons. Physique Nucléaire Expérimentale [nucl-ex].

Διαβάστε περισσότερα

ECE Spring Prof. David R. Jackson ECE Dept. Notes 2

ECE Spring Prof. David R. Jackson ECE Dept. Notes 2 ECE 634 Spring 6 Prof. David R. Jackson ECE Dept. Notes Fields in a Source-Free Region Example: Radiation from an aperture y PEC E t x Aperture Assume the following choice of vector potentials: A F = =

Διαβάστε περισσότερα

Segmentation d IRM cérébrales multidimensionnelles par coupe de graphe

Segmentation d IRM cérébrales multidimensionnelles par coupe de graphe Segmentation d IRM cérébrales multidimensionnelles par coupe de graphe Jérémy Lecoeur To cite this version: Jérémy Lecoeur. Segmentation d IRM cérébrales multidimensionnelles par coupe de graphe. Informatique

Διαβάστε περισσότερα

Bandwidth mismatch calibration in time-interleaved analog-to-digital converters

Bandwidth mismatch calibration in time-interleaved analog-to-digital converters Bandwidth mismatch calibration in time-interleaved analog-to-digital converters Fatima Ghanem To cite this version: Fatima Ghanem. Bandwidth mismatch calibration in time-interleaved analog-to-digital converters.

Διαβάστε περισσότερα

Voice over IP Vulnerability Assessment

Voice over IP Vulnerability Assessment Voice over IP Vulnerability Assessment Humberto Abdelnur To cite this version: Humberto Abdelnur. Voice over IP Vulnerability Assessment. Networking and Internet Architecture [cs.ni]. Université Henri

Διαβάστε περισσότερα

m r = F m r = F ( r) m r = F ( v) F = F (x) m dv dt = F (x) vdv = F (x)dx d dt = dx dv dt dx = v dv dx

m r = F m r = F ( r) m r = F ( v) F = F (x) m dv dt = F (x) vdv = F (x)dx d dt = dx dv dt dx = v dv dx m r = F m r = F ( r) m r = F ( v) x F = F (x) m dv dt = F (x) d dt = dx dv dt dx = v dv dx vdv = F (x)dx 2 mv2 x 2 mv2 0 = F (x )dx x 0 K = 2 mv2 W x0 x = x x 0 F (x)dx K K 0 = W x0 x x, x 2 x K 2 K =

Διαβάστε περισσότερα

Development and Verification of Multi-Level Sub- Meshing Techniques of PEEC to Model High- Speed Power and Ground Plane-Pairs of PFBS

Development and Verification of Multi-Level Sub- Meshing Techniques of PEEC to Model High- Speed Power and Ground Plane-Pairs of PFBS Rose-Hulman Institute of Technology Rose-Hulman Scholar Graduate Theses - Electrical and Computer Engineering Graduate Theses Spring 5-2015 Development and Verification of Multi-Level Sub- Meshing Techniques

Διαβάστε περισσότερα

Το άτομο του Υδρογόνου

Το άτομο του Υδρογόνου Το άτομο του Υδρογόνου Δυναμικό Coulomb Εξίσωση Schrödinger h e (, r, ) (, r, ) E (, r, ) m ψ θφ r ψ θφ = ψ θφ Συνθήκες ψ(, r θφ, ) = πεπερασμένη ψ( r ) = 0 ψ(, r θφ, ) =ψ(, r θφ+, ) π Επιτρεπτές ενέργειες

Διαβάστε περισσότερα

Œˆ ˆ ƒ ˆŸ Ÿ ˆ ˆ Ÿ Œˆ ˆ

Œˆ ˆ ƒ ˆŸ Ÿ ˆ ˆ Ÿ Œˆ ˆ Ó³ Ÿ. 2017.. 14, º 1(206).. 176Ä189 ˆ ˆŠ ˆ ˆŠ Š ˆ Œˆ ˆ ƒ ˆŸ Ÿ ˆ ˆ Ÿ Œˆ ˆ.. Š μ,. ˆ. Š Î 1 Ñ Ò É ÉÊÉ Ö ÒÌ ² μ, Ê μé ³ É É Ö μ²êî μ μ μ μ μ ² Ö Êα ÉÖ ²ÒÌ μ μ ÊÐ Ö ³ Ï μ³μðóõ ± μ Ö Êα μ μ Ì μ É. ± μ μ ÊÐ

Διαβάστε περισσότερα

ITU-R P (2012/02) &' (

ITU-R P (2012/02) &' ( ITU-R P.530-4 (0/0) $ % " "#! &' ( P ITU-R P. 530-4 ii.. (IPR) (ITU-T/ITU-R/ISO/IEC).ITU-R http://www.itu.int/itu-r/go/patents/en. ITU-T/ITU-R/ISO/IEC (http://www.itu.int/publ/r-rec/en ) () ( ) BO BR BS

Διαβάστε περισσότερα

ts s ts tr s t tr r n s s q t r t rs d n i : X n X n 1 r n 1 0 i n s t s 2 d n i dn+1 j = d n j dn+1 i+1 r 2 s s s s ts

ts s ts tr s t tr r n s s q t r t rs d n i : X n X n 1 r n 1 0 i n s t s 2 d n i dn+1 j = d n j dn+1 i+1 r 2 s s s s ts r s r t r t t tr t t 2 t2 str t s s t2 s r PP rs t P r s r t r2 s r r s ts t 2 t2 str t s s s ts t2 t r2 r s ts r t t t2 s s r ss s q st r s t t s 2 r t t s t t st t t t 2 tr t s s s t r t s t s 2 s ts

Διαβάστε περισσότερα

Fusion de données multicapteurs pour la construction incrémentale du modèle tridimensionnel texturé d un environnement intérieur par un robot mobile

Fusion de données multicapteurs pour la construction incrémentale du modèle tridimensionnel texturé d un environnement intérieur par un robot mobile Fusion de données multicapteurs pour la construction incrémentale du modèle tridimensionnel texturé d un environnement intérieur par un robot mobile Ayman Zureiki To cite this version: Ayman Zureiki. Fusion

Διαβάστε περισσότερα

ΓΗ ΚΑΙ ΣΥΜΠΑΝ. Εικόνα 1. Φωτογραφία του γαλαξία μας (από αρχείο της NASA)

ΓΗ ΚΑΙ ΣΥΜΠΑΝ. Εικόνα 1. Φωτογραφία του γαλαξία μας (από αρχείο της NASA) ΓΗ ΚΑΙ ΣΥΜΠΑΝ Φύση του σύμπαντος Η γη είναι μία μονάδα μέσα στο ηλιακό μας σύστημα, το οποίο αποτελείται από τον ήλιο, τους πλανήτες μαζί με τους δορυφόρους τους, τους κομήτες, τα αστεροειδή και τους μετεωρίτες.

Διαβάστε περισσότερα

Aboa Centre for Economics. Discussion paper No. 122 Turku 2018

Aboa Centre for Economics. Discussion paper No. 122 Turku 2018 Joonas Ollonqvist Accounting for the role of tax-benefit changes in shaping income inequality: A new method, with application to income inequality in Finland Aboa Centre for Economics Discussion paper

Διαβάστε περισσότερα

#%" )*& ##+," $ -,!./" %#/%0! %,!

#% )*& ##+, $ -,!./ %#/%0! %,! -!"#$% -&!'"$ & #("$$, #%" )*& ##+," $ -,!./" %#/%0! %,! %!$"#" %!#0&!/" /+#0& 0.00.04. - 3 3,43 5 -, 4 $ $.. 04 ... 3. 6... 6.. #3 7 8... 6.. %9: 3 3 7....3. % 44 8... 6.4. 37; 3,, 443 8... 8.5. $; 3

Διαβάστε περισσότερα

ITU-R P (2009/10)

ITU-R P (2009/10) ITU-R.38-6 (009/0 $% #! " #( ' * & ' /0,-. # GHz 00 MHz 900 ITU-R.38-6 ii.. (IR (ITU-T/ITU-R/ISO/IEC.ITU-R http://www.itu.int/itu-r/go/patents/en. (http://www.itu.int/publ/r-rec/en ( ( BO BR BS BT F M

Διαβάστε περισσότερα

Analyse de modèles pour ITER ; Traitement des conditions aux limites de systèmes modélisant le plasma de bord dans un tokamak

Analyse de modèles pour ITER ; Traitement des conditions aux limites de systèmes modélisant le plasma de bord dans un tokamak Analyse de modèles pour ITER ; Traitement des conditions aux limites de systèmes modélisant le plasma de bord dans un tokamak Thomas Auphan To cite this version: Thomas Auphan. Analyse de modèles pour

Διαβάστε περισσότερα

Defects in Hard-Sphere Colloidal Crystals

Defects in Hard-Sphere Colloidal Crystals Defects in Hard-Sphere Colloidal Crystals The Harvard community has made this article openly available. Please share how this access benefits you. Your story matters. Citation Accessed Citable Link Terms

Διαβάστε περισσότερα

Prés té r t r P Ô P P é té r t q r t t r2 t r t r t q s t r s t s t t s à t té rt rs r r ss r s rs tés r r ss r s rs tés 1 1 t rs r st r ss r s rs tés P r s 13 è îtr ér s r P rr îtr ér s rt r îtr ér s

Διαβάστε περισσότερα

Š ˆ œ Ÿ ˆ œ Œ Œ ƒ ˆ Œ Œ LEPTA

Š ˆ œ Ÿ ˆ œ Œ Œ ƒ ˆ Œ Œ LEPTA Ó³ Ÿ. 2006.. 3, º 7(136).. 78Ä83 Š 537.533.33, 621.384.60-833 Š ˆ œ Ÿ ˆ œ Œ Œ ƒ ˆ Œ Œ LEPTA ( ).. μ²éêï±,.. Ò±μ ±,. ƒ. Šμ Í,.. Šμ μé,. ˆ. μì³ Éμ,.. Œ ² Ìμ, ˆ.. Œ ϱμ,.. ²μ,.., ˆ.. ²,.. μ,.. ³ μ,. Œ. Ò,

Διαβάστε περισσότερα

AVERTISSEMENT. D'autre part, toute contrefaçon, plagiat, reproduction encourt une poursuite pénale. LIENS

AVERTISSEMENT. D'autre part, toute contrefaçon, plagiat, reproduction encourt une poursuite pénale. LIENS AVERTISSEMENT Ce document est le fruit d'un long travail approuvé par le jury de soutenance et mis à disposition de l'ensemble de la communauté universitaire élargie. Il est soumis à la propriété intellectuelle

Διαβάστε περισσότερα

Mohamed-Salem Louly. To cite this version: HAL Id: tel https://tel.archives-ouvertes.fr/tel

Mohamed-Salem Louly. To cite this version: HAL Id: tel https://tel.archives-ouvertes.fr/tel Deux modèles matématiques de l évolution d un bassin sédimentaire. Pénomènes d érosion-sédimentation-transport en géologie. Application en prospection pétrolière Moamed-Salem Louly To cite tis version:

Διαβάστε περισσότερα

Problem 7.19 Ignoring reflection at the air soil boundary, if the amplitude of a 3-GHz incident wave is 10 V/m at the surface of a wet soil medium, at what depth will it be down to 1 mv/m? Wet soil is

Διαβάστε περισσότερα

ο ο 3 α. 3"* > ω > d καΐ 'Ενορία όλις ή Χώρί ^ 3 < KN < ^ < 13 > ο_ Μ ^~~ > > > > > Ο to X Η > ο_ ο Ο,2 Σχέδι Γλεγμα Ο Σ Ο Ζ < o w *< Χ χ Χ Χ < < < Ο

ο ο 3 α. 3* > ω > d καΐ 'Ενορία όλις ή Χώρί ^ 3 < KN < ^ < 13 > ο_ Μ ^~~ > > > > > Ο to X Η > ο_ ο Ο,2 Σχέδι Γλεγμα Ο Σ Ο Ζ < o w *< Χ χ Χ Χ < < < Ο 18 ρ * -sf. NO 1 D... 1: - ( ΰ ΐ - ι- *- 2 - UN _ ί=. r t ' \0 y «. _,2. "* co Ι». =; F S " 5 D 0 g H ', ( co* 5. «ΰ ' δ". o θ * * "ΰ 2 Ι o * "- 1 W co o -o1= to»g ι. *ΰ * Ε fc ΰ Ι.. L j to. Ι Q_ " 'T

Διαβάστε περισσότερα

m 1, m 2 F 12, F 21 F12 = F 21

m 1, m 2 F 12, F 21 F12 = F 21 m 1, m 2 F 12, F 21 F12 = F 21 r 1, r 2 r = r 1 r 2 = r 1 r 2 ê r = rê r F 12 = f(r)ê r F 21 = f(r)ê r f(r) f(r) < 0 f(r) > 0 m 1 r1 = f(r)ê r m 2 r2 = f(r)ê r r = r 1 r 2 r 1 = 1 m 1 f(r)ê r r 2 = 1 m

Διαβάστε περισσότερα

Une Théorie des Constructions Inductives

Une Théorie des Constructions Inductives Une Théorie des Constructions Inductives Benjamin Werner To cite this version: Benjamin Werner. Une Théorie des Constructions Inductives. Génie logiciel [cs.se]. Université Paris- Diderot - Paris VII,

Διαβάστε περισσότερα

www.absolualarme.com met la disposition du public, via www.docalarme.com, de la documentation technique dont les rιfιrences, marques et logos, sont

www.absolualarme.com met la disposition du public, via www.docalarme.com, de la documentation technique dont les rιfιrences, marques et logos, sont w. ww lua so ab me lar m.co t me la sit po dis ion du c, bli pu via lar ca do w. ww me.co m, de la ion nta t do cu me on t ed hn iqu tec les en ce s, rι fιr ma rq ue se t lo go s, so nt la pr op riι tι

Διαβάστε περισσότερα

10-π-electron arenes à la carte: Structure. Sr, Ba; n = 6-8) complexes

10-π-electron arenes à la carte: Structure. Sr, Ba; n = 6-8) complexes Electronic Supplementary Material (ESI) for Physical Chemistry Chemical Physics. This journal is the Owner Societies 2016 Supporting information 10-π-electron arenes à la carte: Structure and Bonding of

Διαβάστε περισσότερα

d 2 y dt 2 xdy dt + d2 x

d 2 y dt 2 xdy dt + d2 x y t t ysin y d y + d y y t z + y ty yz yz t z y + t + y + y + t y + t + y + + 4 y 4 + t t + 5 t Ae cos + Be sin 5t + 7 5 y + t / m_nadjafikhah@iustacir http://webpagesiustacir/m_nadjafikhah/courses/ode/fa5pdf

Διαβάστε περισσότερα

Agujeros negros de masa intermedia: efectos sobre su entorno y detectabilidad Pepe, Carolina 2013

Agujeros negros de masa intermedia: efectos sobre su entorno y detectabilidad Pepe, Carolina 2013 Agujeros negros de masa intermedia: efectos sobre su entorno y detectabilidad Pepe, Carolina 2013 Tesis Doctoral Facultad de Ciencias Exactas y Naturales Universidad de Buenos Aires www.digital.bl.fcen.uba.ar

Διαβάστε περισσότερα

VISCOUS FLUID FLOWS Mechanical Engineering

VISCOUS FLUID FLOWS Mechanical Engineering NEER ENGI STRUCTURE PRESERVING FORMULATION OF HIGH VISCOUS FLUID FLOWS Mechanical Engineering Technical Report ME-TR-9 grad curl div constitutive div curl grad DATA SHEET Titel: Structure preserving formulation

Διαβάστε περισσότερα