|
|
- Πάνθηρας Βασιλειάδης
- 6 χρόνια πριν
- Προβολές:
Transcript
1
2
3
4
5
6
7
8
9
10
11
12
13
14
15
16
17
18
19 Prblma dl smipian Cas i cs ω µ Cas sin cs i cs
20 Cas fas [ ] [ ] ] [ ttal S S J L J J L A d I I A d I d I V d d V V d d V n J n J ˆ 0 ˆ ˆ ˆ 0 ˆ 0 ˆ ˆ ˆ 0 S S S S i i Z sin
21 ω µ V V Z I I A V Z V Z I V Z V Z I c c c c c quain W- mgna in frma nn cannica rnl ω µ V A S 0 0 < < A nn standard 0 < < V S nn standard
22 0 0 < < d g d S g S s A A A J J J 0 0 sin 0 0 cs g s g s J Z J g Z d Z A cs sin sin 0 cs d V A ω µ cs sin
23 d V A ω µ cs sin fas: afattriain d V A ω µ cs sin cs cs sin sin cs cs sin cs sin bdcmpsiin
24 0 cs sin cs sin sin ω µ w V A d csparain dll piu dll mn cs d Sluin A ω µ V i A V V ω µ sign A I I i
25 3 fas. Discussin sign d i ω µ i i Z sin sin cs } cs cs { cs cs 4 i F F d Fu: funin di Frsnl
26 Andamnt vicin l spigl: / A J S / divrg
27 Dcmpsiin in camp gmtric camp scattrrat s g s g D u u >> cs cs sin sin 4 / 4 / cs cs
28
29
30
31 ω ε d A V V divrg i i s / 0 } cs cs { cs cs 4 F F
32 J S / 0 0 pr 0
33 Dcmpsiin in camp gmtric camp scattrrat s g s g D u u >> cs cs sin sin 4 / 4 / cs cs
34 Dcmpsiin in camp gmtric camp scattrrat s g s g D u u >> cs cs cs cs 4 / 4 / cs cs
35 Far fild prsnt in a hmgnus angular rgin Th surc fild is cnstitutd b a plan wav having th fllwing lngitudinal cmpnnts:. i cs } i cs whr b indicating with β and th nithal and aimuthal angl f th dirctin f th plan wav nˆ i it is: ω µ ε cs β sin β. In an arbitrar hmgnus angular rgin s fr ampl fig. th lngitudinal cmpnnts f an lctrmagntic fild ar prssd b th Smmrfld rprsntatin:..3 s [ w ] c c s [ w ] c c cs[ w ] cs[ w ] dw dw
36 whr C and C cnstituts th Smmrfld cntur and s w and s w Smmrfld functins rlvant t th lngitudinal filds and : W cnsidr nl tim harmnic lctrmagntic filds with a tim dpndnc spcifid t b th factr ω which is mittd. Lt s cnsidr a hmgnus angular rgin. Withut lss f gnralit w intrduc a plar sstm f crdinats whr th dirctin 0 blngs t this rgin. fig. hmgnus angular rgin. In gnral in this rgin thr is th prsnc f all th cmpnnts and fr th ttal fild th factr is mittd. Th Winr-pf tchniqu fr wdg prblms is basd n th intrductin f th fllwing Laplac transfrms:.4 η η V d I η η d 0 0 η η.5 V η d I η d 0 0 Lt s us supps t nw th fllwing Laplac transfrm rlvant t th tangntial cmpnnts f th lctrmagntic fild n th dirctin 0 Lt s us supps t nw th fllwing Laplac transfrm rlvant t th tangntial cmpnnts f th lctrmagntic fild n th dirctin η V η d 0 0 V 0 0 η η d 0 0 η I η d 0 0 I 0 0 η η d
37 B putting.8 η cs w.9 η sin w w hav th fllwing prssins f th Smmrfld functins rlvant t th lngitudinal filds and :.0 cs w s w sin wv cs w0 I cs w0 I cs w0 ω ε ω ε. cs w s w sin wi cs w0 V cs w0 V cs w0 ω µ ω µ Th Smmrfld functins prvid th diffractd filds prsnt in th angular rgin: 4 d. [ s s ] d.3 [ s s ] 4 An ampl: Diffractin b a prfctl cnducting half-plan b an incidnt plan wav Figur : Gmtr f th prblm sw angl β
38 Fr th sa f simplicit w will cnsidr nl th cas whr th wdg rduc t a half-plan Φ fig. PC half-plan prblm B indicating with.4 t ˆ ˆ t ˆ ˆ lt s intrduc th bilatral Laplac transfrms: V ˆ t d.5 I d t Frm th thr f th stratifid mdia w hav:.6 V 0 Z I 0 c.7 V 0 Z c I 0
39 O.8 Zc P ωεξ ξ whr: O O ξ ξ O O O P plnmial matri ωε B rprsnting th filds in.4 and.5 in plar crdinats and taing int accunt th dfinitins. and.3 ilds th Winr-pf quatins:.9.0 ξ V 0 I 0 I 0 ωε ωε I I ωε ωε ξ I 0 V 0 V 0 ωµ ωµ ξ I. ξ V 0 I 0 I 0 ωε ωε I I ωε ωε. η ξ I 0 V 0 V 0 ωµ ωµ ξ I Th sstm dcupls in fur indpndnt W- quatins b summing and subtracting
40 quatins.7 and.9 and b summing and subtracting quatins.8 and.0. It ilds:.3 ξ V 0 I I I I ωε ωε.4 I 0 I 0 ωε ωε I I I I ωε ωε.5 I 0 I I.6 V 0 V 0 I I ξ ωµ ωµ In th fur uncupld W- quatins th plus functins ar V 0 I 0 I 0 I 0 and V 0 V 0 ωε ωε ωµ ωµ and th minus functins ar: I I I I I I and I I W cnsidr as surc th gmtrical ptic cntributin n th half plan. Taing int accunt that th in th cas f fig. th fac is nt illuminatd w hav:.7 whr: g g Z cs sin I ± I I Z g g g I ± I I cs p Th nl rquird factriatin is that f th scalar: p p
41 .8 ξ Th slutin f th fur W- quatins can b dn immdiatl and it ilds in th w- plan th slutin Φ : cs sin Φ Φ.9 V cs w0 Φsin w cs w cs Φ Φ.30 V cs w0 cs ct wct βsin w Zcs w csc βsin Φ Φ Φ Φ Φ cs w cs Φ Φ sin w Φ.3 I cs w0 Φsin w cs w cs Φ Φ I cs w0.3 Z ct wct β sin w csc βsin Φ Φ ZΦ cs w cs Φ Φ Substituting in.8 and.9 ild th Smmrfld functins:.33 s 55 cs Φ w Φ sin w sin Φ Φ
42 .34 s cs w Φ w Φ sin w sin Φ Φ Substituting in.0 and. ilds th lngitudinal diffractd filds: cs cs d cs cs 4 sin sin d cs cs quatins.33 and.34 hld fr arbitrar valu f < < Th diffractd ras cnstituts a gnratri f th Kllr cn and it is dfind b th angular sphrical crdinats β and fig.. Taing int accunt that th incidnt fild has angular sphrical crdinats β and it is cnvnint t rlat th transvrsal d d cmpnnt β f th diffractd ra t th transvrsal cmpnnt i i β f th incidnt ra. B gmtrical cnsidratin w hav : d d d d β Z.37 sin β sin β.38 i sin β i β i Z sin β i Th prvius quatins cannt b usd whn th bsrvatin pint apprachs shadw bundaris f th incidnt and th rflctd wavs.
43
Homework #6. A circular cylinder of radius R rotates about the long axis with angular velocity
Homwork #6 1. (Kittl 5.1) Cntrifug. A circular cylindr of radius R rotats about th long axis with angular vlocity ω. Th cylindr contains an idal gas of atoms of mass m at tmpratur. Find an xprssion for
2 2 2 The correct formula for the cosine of the sum of two angles is given by the following theorem.
5 TRIGONOMETRIC FORMULAS FOR SUMS AND DIFFERENCES The fundamental trignmetric identities cnsidered earlier express relatinships amng trignmetric functins f a single variable In this sectin we develp trignmetric
2 2 2 The correct formula for the cosine of the sum of two angles is given by the following theorem.
5 TRIGONOMETRIC FORMULAS FOR SUMS AND DIFFERENCES The fundamental trignmetric identities cnsidered earlier express relatinships amng trignmetric functins f a single variable In this sectin we develp trignmetric
General theorems of Optical Imaging systems
Gnral thorms of Optcal Imagng sstms Tratonal Optcal Imagng Topcs Imagng qualt harp: mags a pont sourc to a pont Dstorton fr: mags a shap to a smlar shap tgmatc Imagng Imags a pont sourc to a nfntl sharp
Pairs of Random Variables
Pairs of Random Variabls Rading: Chaptr 4. 4. Homwork: (do at last 5 out of th following problms 4..4, 4..6, 4.., 4.3.4, 4.3.5, 4.4., 4.4.4, 4.5.3, 4.6.3, 4.6.7, 4.6., 4.7.9, 4.7., 4.8.3, 4.8.7, 4.9.,
Calculus and Differential Equations page 1 of 17 CALCULUS and DIFFERENTIAL EQUATIONS
alculus and Diffrnial Equaions pag of 7 ALULUS and DIFFERENTIAL EQUATIONS Th following 55 qusions concrn calculus and diffrnial quaions. In his vrsion of h am, h firs choic is always h corrc on. In h acual
SOLUTIONS & ANSWERS FOR KERALA ENGINEERING ENTRANCE EXAMINATION-2018 PAPER II VERSION B1
SOLUTIONS & ANSWERS FOR KERALA ENGINEERING ENTRANCE EXAMINATION-8 PAPER II VERSION B [MATHEMATICS]. Ans: ( i) It is (cs5 isin5 ) ( i). Ans: i z. Ans: i i i The epressin ( i) ( ). Ans: cs i sin cs i sin
Π Ο Λ Ι Τ Ι Κ Α Κ Α Ι Σ Τ Ρ Α Τ Ι Ω Τ Ι Κ Α Γ Ε Γ Ο Ν Ο Τ Α
Α Ρ Χ Α Ι Α Ι Σ Τ Ο Ρ Ι Α Π Ο Λ Ι Τ Ι Κ Α Κ Α Ι Σ Τ Ρ Α Τ Ι Ω Τ Ι Κ Α Γ Ε Γ Ο Ν Ο Τ Α Σ η µ ε ί ω σ η : σ υ ν ά δ ε λ φ ο ι, ν α µ ο υ σ υ γ χ ω ρ ή σ ε τ ε τ ο γ ρ ή γ ο ρ ο κ α ι α τ η µ έ λ η τ ο ύ
Chapter 4 : Linear Wire Antenna
Chapt 4 : Lina Wi Antnna nfinitsima Dipo Sma Dipo Finit Lngth Dipo Haf-Wavngth Dipo Lina mnts na o on nfinit Pfct Conductos nfinitsima Dipo Lngth
Reflection & Transmission
Rflc & Tasmss 4 D. Ray Kw Rflc & Tasmss - D. Ray Kw Gmc Opcs (M wavs flc fac - asmss cdc.. Sll s Law: s s 3. Ccal agl: s c / 4. Tal flc wh > c ly f > Rflc & Tasmss - D. Ray Kw Pla Wav λ wavfs λ λ. < ;
Matrices and Determinants
Matrices and Determinants SUBJECTIVE PROBLEMS: Q 1. For what value of k do the following system of equations possess a non-trivial (i.e., not all zero) solution over the set of rationals Q? x + ky + 3z
Aperture Radiation: Huygen s Equation
perture Radiatin: Hugen s quatin = Radiating patch, assume unifrm plane wave: H, /H = 377Ω perture in X-Y plane ˆ ˆ α r(, R θ ϕ ϕ z Superpsitin f cntributins frm radiating patches H J surface current S
Κύµατα παρουσία βαρύτητας
Κύµατα παουσία βαύτητας 8. Grait as in th ocan Sarantis Sofianos Dpt. of hsics, Unirsit of thns Was in th ocan Srfac grait as Short and long limit in grait as Wa charactristics Intrnal as Charactristic
Relative Valuation. Relative Valuation. Relative Valuation. Υπολογισµός αξίας επιχείρησης µε βάση τρέχουσες αποτιµήσεις οµοειδών εταιρειών
Rlativ Valuatio Αρτίκης Γ. Παναγιώτης Rlativ Valuatio Rlativ Valuatio Υπολογισµός αξίας επιχείρησης µε βάση τρέχουσες αποτιµήσεις οµοειδών εταιρειών Ø Επιλογή οµοειδών επιχειρήσεων σε όρους κινδύνου, ανάπτυξης
ECE 222b Applied Electromagnetics Notes Set 3a
C b lid lcomagnics Nos S 3a Insuco: Pof. Viali Lomakin Damn of lcical and Comu ngining Univsi of Califonia San Digo Unifom Plan Wavs Consid Mawll s quaions: In a losslss mdium ε and µ a al and σ : Sinc
D Alembert s Solution to the Wave Equation
D Alembert s Solution to the Wave Equation MATH 467 Partial Differential Equations J. Robert Buchanan Department of Mathematics Fall 2018 Objectives In this lesson we will learn: a change of variable technique
Lecture 31. Wire Antennas. Generation of radiation by real wire antennas
Lctu 31 Wi Antnnas n this lctu yu will lan: Gnatin f aiatin by al wi antnnas Sht ipl antnnas Half-wav ipl antnnas Th-half-wav ipl antnnas Small wi lp antnnas magntic ipl antnnas ECE 303 Fall 006 Fahan
CRASH COURSE IN PRECALCULUS
CRASH COURSE IN PRECALCULUS Shiah-Sen Wang The graphs are prepared by Chien-Lun Lai Based on : Precalculus: Mathematics for Calculus by J. Stuwart, L. Redin & S. Watson, 6th edition, 01, Brooks/Cole Chapter
Space-Time Symmetries
Chapter Space-Time Symmetries In classical fiel theory any continuous symmetry of the action generates a conserve current by Noether's proceure. If the Lagrangian is not invariant but only shifts by a
ΕΝΙΣΧΥΣΗ ΠΛΑΚΩΝ ΚΑΙ ΔΟΚΩΝ ΣΕ ΚΑΜΨΗ ΜΕ ΜΑΝΔΥΕΣ Η ΕΛΑΣΜΑΤΑ ΣΥΝΘΕΤΩΝ ΥΛΙΚΩΝ.
ΕΝΙΣΧΥΣΗ ΠΛΑΚΩΝ ΚΑΙ ΔΟΚΩΝ ΣΕ ΚΑΜΨΗ ΜΕ ΜΑΝΔΥΕΣ Η ΕΛΑΣΜΑΤΑ ΣΥΝΘΕΤΩΝ ΥΛΙΚΩΝ. Σύμφωνα με τον Κανονιμό Επεμβάεων, ο νέος οπλιμός υπολοίζεται έτι ώτε ε υνεραία με τον υφιτάμενο παλαιό οπλιμό να αναλαμβάνονται
16 Electromagnetic induction
Chatr : Elctromagntic Induction Elctromagntic induction Hint to Problm for Practic., 0 d φ or dφ 0 0.0 Wb. A cm cm 7 0 m, A 0 cm 0 cm 00 0 m B 0.8 Wb/m, B. Wb/m,, dφ d BA (B.A) BA 0.8 7 0. 00 0 80 0 8
Convolution product formula for associated homogeneous distributions on R
Cnvlutin prduct frmula fr assciatd hmgnus distributins n R Ghislain R. FRANSSENS Blgian Institut fr Spac Arnmy Ringlaan 3 B-80 Brussls Blgium E-mail: ghislain.franssns@arnmy.b Octbr 009 Abstract Th st
Durbin-Levinson recursive method
Durbin-Levinson recursive method A recursive method for computing ϕ n is useful because it avoids inverting large matrices; when new data are acquired, one can update predictions, instead of starting again
Derivation of Optical-Bloch Equations
Appendix C Derivation of Optical-Bloch Equations In this appendix the optical-bloch equations that give the populations and coherences for an idealized three-level Λ system, Fig. 3. on page 47, will be
Διερεύνηση και αξιολόγηση μεθόδων ομογενοποίησης υδροκλιματικών δεδομένων ΔΙΠΛΩΜΑΤΙΚΗ ΕΡΓΑΣΙΑ
ΕΘΝΙΚΟ ΜΕΤΣΟΒΕΙΟ ΠΟΛΥΤΕΧΝΕΙΟ ΣΧΟΛΗ ΠΟΛΙΤΙΚΩΝ ΜΗΧΑΝΙΚΩΝ Τομέας Υδατικών Πόρων και Περιβάλλοντος Εύα- Στυλιανή Στείρου Διερεύνηση και αξιολόγηση μεθόδων ομογενοποίησης υδροκλιματικών δεδομένων ΔΙΠΛΩΜΑΤΙΚΗ
PULLEYS 1. GROOVE SPECIFICATIONS FOR V-BELT PULLEYS. Groove dimensions and tolerances for Hi-Power PowerBand according to RMA engineering standards
1. GROOVE SPECIFICATIONS FOR V-BELT PULLEYS Figur 3 - Groov dimnsion nomnclatur or V-blts α go lp b Ectiv diamtr Datum diamtr d Tabl No. 1 - Groov dimnsions and tolrancs or Hi-Powr PowrBand according to
Α Ρ Ι Θ Μ Ο Σ : 6.913
Α Ρ Ι Θ Μ Ο Σ : 6.913 ΠΡΑΞΗ ΚΑΤΑΘΕΣΗΣ ΟΡΩΝ ΔΙΑΓΩΝΙΣΜΟΥ Σ τ η ν Π ά τ ρ α σ ή μ ε ρ α σ τ ι ς δ ε κ α τ έ σ σ ε ρ ι ς ( 1 4 ) τ ο υ μ ή ν α Ο κ τ ω β ρ ί ο υ, η μ έ ρ α Τ ε τ ά ρ τ η, τ ο υ έ τ ο υ ς δ
Appendix A. Stability of the logistic semi-discrete model.
Ecological Archiv E89-7-A Elizava Pachpky, Rogr M. Nib, and William W. Murdoch. 8. Bwn dicr and coninuou: conumr-rourc dynamic wih ynchronizd rproducion. Ecology 89:8-88. Appndix A. Sabiliy of h logiic
Section 8.3 Trigonometric Equations
99 Section 8. Trigonometric Equations Objective 1: Solve Equations Involving One Trigonometric Function. In this section and the next, we will exple how to solving equations involving trigonometric functions.
Space Physics (I) [AP-3044] Lecture 1 by Ling-Hsiao Lyu Oct Lecture 1. Dipole Magnetic Field and Equations of Magnetic Field Lines
Space Physics (I) [AP-344] Lectue by Ling-Hsiao Lyu Oct. 2 Lectue. Dipole Magnetic Field and Equations of Magnetic Field Lines.. Dipole Magnetic Field Since = we can define = A (.) whee A is called the
3.4 SUM AND DIFFERENCE FORMULAS. NOTE: cos(α+β) cos α + cos β cos(α-β) cos α -cos β
3.4 SUM AND DIFFERENCE FORMULAS Page Theorem cos(αβ cos α cos β -sin α cos(α-β cos α cos β sin α NOTE: cos(αβ cos α cos β cos(α-β cos α -cos β Proof of cos(α-β cos α cos β sin α Let s use a unit circle
& : $!" # RC : ) %& & '"( RL : ), *&+ RLC : - # ( : $. %! & / 0!1& ( :
: : C : : C : : : .. ).. (................... ٢ ( - ). :.... S MP. T S..... -. (... ) :. :. : :. - - - - ٣ sweep :X. :Y. :. CCD.. ( - ) ( - ) ( - ) ( ) ( ) ( ) X : gnd -.... ٤ DC AC - AC DC DC - Y ( )
derivation of the Laplacian from rectangular to spherical coordinates
derivation of the Laplacian from rectangular to spherical coordinates swapnizzle 03-03- :5:43 We begin by recognizing the familiar conversion from rectangular to spherical coordinates (note that φ is used
If we restrict the domain of y = sin x to [ π, π ], the restrict function. y = sin x, π 2 x π 2
Chapter 3. Analytic Trigonometry 3.1 The inverse sine, cosine, and tangent functions 1. Review: Inverse function (1) f 1 (f(x)) = x for every x in the domain of f and f(f 1 (x)) = x for every x in the
If we restrict the domain of y = sin x to [ π 2, π 2
Chapter 3. Analytic Trigonometry 3.1 The inverse sine, cosine, and tangent functions 1. Review: Inverse function (1) f 1 (f(x)) = x for every x in the domain of f and f(f 1 (x)) = x for every x in the
Section 8.2 Graphs of Polar Equations
Section 8. Graphs of Polar Equations Graphing Polar Equations The graph of a polar equation r = f(θ), or more generally F(r,θ) = 0, consists of all points P that have at least one polar representation
Faculdade de Engenharia. Transmission Lines ELECTROMAGNETIC ENGINEERING MAP TELE 2008/2009
Facudad d Ennharia Transmission ins EECTROMAGNETC ENGNEERNG MAP TEE 8/9 Transmission ins Facudad d Ennharia transmission ins wavuids supportin TEM wavs most common typs para-pat wavuids coaxia wavuids
ibemo Kazakhstan Republic of Kazakhstan, West Kazakhstan Oblast, Aksai, Pramzone, BKKS office complex Phone: ; Fax:
3.4. Click here for solutions. Click here for answers. CURVE SKETCHING. y cos x sin x. x 1 x 2. x 2 x 3 4 y 1 x 2. x 5 2
SECTION. CURVE SKETCHING. CURVE SKETCHING A Click here for answers. S Click here for solutions. 9. Use the guidelines of this section to sketch the curve. cos sin. 5. 6 8 7 0. cot, 0.. 9. cos sin. sin
The Finite Element Method
Th Finit Elmnt Mthod Plan (D) Truss and Fram Elmnts Rad: Sctions 4.6 and 5.4 CONTENTS Rviw of bar finit lmnt in th local coordinats Plan truss lmnt Rviw of bam finit lmnt in th local coordinats Plan fram
CHAPTER 101 FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD
CHAPTER FOURIER SERIES FOR PERIODIC FUNCTIONS OF PERIOD EXERCISE 36 Page 66. Determine the Fourier series for the periodic function: f(x), when x +, when x which is periodic outside this rge of period.
Uniform Convergence of Fourier Series Michael Taylor
Uniform Convergence of Fourier Series Michael Taylor Given f L 1 T 1 ), we consider the partial sums of the Fourier series of f: N 1) S N fθ) = ˆfk)e ikθ. k= N A calculation gives the Dirichlet formula
CHAPTER 10. Hence, the circuit in the frequency domain is as shown below. 4 Ω V 1 V 2. 3Vx 10 = + 2 Ω. j4 Ω. V x. At node 1, (1) At node 2, where V
February 5, 006 CHAPTER 0 P.P.0. 0 in(t 0 0, ω H jωl j4 0. F -j.5 jωc Hence, e circuit in e frequency dmain i a hwn belw. -j.5 Ω 4 Ω 0 0 A Ω x j4 Ω x At nde, At nde, 0 - j.5 00 (5 j4 j ( 4 x where x j4
2. Α ν ά λ υ σ η Π ε ρ ι ο χ ή ς. 3. Α π α ι τ ή σ ε ι ς Ε ρ γ ο δ ό τ η. 4. Τ υ π ο λ ο γ ί α κ τ ι ρ ί ω ν. 5. Π ρ ό τ α σ η. 6.
Π Ε Ρ Ι Ε Χ Ο Μ Ε Ν Α 1. Ε ι σ α γ ω γ ή 2. Α ν ά λ υ σ η Π ε ρ ι ο χ ή ς 3. Α π α ι τ ή σ ε ι ς Ε ρ γ ο δ ό τ η 4. Τ υ π ο λ ο γ ί α κ τ ι ρ ί ω ν 5. Π ρ ό τ α σ η 6. Τ ο γ ρ α φ ε ί ο 1. Ε ι σ α γ ω
7. Schematic Diagram. 7-1 Overall Block Diagram FRONT MAIN MAIN CD SMPS (MAX-A54U)...
7. Schematic Diagram 7- Overall Block Diagram... 7-7- FRONT... 7-7- MAIN-... 7-7- MAIN-... 7-5 7-5 CD... 7-7- SM (MAX-A5U)... 7-7 7-7 SM (MAX-A55U)... 7- Samsung Electronics This Document can not be used
Section 7.6 Double and Half Angle Formulas
09 Section 7. Double and Half Angle Fmulas To derive the double-angles fmulas, we will use the sum of two angles fmulas that we developed in the last section. We will let α θ and β θ: cos(θ) cos(θ + θ)
Solution Series 9. i=1 x i and i=1 x i.
Lecturer: Prof. Dr. Mete SONER Coordinator: Yilin WANG Solution Series 9 Q1. Let α, β >, the p.d.f. of a beta distribution with parameters α and β is { Γ(α+β) Γ(α)Γ(β) f(x α, β) xα 1 (1 x) β 1 for < x
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
6.1. Dirac Equation. Hamiltonian. Dirac Eq.
6.1. Dirac Equation Ref: M.Kaku, Quantum Field Theory, Oxford Univ Press (1993) η μν = η μν = diag(1, -1, -1, -1) p 0 = p 0 p = p i = -p i p μ p μ = p 0 p 0 + p i p i = E c 2 - p 2 = (m c) 2 H = c p 2
Practice Exam 2. Conceptual Questions. 1. State a Basic identity and then verify it. (a) Identity: Solution: One identity is csc(θ) = 1
Conceptual Questions. State a Basic identity and then verify it. a) Identity: Solution: One identity is cscθ) = sinθ) Practice Exam b) Verification: Solution: Given the point of intersection x, y) of the
1999 by CRC Press LLC
Plarikas A. D. Trignmetric and Hyperblic Fnctins The Handbk f Frmlas and Tables fr Signal Prcessing. Ed. Aleander D. Plarikas Bca Ratn: CRC Press LLC,999 999 by CRC Press LLC 43 Trignmetry and Hyperblic
Errata Sheet. 2 k. r 2. ts t. t t ... cos n W. cos nx W. W n x. Page Location Error Correction 2 Eq. (1.3) q dt. W/m K. 100 Last but 6 2.
Eaa S Pag can E Ccn Eq. (. q q k W/ K k W/ K A A 6 n as bu 6 s q lns s q T k T k Q.. Wall s aus n gvn Wall s aus a an C. 7 n, lf kc cs ( s sn kc cs ( s sn s f cs k sn cs k sn quan C ( s C ( s an ln 6 sn
1 String with massive end-points
1 String with massive end-points Πρόβλημα 5.11:Θεωρείστε μια χορδή μήκους, τάσης T, με δύο σημειακά σωματίδια στα άκρα της, το ένα μάζας m, και το άλλο μάζας m. α) Μελετώντας την κίνηση των άκρων βρείτε
Representing Relations Using Digraph
M R n = M R, Κλειστότητες, Ισοδυναµίες, Μερικές ιατάξεις Ορέστης Τελέλης tllis@unipi.gr Τµήµα Ψηφιακών Συστηµάτων, Πανεπιστήµιο Πειραιώς Σύνοψη Προηγούµενου EXAMPLE 6 from th finition of Booln powrs. Exris
α A G C T 國立交通大學生物資訊及系統生物研究所林勇欣老師
A G C T Juks and Cantor s (969) on-aramtr modl A T C G A G 0 0 0-3 C T A() A( t ) ( 3 ) ( ) A() A() ( 3 ) ( ) A( A( A( A( t ) A( 3 A( t ) ( ) A( A( Juks and Cantor s (969) on-aramtr modl A( A( t ) A( d
ω ω ω ω ω ω+2 ω ω+2 + ω ω ω ω+2 + ω ω+1 ω ω+2 2 ω ω ω ω ω ω ω ω+1 ω ω2 ω ω2 + ω ω ω2 + ω ω ω ω2 + ω ω+1 ω ω2 + ω ω+1 + ω ω ω ω2 + ω
0 1 2 3 4 5 6 ω ω + 1 ω + 2 ω + 3 ω + 4 ω2 ω2 + 1 ω2 + 2 ω2 + 3 ω3 ω3 + 1 ω3 + 2 ω4 ω4 + 1 ω5 ω 2 ω 2 + 1 ω 2 + 2 ω 2 + ω ω 2 + ω + 1 ω 2 + ω2 ω 2 2 ω 2 2 + 1 ω 2 2 + ω ω 2 3 ω 3 ω 3 + 1 ω 3 + ω ω 3 +
Διπλωματική Εργασία του φοιτητή του Τμήματος Ηλεκτρολόγων Μηχανικών και Τεχνολογίας Υπολογιστών της Πολυτεχνικής Σχολής του Πανεπιστημίου Πατρών
ΠΑΝΕΠΙΣΤΗΜΙΟ ΠΑΤΡΩΝ ΤΜΗΜΑ ΗΛΕΚΤΡΟΛΟΓΩΝ ΜΗΧΑΝΙΚΩΝ ΚΑΙ ΤΕΧΝΟΛΟΓΙΑΣ ΥΠΟΛΟΓΙΣΤΩΝ ΤΟΜΕΑΣ:ΗΛΕΚΤΡΟΝΙΚΗΣ ΚΑΙ ΥΠΟΛΟΓΙΣΤΩΝ ΕΡΓΑΣΤΗΡΙΟ ΗΛΕΚΤΡΟΝΙΚΩΝ ΕΦΑΡΜΟΓΩΝ Διπλωματική Εργασία του φοιτητή του Τμήματος Ηλεκτρολόγων
Mock Exam 7. 1 Hong Kong Educational Publishing Company. Section A 1. Reference: HKDSE Math M Q2 (a) (1 + kx) n 1M + 1A = (1) =
Mock Eam 7 Mock Eam 7 Section A. Reference: HKDSE Math M 0 Q (a) ( + k) n nn ( )( k) + nk ( ) + + nn ( ) k + nk + + + A nk... () nn ( ) k... () From (), k...() n Substituting () into (), nn ( ) n 76n 76n
(... )..!, ".. (! ) # - $ % % $ & % 2007
(! ), "! ( ) # $ % & % $ % 007 500 ' 67905:5394!33 : (! ) $, -, * +,'; ), -, *! ' - " #!, $ & % $ ( % %): /!, " ; - : - +', 007 5 ISBN 978-5-7596-0766-3 % % - $, $ &- % $ % %, * $ % - % % # $ $,, % % #-
Finite Field Problems: Solutions
Finite Field Problems: Solutions 1. Let f = x 2 +1 Z 11 [x] and let F = Z 11 [x]/(f), a field. Let Solution: F =11 2 = 121, so F = 121 1 = 120. The possible orders are the divisors of 120. Solution: The
2. Μηχανικό Μαύρο Κουτί: κύλινδρος με μια μπάλα μέσα σε αυτόν.
Experiental Copetition: 14 July 011 Proble Page 1 of. Μηχανικό Μαύρο Κουτί: κύλινδρος με μια μπάλα μέσα σε αυτόν. Ένα μικρό σωματίδιο μάζας (μπάλα) βρίσκεται σε σταθερή απόσταση z από το πάνω μέρος ενός
Inverse trigonometric functions & General Solution of Trigonometric Equations. ------------------ ----------------------------- -----------------
Inverse trigonometric functions & General Solution of Trigonometric Equations. 1. Sin ( ) = a) b) c) d) Ans b. Solution : Method 1. Ans a: 17 > 1 a) is rejected. w.k.t Sin ( sin ) = d is rejected. If sin
Homework 8 Model Solution Section
MATH 004 Homework Solution Homework 8 Model Solution Section 14.5 14.6. 14.5. Use the Chain Rule to find dz where z cosx + 4y), x 5t 4, y 1 t. dz dx + dy y sinx + 4y)0t + 4) sinx + 4y) 1t ) 0t + 4t ) sinx
Monochromatic Radiation is Always 100% Polarized
Mnchrmatic Radiatin is lwas % Plarized Plarizatin llipse z Prpagatin Right-Hand Plarizatin v b z θ a ϕ (t) v 3 Parameters Specif llipse e.g. a, b, ϕ a, ϕ, θ v, v, θ ls, (need + r t right r left elliptical)
ΚΥΠΡΙΑΚΗ ΕΤΑΙΡΕΙΑ ΠΛΗΡΟΦΟΡΙΚΗΣ CYPRUS COMPUTER SOCIETY ΠΑΓΚΥΠΡΙΟΣ ΜΑΘΗΤΙΚΟΣ ΔΙΑΓΩΝΙΣΜΟΣ ΠΛΗΡΟΦΟΡΙΚΗΣ 6/5/2006
Οδηγίες: Να απαντηθούν όλες οι ερωτήσεις. Ολοι οι αριθμοί που αναφέρονται σε όλα τα ερωτήματα είναι μικρότεροι το 1000 εκτός αν ορίζεται διαφορετικά στη διατύπωση του προβλήματος. Διάρκεια: 3,5 ώρες Καλή
Approximation of distance between locations on earth given by latitude and longitude
Approximation of distance between locations on earth given by latitude and longitude Jan Behrens 2012-12-31 In this paper we shall provide a method to approximate distances between two points on earth
webpage :
Amin Haliloic Mah Eciss E-mail : amin@shkhs wbpa : wwwshkhs/amin MATH EXERISES GRADIENT DIVERGENE URL DEL NABLA OERATOR LALAIAN OERATOR ONTINUITY AND NAVIER-STOKES EQUATIONS VETOR RODUTS I and hn scala
Affine Weyl Groups. Gabriele Nebe. Summerschool GRK 1632, September Lehrstuhl D für Mathematik
Affine Weyl Groups Gabriele Nebe Lehrstuhl D für Mathematik Summerschool GRK 1632, September 2015 Crystallographic root systems. Definition A crystallographic root system Φ is a finite set of non zero
Notes on the Open Economy
Notes on the Open Econom Ben J. Heijdra Universit of Groningen April 24 Introduction In this note we stud the two-countr model of Table.4 in more detail. restated here for convenience. The model is Table.4.
Similarly, we may define hyperbolic functions cosh α and sinh α from the unit hyperbola
Universit of Hperbolic Functions The trigonometric functions cos α an cos α are efine using the unit circle + b measuring the istance α in the counter-clockwise irection along the circumference of the
TeSys contactors a.c. coils for 3-pole contactors LC1-D
References a.c. coils for 3-pole contactors LC1-D Control circuit voltage Average resistance Inductance of Reference (1) Weight Uc at 0 C ± 10 % closed circuit For 3-pole " contactors LC1-D09...D38 and
1 B0 C00. nly Difo. r II. on III t o. ly II II. Di XR. Di un 5.8. Di Dinly. Di F/ / Dint. mou. on.3 3 D. 3.5 ird Thi. oun F/2. s m F/3 /3.
. F/ /3 3. I F/ 7 7 0 0 Mo ode del 0 00 0 00 A 6 A C00 00 0 S 0 C 0 008 06 007 07 09 A 0 00 0 00 0 009 09 A 7 I 7 7 0 0 F/.. 6 6 8 8 0 00 0 F/3 /3. fo I t o nt un D ou s ds 3. ird F/ /3 Thi ur T ou 0 Fo
On the Galois Group of Linear Difference-Differential Equations
On the Galois Group of Linear Difference-Differential Equations Ruyong Feng KLMM, Chinese Academy of Sciences, China Ruyong Feng (KLMM, CAS) Galois Group 1 / 19 Contents 1 Basic Notations and Concepts
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 = =
.. ntsets ofa.. d ffeom.. orp ism.. na s.. m ooth.. man iod period I n open square. n t s e t s ofa \quad d ffeom \quad orp ism \quad na s \quad m o
G G - - -- - W - - - R S - q k RS ˆ W q q k M G W R S L [ RS - q k M S 4 R q k S [ RS [ M L ˆ L [M O S 4] L ˆ ˆ L ˆ [ M ˆ S 4 ] ˆ - O - ˆ q k ˆ RS q k q k M - j [ RS ] [ M - j - L ˆ ˆ ˆ O ˆ [ RS ] [ M
Math 6 SL Probability Distributions Practice Test Mark Scheme
Math 6 SL Probability Distributions Practice Test Mark Scheme. (a) Note: Award A for vertical line to right of mean, A for shading to right of their vertical line. AA N (b) evidence of recognizing symmetry
Additional Results for the Pareto/NBD Model
Additional Results for the Pareto/NBD Model Peter S. Fader www.petefader.com Bruce G. S. Hardie www.brucehardie.com January 24 Abstract This note derives expressions for i) the raw moments of the posterior
Second Order RLC Filters
ECEN 60 Circuits/Electronics Spring 007-0-07 P. Mathys Second Order RLC Filters RLC Lowpass Filter A passive RLC lowpass filter (LPF) circuit is shown in the following schematic. R L C v O (t) Using phasor
( y) Partial Differential Equations
Partial Dierential Equations Linear P.D.Es. contains no owers roducts o the deendent variables / an o its derivatives can occasionall be solved. Consider eamle ( ) a (sometimes written as a ) we can integrate
Appendix to On the stability of a compressible axisymmetric rotating flow in a pipe. By Z. Rusak & J. H. Lee
Appendi to On the stability of a compressible aisymmetric rotating flow in a pipe By Z. Rusak & J. H. Lee Journal of Fluid Mechanics, vol. 5 4, pp. 5 4 This material has not been copy-edited or typeset
19. ATOMS, MOLECULES AND NUCLEI HOMEWORK SOLUTIONS
. ATOMS, MOLECULES AND NUCLEI HOMEWORK SOLUTIONS. Givn :.53 Å 3?? n n ε πm n n Radius of n t Bo obit, n n ε πm n n 3 n 3 n 3 (3) () (.53).77Å n n ( ) () (.53) 53 Å. Givn : 3 7.7 x m? n n ε πm Radius of
Class 03 Systems modelling
Class 03 Systems mdelling Systems mdelling input utput spring / mass / damper Systems mdelling spring / mass / damper Systems mdelling spring / mass / damper applied frce displacement input utput Systems
ΑΓΓΕΛΗΣ ΧΡΗΣΤΟΣ ΠΑΝΑΓΙΩΤΗΣ 6 OO ΑΓΓΕΛΙΔΗΣ ΧΑΡΙΛΑΟΣ ΧΡΗΣΤΟΣ 4 OO ΑΓΓΟΥ ΑΝΑΣΤΑΣΙΑ ΔΗΜΗΤΡΙΟΣ 6 OO ΑΔΑΜΙΔΟΥ ΕΥΑΓΓΕΛΙΑ ΑΒΡΑΑΜ 3 OO ΑΛΕΒΙΖΟΥ ΠΑΝΑΓΙΩΤΑ
ΕΠΩΝΥΜΙΑ ΠΕΡΙΟΔΟΣ ΜΕΣΟ ΑΓΓΕΛΗΣ ΧΡΗΣΤΟΣ ΠΑΝΑΓΙΩΤΗΣ 6 OO ΑΓΓΕΛΙΔΗΣ ΧΑΡΙΛΑΟΣ ΧΡΗΣΤΟΣ 4 OO ΑΓΓΟΥ ΑΝΑΣΤΑΣΙΑ ΔΗΜΗΤΡΙΟΣ 6 OO ΑΔΑΜΙΔΟΥ ΕΥΑΓΓΕΛΙΑ ΑΒΡΑΑΜ 3 OO ΑΛΕΒΙΖΟΥ ΠΑΝΑΓΙΩΤΑ ΔΗΜΗΤΡΙΟΣ 7 OO ΑΝΑΓΝΩΣΤΟΠΟΥΛΟΥ ΖΩΙΤΣΑ
Lossy Medium EE142. Dr. Ray Kwok
Lssy Mdium EE4 D. Ray Kwk fn: Fundamntals f Engining Eltmagntis, David K. Chng (Addisn-Wsly) Eltmagntis f Engins, Fawwaz T. Ulaby (Pnti Hall) Lssy Mdium - D. Ray Kwk Ohm s Law A E V V El IR ( JA) E Jρ
Trigonometric Formula Sheet
Trigonometric Formula Sheet Definition of the Trig Functions Right Triangle Definition Assume that: 0 < θ < or 0 < θ < 90 Unit Circle Definition Assume θ can be any angle. y x, y hypotenuse opposite θ
Example Sheet 3 Solutions
Example Sheet 3 Solutions. i Regular Sturm-Liouville. ii Singular Sturm-Liouville mixed boundary conditions. iii Not Sturm-Liouville ODE is not in Sturm-Liouville form. iv Regular Sturm-Liouville note
Κεφάλαιο 1 Πραγματικοί Αριθμοί 1.1 Σύνολα
x 2 + 1 = 0 N = {1, 2, 3....}, Z Q a, b a, b N c, d c, d N a + b = c, a b = d. a a N 1 a = a 1 = a. < > P n P (n) P (1) n = 1 P (n) P (n + 1) n n + 1 P (n) n P (n) n P n P (n) P (m) P (n) n m P (n + 1)
Παραγωγή ήχου από ψάρια που υέρουν νηκτική κύστη: Παραμετρική ανάλυση του μοντέλου
Παραγωγή ήχου από ψάρια που υέρουν νηκτική κύστη: Παραμετρική ανάλυση του μοντέλου Σππξίδσλ Κνπδνύπεο Τκήκα Μνπζηθήο Τερλνινγίαο θαη Αθνπζηηθήο, Τ.Δ.Ι. Κξήηεο skuz@staff.teicrete.gr Παλαγηώηεο Παπαδάθεο
Σχεδίαση και Ανάπτυξη Παιχνιδιού για την Εκμάθηση των Βασικών Στοιχείων ενός Υπολογιστή με Χρήση του Περιβάλλοντος GameMaker
Α Ρ Ι Σ Τ Ο Τ Ε Λ Ε Ι Ο Π Α Ν Ε Π Ι Σ Τ Η Μ Ι Ο Θ Ε Σ Σ Α Λ Ο Ν Ι Κ Η Σ ΣΧΟΛΗ ΘΕΤΙΚΩΝ ΕΠΙΣΤΗΜΩΝ ΤΜΗΜΑ ΠΛΗΡΟΦΟΡΙΚΗΣ ΠΤΥΧΙΑΚΗ ΕΡΓΑΣΙΑ Ηλίας Ανδρεάδης Α.Ε.Μ 1443 Μιχάλης Στρατίδης Α.Ε.Μ 1543 Σχεδίαση και
A Two-Sided Laplace Inversion Algorithm with Computable Error Bounds and Its Applications in Financial Engineering
Electronic Companion A Two-Sie Laplace Inversion Algorithm with Computable Error Bouns an Its Applications in Financial Engineering Ning Cai, S. G. Kou, Zongjian Liu HKUST an Columbia University Appenix
Problem Set 9 Solutions. θ + 1. θ 2 + cotθ ( ) sinθ e iφ is an eigenfunction of the ˆ L 2 operator. / θ 2. φ 2. sin 2 θ φ 2. ( ) = e iφ. = e iφ cosθ.
Chemistry 362 Dr Jean M Standard Problem Set 9 Solutions The ˆ L 2 operator is defined as Verify that the angular wavefunction Y θ,φ) Also verify that the eigenvalue is given by 2! 2 & L ˆ 2! 2 2 θ 2 +
[1] P Q. Fig. 3.1
1 (a) Define resistance....... [1] (b) The smallest conductor within a computer processing chip can be represented as a rectangular block that is one atom high, four atoms wide and twenty atoms long. One
Lifting Entry (continued)
ifting Entry (continued) Basic planar dynamics of motion, again Yet another equilibrium glide Hypersonic phugoid motion Planar state equations MARYAN 1 01 avid. Akin - All rights reserved http://spacecraft.ssl.umd.edu
Lecture 30. An Array of Two Hertzian Dipole Antennas
Lctu 30 An A f Tw tin Di Antnns n tis ctu u wi n: tin di ntnn s ntfnc nd f-fid ditin ttns C 303 F 005 Fn Rn Cn Univsit Cctistics f Sing tin Di Antnn Antnn in: F tin di t gin is: S(, t ) 3 (, ) Pd ( ) (,
Potential Dividers. 46 minutes. 46 marks. Page 1 of 11
Potential Dividers 46 minutes 46 marks Page 1 of 11 Q1. In the circuit shown in the figure below, the battery, of negligible internal resistance, has an emf of 30 V. The pd across the lamp is 6.0 V and
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
SCHOOL OF MATHEMATICAL SCIENCES G11LMA Linear Mathematics Examination Solutions
SCHOOL OF MATHEMATICAL SCIENCES GLMA Linear Mathematics 00- Examination Solutions. (a) i. ( + 5i)( i) = (6 + 5) + (5 )i = + i. Real part is, imaginary part is. (b) ii. + 5i i ( + 5i)( + i) = ( i)( + i)
ΤΕΧΝΟΛΟΓΙΚΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΥΠΡΟΥ ΣΧΟΛΗ ΕΠΙΣΤΗΜΩΝ ΥΓΕΙΑΣ
ΤΕΧΝΟΛΟΓΙΚΟ ΠΑΝΕΠΙΣΤΗΜΙΟ ΚΥΠΡΟΥ ΣΧΟΛΗ ΕΠΙΣΤΗΜΩΝ ΥΓΕΙΑΣ Πτυχιακή Εργασία "Η ΣΗΜΑΝΤΙΚΟΤΗΤΑ ΤΟΥ ΜΗΤΡΙΚΟΥ ΘΗΛΑΣΜΟΥ ΣΤΗ ΠΡΟΛΗΨΗ ΤΗΣ ΠΑΙΔΙΚΗΣ ΠΑΧΥΣΑΡΚΙΑΣ" Ειρήνη Σωτηρίου Λεμεσός 2014 ΤΕΧΝΟΛΟΓΙΚΟ ΠΑΝΕΠΙΣΤΗΜΙΟ
1. A fully continuous 20-payment years, 30-year term life insurance of 2000 is issued to (35). You are given n A 1
Chapter 7: Exercises 1. A fully continuous 20-payment years, 30-year term life insurance of 2000 is issued to (35). You are given n A 1 35+n:30 n a 35+n:20 n 0 0.068727 11.395336 10 0.097101 7.351745 25
Από την Κριτική Εθνογραφία στην Κριτική Έρευνα Δράσης: Ένα συνεχές στο σχεδιασμό της εκπαιδευτικής καινοτομίας 1
Από την Κριτική Εθνογραφία στην Κριτική Έρευνα Δράσης: Ένα συνεχές στο σχεδιασμό της εκπαιδευτικής καινοτομίας 1 Ελευθέριος Βεκρής Δρ. Επιστημών της Αγωγής Εκπαιδευτικός Δευτεροβάθμιας Εκπαίδευσης From