6.641, Electromagnetic Fields, Forces, and Motion Prof. Markus Zahn Lecture 7: Polarization and Conduction
|
|
- Κρέων Παπαδόπουλος
- 5 χρόνια πριν
- Προβολές:
Transcript
1 6.641, Electromgnetic Fiels, Forces, n Motion Prof. Mrkus Zhn Lecture 7: Polriztion n Conuction I. Experimentl Oservtion A. Fixe oltge - Switch Close ( v= o ) As n insulting mteril enters free-spce cpcitor t constnt voltge more chrge flows onto the electroes; i.e. s x increses, i increses. B. Fixe Chrge - Switch open (i=0) As n insulting mteril enters free spce cpcitor t constnt chrge, the voltge ecreses; i.e. s x increses, v ecreses. II. Dipole Moel of Polriztion A. Polriztion ector P = Np = Nq ( p = q ipole moment) N ipoles/olume ( P is ipole ensity) q q Prof. Mrkus Zhn Pge 1 of 7
2 Courtesy of Krieger Pulishing. Use with permission. Prof. Mrkus Zhn Pge of 7
3 Q = qni = ρ insie S P pire chrge or equivlently polriztion chrge ensity Q = P i = ip = ρ insie S P (Divergence Theorem) P=qN i P = ρ P B. Guss Lw ( E) i = ρ = ρ ρ = ρ ip o totl u P u unpire chrge ensity; lso clle free chrge ensity ( E P ) = ρ i o u D = E P Displcement Flux Density o i D = ρ u C. Bounry Conitions Prof. Mrkus Zhn Pge 3 of 7
4 u u su S i D= ρ D i = ρ n i D D = σ P P sp S i P= ρ P i = ρ n i P P = σ ( ) i E = ρ ρ E i = ρ ρ n i E E = σ σ o u P o u P o su sp S D. Polriztion Current Density Q = qn = qni = P i [Amount of Chrge pssing through surfce re element ] i p Q P = = i t t [Current pssing through surfce re element ] = Jp i polriztion current ensity J p P = t Ampere s lw: xh = J J u p o E t P = Ju t o E t ( o ) = Ju E P t D t = Ju Prof. Mrkus Zhn Pge 4 of 7
5 III. Equipotentil Sphere in Uniform Electric Fiel r o o o lim Φ r, θ =Ercosθ Φ= E z =Ercosθ Φ ( r = R, θ ) = 0 3 R Φ ( r, θ ) = Eo r cos θ r This solution is compose of the superposition of uniform electric fiel plus the fiel ue to point electric ipole t the center of the sphere: p cosθ Φ = π ipole 4 or 3 with p = 4π E R o o This ipole is ue to the surfce chrge istriution on the sphere. 3 Φ R σ s ( r = R, θ ) = oer ( r = R, θ ) = o = oeo 1 cos 3 θ r r= R r r= R = 3 E cosθ o o Prof. Mrkus Zhn Pge 5 of 7
6 I. Artificil Dielectric v v E =, s E σ = = A q =σ sa = v C = q = A v _ υ E Courtesy of Hermnn A. Hus n Jmes R. Melcher. Use with permission. For sphericl rry of non-intercting spheres (s >> R) _ 3 3 P=4π R E iz P =N p =4π R E N o o z z o o N= 1 s 3 R 3 R 3 P= o 4π E= ψe o E ψe =4π s s ψ e (electric susceptiility) D= o E P= o 1 ψe E= E r (reltive ielectric constnt) 3 R = r o = o 1 ψ e = o 1 4π s Prof. Mrkus Zhn Pge 6 of 7
7 . Demonstrtion: Artificil Dielectric Courtesy of Hermnn A. Hus n Jmes R. Melcher. Use with permission. Prof. Mrkus Zhn Pge 7 of 7
8 Courtesy of Hermnn A. Hus n Jmes R. Melcher. Use with permission. v E= σs= E= v A q A q= σsa= v C= = v v i= ω C = R ( ) 3 o A R A C= =4πo s o s R=1.87 cm, s=8 cm, A= (0.4) m, =0.15m ω =π(50 Hz), R s =100 k Ω, =566 volts pek C=1.5 pf v 0 = ω CRs =(π) (50) (1.5 x 10-1 ) (10 5 ) 566 = volts pek Prof. Mrkus Zhn Pge 8 of 7
9 I. Plsm Conuction Moel (Clssicl) v m = q E m v p ν t n v p m = qe mνv t n p = n kt, p = nkt k=1.38 x 10-3 joules/ o K Boltzmnn Constnt A. Lonon Moel of Superconuctivity [ T 0, ν± 0] v v m = q E, m = qe t t J = q n v, J = q n v ( ) J qe v q n = ( q n v ) = q n = q n = E t t t m m ω p ( ) J qe v q n = ( q n v ) = q n = q n = E t t t m m ω p ω q n q n p =, ω p = m m (ω p = plsm frequency) For electrons: q - =1.6 x Couloms, m - =9.1 x kg n - =10 0 /m 3 1, = x10 frs/m o ω p ωp 10 f p = 9x10 π q n m 11 = 5.6 x10 Hz r/s Prof. Mrkus Zhn Pge 9 of 7
10 B. Drift-Diffusion Conuction [Neglect inerti] 0 v ( n k T) q k T m = q E m v v = E n ν t n m ν m ν n 0 v ( n k T) q k T m = q E m v v = E n ν t n mν mνn q n q k T J = q n v = E n m ν m ν q n q k T J = q n v = E n mν mν ρ =q n, ρ = q n J = ρ µ ED ρ J = ρ µ E D ρ µ q =, D = kt m ν m ν µ q kt =, D = mν m ν chrge moilities Moleculr Diffusion Coefficients D D kt = = µ µ q = therml voltge (5 T 300 o K) Einstein s Reltion Prof. Mrkus Zhn Pge 10 of 7
11 C. Drift-Diffusion Conuction Equilirium ( J = J = 0 ) J = 0 = ρ µ ED ρ = ρ µ Φ D ρ J = 0 = ρ µ E D ρ = ρ µ Φ D ρ D kt Φ = ρ = lnρ ρ µ q D kt Φ = ρ = lnρ ρ µ q ρ ρ q /kt = oe Φ ρ ρ q /kt = oe Φ Boltzmnn Distriutions ( =0 ) = ( =0 ) = o ρ Φ ρ Φ ρ [Potentil is zero when system is chrge neutrl] ( ρ ρ) ρo Φ Φ ρ ρ Φ q Φ q /kt q /kt o = = = e e = sinh kt (Poisson-Boltzmnn Eqution) Smll Potentil Approximtion: q Φ << 1 kt qφ sinh kt qφ kt ρ0q Φ Φ =0 kt Φ L Φ kt =0 ; L = ρ q o Deye Length Prof. Mrkus Zhn Pge 11 of 7
12 D. Cse Stuies 1. Plnr Sheet Φ Φ x/l =0 Φ =A1 e A e x L x/l B.C. Φ( x ± ) =0 ( x 0 ) = o Φ = ( x) Φ = x/l o e x > 0 < x/l o e x 0 Prof. Mrkus Zhn Pge 1 of 7
13 Φ E x = = x o e x/l x > 0 L o e x/l x < 0 L Ex ρ = = x e x 0 o x/l > L e x 0 o x/l < L σ ( = ) ( = ) s x=0 = Ex x 0 Ex x 0 = L o. Point Chrge (Deye Shieling) Φ 1 r r r Φ L 1 = r r r =0 Φ r ( Φ) E. Ohmic Conuction r Φ rφ r Φ =0 L r = A e A e r/l Φ 1 Q r = e 4π r r/l 0 r/l J = ρ µ ED ρ J = ρ µ E D ρ If chrge ensity grients smll, then ρ negligile ± ρ = ρ = ρ o J=J J = ρ µ ρ µ E= ρ µ µ E= σe o J= σ E (Ohm s Lw) σ = ohmic conuctivity Prof. Mrkus Zhn Pge 13 of 7
14 F. pn Junction Dioe Prof. Mrkus Zhn Pge 14 of 7
15 kt N Φ = Φ Φ = ln N A D n p q ni qn x qn x Φ ( x=0 ) = Φ p = Φn A p D n qnd x qna x n Φ = Φn Φp = p qn D xn qnd xn ND = ( xn xp) = 1 NA Prof. Mrkus Zhn Pge 15 of 7
16 II. Reltionship Between Resistnce n Cpcitnce In Uniform Mei Descrie y n σ. Di Ei qu S S C= = = v Eis Eis L Eis Eis v L L R= = = i Ji σ Ei S L S Eis Ei L L RC = = σ Ei Eis S L σ Check: Prllel Plte Electroes: l A R=, C= RC= σ A l σ Prof. Mrkus Zhn Pge 16 of 7
17 Coxil ln πl R=, C= RC= πσl ln σ Concentric Sphericl 1 1 R R 4 π 1 1 σ R R 1 R=, C= RC= 4 πσ 1 Prof. Mrkus Zhn Pge 17 of 7
18 III. Chnge Relxtion in Uniform Conuctors i ρ t u J u = 0 i E= ρ u J u = σ E ρu ρu σ σ i E = 0 ρu = 0 t t ρu τ = e σ = ielectric relxtion time ρ u t t τ ρu =0 ρu = ρ0 r, t=0 e τ e e IX. Demonstrtion Relxtion of Chrge on Prticle in Ohmic Conuctor Courtesy of Hermnn A. Hus n Jmes R. Melcher. Use with permission. Courtesy of Hermnn A. Hus n Jmes R. Melcher. Use with permission. Prof. Mrkus Zhn Pge 18 of 7
19 i i σ q q u J = σ E = = S S t q q =0 q=q t=0 e e τ = t τ e t τ ( e ) σ Prtilly Uniformly Chrge Sphere Courtesy of Krieger Pulishing. Use with permission. Prof. Mrkus Zhn Pge 19 of 7
20 ρ r < R ρ ( t=0 ) = Q = πr ρ 3 0 r > R 3 u T t τ ( t ) = e e r R = ρ ρ < τ σ u 0 1 e 0 r > R 1 r E r,t = t τe t τe ρ0 re Qre = 0 < r < R 3 4 π R Qe 4 π r t τe 0 Q 4 π r 3 1 R < r < R 1 r > R 1 σ ( r = R ) = E ( r = R ) E ( r = R ) su 0 r r t τe ( ) Q = 1 e 4 π R X. Self-Excite Wter Dynmos A. DC High oltge Genertion (Self-Excite) Prof. Mrkus Zhn Pge 0 of 7
21 Prof. Mrkus Zhn Pge 1 of 7
22 v st nc i v 1 = C v 1 = e nci = Cs t 1 1 v1 st nc i v = C v = e nci = Cs t 1 nci 1 1 Cs =0 nc i 1 Cs Det = 0 nci Cs nc C i ± =1 s= root lows up nci t C e Any perturtion grows exponentilly with time B. AC High oltge Self Excite Genertion v nc i v 1 = C ; v 1 = 1 e t v3 nc i v = C v = e t v1 nc i v 3 = C v 3 = 3 e t st st st nc i Cs nci Cs =0 Cs 0 nc i 3 et = 0 Prof. Mrkus Zhn Pge of 7
23 ( nc ) ( Cs ) =0 s= ( 1) 1 i nc C 3 3 i 3 s = nc C (exponentilly ecying solution) 1 i 13 1± 3j 1 = 1, ( ) nc C i s,3 = 1± 3 j (lows up exponentilly ecuse s rel >0 ; ut lso oscilltes t frequency s img 0) XI. Conservtion of Chrge Bounry Conition i ρ t u J u =0 i Ju ρu =0 S t ni J J σsu =0 t Prof. Mrkus Zhn Pge 3 of 7
24 XII. Mxwell s Cpcitor A. Generl Equtions E= _ E t i 0 < x < _ x E t i < x < 0 x E = v t =E t E t x x σsu ni J J =0 E ( t) E ( t) E ( t) E ( t ) σ σ =0 t t v t E ( t ) = E t v t v t σe ( t) σ E ( t) E ( t) E ( t) =0 t E σ σ v t v σ E ( t ) = t t Prof. Mrkus Zhn Pge 4 of 7
25 B. Step oltge: v ( t ) = u( t ) v = δ (n impulse) t Then ( t ) At t=0 E v = = t t t δ Integrte from t=0 - to t=0 0 E t t= 0 t= 0 δ t= 0 t t= 0 t= 0 ( = ) E t 0 = 0 t = E = t = E ( t = 0 ) = E ( t = 0 ) = For t > 0, v =0 t E σ σ σ E ( t ) = t σ t τ E ( t ) = A e ; τ = σ σ σ σ σ σ E ( t = 0 ) = A = A = σ σ σ σ σ t E ( t ) = ( 1 e ) e σ σ E t = E t τ t τ Prof. Mrkus Zhn Pge 5 of 7
26 σ ( t ) = E ( t) E ( t ) = E ( t) E ( t) su =E t ( σ σ ) ( σ σ ) = 1 e τ ( ) t C. Sinusoil Stey Stte: jω jω E t = Re E e jω E t = Re E e t t v t = Re e Conservtion of Chrge Interfcil Bounry Conition σ E ( t) σ E ( t) E ( t) E ( t ) = 0 t t E σ ω j E σ j ω = 0 E E = E E = E E σ jω σ j ω = 0 σ ω ( σ ω E ) σ ω j j = j = 0 E E = = jω σ jω σ ( σ ω ) ( σ ω ) j j σ = E E su ( ) σ σ ( σ ω ) ( σ ω ) = j j Prof. Mrkus Zhn Pge 6 of 7
27 D. Equivlent Circuit (Electroe Are A) I= j E A= j E A ( σ ω ) ( σ ω ) = R R R C jω 1 R C jω 1 R =, R = σ A σ A C =, C = A A Prof. Mrkus Zhn Pge 7 of 7
Note: Please use the actual date you accessed this material in your citation.
MIT OpenCourseWre http://ocw.mit.edu 6.641 Electromgnetic Fields, Forces, nd Motion, Spring 005 Plese use the following cittion formt: Mrkus Zhn, 6.641 Electromgnetic Fields, Forces, nd Motion, Spring
Διαβάστε περισσότεραNote: Please use the actual date you accessed this material in your citation.
MIT OpenCourseWre http://ocw.mit.edu 6.013/ESD.013J Electromgnetics nd Applictions, Fll 005 Plese use the following cittion formt: Mrkus Zhn, Erich Ippen, nd Dvid Stelin, 6.013/ESD.013J Electromgnetics
Διαβάστε περισσότεραCHAPTER (2) Electric Charges, Electric Charge Densities and Electric Field Intensity
CHAPTE () Electric Chrges, Electric Chrge Densities nd Electric Field Intensity Chrge Configurtion ) Point Chrge: The concept of the point chrge is used when the dimensions of n electric chrge distriution
Διαβάστε περισσότερα6.642 Continuum Electromechanics
MIT OpenCourseWre http://ocw.mit.eu 6.64 Continuum Electromechnics Fll 8 For informtion out citing these mterils or our Terms of Use, visit: http://ocw.mit.eu/terms. 6.64, Continuum Electromechnics rof.
Διαβάστε περισσότερα6.642, Continuum Electromechanics, Fall 2004 Prof. Markus Zahn Lecture 8: Electrohydrodynamic and Ferrohydrodynamic Instabilities
6.64, Continuum Electromechnics, Fll 4 Prof. Mrus Zhn Lecture 8: Electrohydrodynmic nd Ferrohydrodynmic Instilities I. Mgnetic Field Norml Instility Courtesy of MIT Press. Used with permission. A. Equilirium
Διαβάστε περισσότερα6.642 Continuum Electromechanics
MIT OpenCourseWre http://ocw.mit.edu 6.64 Continuum Electromechnics Fll 8 For informtion out citing these mterils or our Terms of Use, visit: http://ocw.mit.edu/terms. 6.64, Continuum Electromechnics,
Διαβάστε περισσότεραΠ 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
Διαβάστε περισσότεραl 0 l 2 l 1 l 1 l 1 l 2 l 2 l 1 l p λ λ µ R N l 2 R N l 2 2 = N x i l p p R N l p N p = ( x i p ) 1 p i=1 l 2 l p p = 2 l p l 1 R N l 1 i=1 x 2 i 1 = N x i i=1 l p p p R N l 0 0 = {i x i 0} R
Διαβάστε περισσότεραUniversity of Kentucky Department of Physics and Astronomy PHY 525: Solid State Physics II Fall 2000 Final Examination Solutions
University of Kentucy Deprtment of Pysics nd stronomy PHY : Solid Stte Pysics II Fll Finl Emintion Solutions Dte: December, (Mondy ime llowed: minutes. nswer ll questions.. Het cpcity of ferromgnets. (
Διαβάστε περισσότεραNote: 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 περισσότεραSecond 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
Διαβάστε περισσότεραVidyamandir Classes. Solutions to Revision Test Series - 2/ ACEG / IITJEE (Mathematics) = 2 centre = r. a
Per -.(D).() Vdymndr lsses Solutons to evson est Seres - / EG / JEE - (Mthemtcs) Let nd re dmetrcl ends of crcle Let nd D re dmetrcl ends of crcle Hence mnmum dstnce s. y + 4 + 4 6 Let verte (h, k) then
Διαβάστε περισσότεραCapacitors - Capacitance, Charge and Potential Difference
Capacitors - Capacitance, Charge and Potential Difference Capacitors store electric charge. This ability to store electric charge is known as capacitance. A simple capacitor consists of 2 parallel metal
Διαβάστε περισσότεραSelf and Mutual Inductances for Fundamental Harmonic in Synchronous Machine with Round Rotor (Cont.) Double Layer Lap Winding on Stator
Sel nd Mutul Inductnces or Fundmentl Hrmonc n Synchronous Mchne wth Round Rotor (Cont.) Double yer p Wndng on Sttor Round Rotor Feld Wndng (1) d xs s r n even r Dene S r s the number o rotor slots. Dene
Διαβάστε περισσότεραRectangular Polar Parametric
Hrold s AP Clculus BC Rectngulr Polr Prmetric Chet Sheet 15 Octoer 2017 Point Line Rectngulr Polr Prmetric f(x) = y (x, y) (, ) Slope-Intercept Form: y = mx + Point-Slope Form: y y 0 = m (x x 0 ) Generl
Διαβάστε περισσότεραElectromagnetic Waves I
Electromgnetic Wves I Jnury, 03. Derivtion of wve eqution of string. Derivtion of EM wve Eqution in time domin 3. Derivtion of the EM wve Eqution in phsor domin 4. The complex propgtion constnt 5. The
Διαβάστε περισσότεραF19MC2 Solutions 9 Complex Analysis
F9MC Solutions 9 Complex Analysis. (i) Let f(z) = eaz +z. Then f is ifferentiable except at z = ±i an so by Cauchy s Resiue Theorem e az z = πi[res(f,i)+res(f, i)]. +z C(,) Since + has zeros of orer at
Διαβάστε περισσότεραDETERMINATION OF DYNAMIC CHARACTERISTICS OF A 2DOF SYSTEM. by Zoran VARGA, Ms.C.E.
DETERMINATION OF DYNAMIC CHARACTERISTICS OF A 2DOF SYSTEM by Zoran VARGA, Ms.C.E. Euro-Apex B.V. 1990-2012 All Rights Reserved. The 2 DOF System Symbols m 1 =3m [kg] m 2 =8m m=10 [kg] l=2 [m] E=210000
Διαβάστε περισσότερα2-1. Power Transistors. Transistors for Audio Amplifier. Transistors for Humidifier. Darlington Transistors. Low VCE (sat) High hfe Transistors
Power Trnsistors -. Power Trnsistors Trnsistors for Audio Amplifier Trnsistors for Switch Mode Power Supply Trnsistors for Humidifier Trnsistor for Disply Horizontl Deflection Output Drlington Trnsistors
Διαβάστε περισσότεραReview-2 and Practice problems. sin 2 (x) cos 2 (x)(sin(x)dx) (1 cos 2 (x)) cos 2 (x)(sin(x)dx) let u = cos(x), du = sin(x)dx. = (1 u 2 )u 2 ( du)
. Trigonometric Integrls. ( sin m (x cos n (x Cse-: m is odd let u cos(x Exmple: sin 3 (x cos (x Review- nd Prctice problems sin 3 (x cos (x Cse-: n is odd let u sin(x Exmple: cos 5 (x cos 5 (x sin (x
Διαβάστε περισσότεραTheoretical Competition: 12 July 2011 Question 2 Page 1 of 2
Theoretcl Competton: July Queston ge of. Ηλεκτρισμένη Σαπουνόφουσκα Θεωρήστε μια σφαιρική σαπουνόφουσκα ακτίνας. Ο αέρας στο εσωτερικό της σαπουνόφουσκας έχει πυκνότητα ρ και θερμοκρασία T. Η σαπουνόφουσκα
Διαβάστε περισσότεραSpace-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
Διαβάστε περισσότεραDelhi Noida Bhopal Hyderabad Jaipur Lucknow Indore Pune Bhubaneswar Kolkata Patna Web: Ph:
Seria : 0. T_ME_(+B)_Strength of Materia_9078 Dehi Noida Bhopa Hyderabad Jaipur Luckno Indore une Bhubanesar Kokata atna Web: E-mai: info@madeeasy.in h: 0-56 CLSS TEST 08-9 MECHNICL ENGINEERING Subject
Διαβάστε περισσότεραΑπόκριση σε Μοναδιαία Ωστική Δύναμη (Unit Impulse) Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο. Απόστολος Σ.
Απόκριση σε Δυνάμεις Αυθαίρετα Μεταβαλλόμενες με το Χρόνο The time integral of a force is referred to as impulse, is determined by and is obtained from: Newton s 2 nd Law of motion states that the action
Διαβάστε περισσότεραRadiation Stress Concerned with the force (or momentum flux) exerted on the right hand side of a plane by water on the left hand side of the plane.
upplement on Radiation tress and Wave etup/et down Radiation tress oncerned wit te force (or momentum flu) eerted on te rit and side of a plane water on te left and side of te plane. plane z "Radiation
Διαβάστε περισσότερα5 Ι ^ο 3 X X X. go > 'α. ο. o f Ο > = S 3. > 3 w»a. *= < ^> ^ o,2 l g f ^ 2-3 ο. χ χ. > ω. m > ο ο ο - * * ^r 2 =>^ 3^ =5 b Ο? UJ. > ο ο.
728!. -θ-cr " -;. '. UW -,2 =*- Os Os rsi Tf co co Os r4 Ι. C Ι m. Ι? U Ι. Ι os ν ) ϋ. Q- o,2 l g f 2-2 CT= ν**? 1? «δ - * * 5 Ι -ΐ j s a* " 'g cn" w *" " 1 cog 'S=o " 1= 2 5 ν s/ O / 0Q Ε!θ Ρ h o."o.
Διαβάστε περισσότεραΑ 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
Διαβάστε περισσότεραPhys460.nb Solution for the t-dependent Schrodinger s equation How did we find the solution? (not required)
Phys460.nb 81 ψ n (t) is still the (same) eigenstate of H But for tdependent H. The answer is NO. 5.5.5. Solution for the tdependent Schrodinger s equation If we assume that at time t 0, the electron starts
Διαβάστε περισσότεραSolutions to Exercise Sheet 5
Solutions to Eercise Sheet 5 jacques@ucsd.edu. Let X and Y be random variables with joint pdf f(, y) = 3y( + y) where and y. Determine each of the following probabilities. Solutions. a. P (X ). b. P (X
Διαβάστε περισσότεραb. Use the parametrization from (a) to compute the area of S a as S a ds. Be sure to substitute for ds!
MTH U341 urface Integrals, tokes theorem, the divergence theorem To be turned in Wed., Dec. 1. 1. Let be the sphere of radius a, x 2 + y 2 + z 2 a 2. a. Use spherical coordinates (with ρ a) to parametrize.
Διαβάστε περισσότεραMatrices 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
Διαβάστε περισσότεραME 365: SYSTEMS, MEASUREMENTS, AND CONTROL (SMAC) I
ME 365: SYSTEMS, MEASUREMENTS, AND CONTROL SMAC) I Dynamicresponseof 2 nd ordersystem Prof.SongZhangMEG088) Solutions to ODEs Forann@thorderLTIsystem a n yn) + a n 1 y n 1) ++ a 1 "y + a 0 y = b m u m)
Διαβάστε περισσότεραHomework 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
Διαβάστε περισσότεραJesse Maassen and Mark Lundstrom Purdue University November 25, 2013
Notes on Average Scattering imes and Hall Factors Jesse Maassen and Mar Lundstrom Purdue University November 5, 13 I. Introduction 1 II. Solution of the BE 1 III. Exercises: Woring out average scattering
Διαβάστε περισσότεραECE 222b Applied Electromagnetics Notes Set 4c
ECE 222b Applied Electromgnetics Notes Set 4c Instructor: Prof. Vitliy Lomkin Deprtment of Electricl nd Computer Engineering University of Cliforni, Sn Diego 1 Cylindricl Wve Functions (1) Helmoholt eqution:
Διαβάστε περισσότεραIntegrals in cylindrical, spherical coordinates (Sect. 15.7)
Integrals in clindrical, spherical coordinates (Sect. 5.7 Integration in spherical coordinates. Review: Clindrical coordinates. Spherical coordinates in space. Triple integral in spherical coordinates.
Διαβάστε περισσότεραMock 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
Διαβάστε περισσότεραThe Probabilistic Method - Probabilistic Techniques. Lecture 7: The Janson Inequality
The Probabilistic Method - Probabilistic Techniques Lecture 7: The Janson Inequality Sotiris Nikoletseas Associate Professor Computer Engineering and Informatics Department 2014-2015 Sotiris Nikoletseas,
Διαβάστε περισσότεραthe total number of electrons passing through the lamp.
1. A 12 V 36 W lamp is lit to normal brightness using a 12 V car battery of negligible internal resistance. The lamp is switched on for one hour (3600 s). For the time of 1 hour, calculate (i) the energy
Διαβάστε περισσότεραMagnetically Coupled Circuits
DR. GYURCSEK ISTVÁN Magnetically Coupled Circuits Sources and additional materials (recommended) Dr. Gyurcsek Dr. Elmer: Theories in Electric Circuits, GlobeEdit, 2016, ISBN:978-3-330-71341-3 Ch. Alexander,
Διαβάστε περισσότεραSCHOOL 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)
Διαβάστε περισσότεραHandbook of Electrochemical Impedance Spectroscopy
Handbook of Electrochemical Impedance Spectroscopy Im Z u c T u c T Re Z CIRCUITS made of RESISTORS and INDUCTORS ER@SE/LEPMI J.-P. Diard, B. Le Gorrec, C. Montella Hosted by Bio-Logic @ www.bio-logic.info
Διαβάστε περισσότερα2. 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
Διαβάστε περισσότεραSolutions 3. February 2, Apply composite Simpson s rule with m = 1, 2, 4 panels to approximate the integrals:
s Februry 2, 216 1 Exercise 5.2. Apply composite Simpson s rule with m = 1, 2, 4 pnels to pproximte the integrls: () x 2 dx = 1 π/2, (b) cos(x) dx = 1, (c) e x dx = e 1, nd report the errors. () f(x) =
Διαβάστε περισσότεραSpherical Coordinates
Spherical Coordinates MATH 311, Calculus III J. Robert Buchanan Department of Mathematics Fall 2011 Spherical Coordinates Another means of locating points in three-dimensional space is known as the spherical
Διαβάστε περισσότεραο 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 περισσότεραECE 308 SIGNALS AND SYSTEMS FALL 2017 Answers to selected problems on prior years examinations
ECE 308 SIGNALS AND SYSTEMS FALL 07 Answers to selected problems on prior years examinations Answers to problems on Midterm Examination #, Spring 009. x(t) = r(t + ) r(t ) u(t ) r(t ) + r(t 3) + u(t +
Διαβάστε περισσότεραLecture 21: Scattering and FGR
ECE-656: Fall 009 Lecture : Scattering and FGR Professor Mark Lundstrom Electrical and Computer Engineering Purdue University, West Lafayette, IN USA Review: characteristic times τ ( p), (, ) == S p p
Διαβάστε περισσότεραChapter 5. Exercise Solutions. Microelectronics: Circuit Analysis and Design, 4 th edition Chapter 5 EX5.1 = 1 I. = βi EX EX5.3 = = I V EX5.
Microelectronics: ircuit nalysis and Design, 4 th edition hapter 5 y D.. Neamen xercise Solutions xercise Solutions X5. ( β ).0 β 4. β 40. 0.0085 hapter 5 β 40. α 0.999 β 4..0 0.0085.95 X5. O 00 O n 3
Διαβάστε περισσότεραCHAPTER 25 SOLVING EQUATIONS BY ITERATIVE METHODS
CHAPTER 5 SOLVING EQUATIONS BY ITERATIVE METHODS EXERCISE 104 Page 8 1. Find the positive root of the equation x + 3x 5 = 0, correct to 3 significant figures, using the method of bisection. Let f(x) =
Διαβάστε περισσότερα( )( ) La Salle College Form Six Mock Examination 2013 Mathematics Compulsory Part Paper 2 Solution
L Slle ollege Form Si Mock Emintion 0 Mthemtics ompulsor Prt Pper Solution 6 D 6 D 6 6 D D 7 D 7 7 7 8 8 8 8 D 9 9 D 9 D 9 D 5 0 5 0 5 0 5 0 D 5. = + + = + = = = + = =. D The selling price = $ ( 5 + 00)
Διαβάστε περισσότεραAquinas College. Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET
Aquinas College Edexcel Mathematical formulae and statistics tables DO NOT WRITE ON THIS BOOKLET Pearson Edexcel Level 3 Advanced Subsidiary and Advanced GCE in Mathematics and Further Mathematics Mathematical
Διαβάστε περισσότεραRS306 High Speed Fuse for Semiconductor Protection
Product Information Standard square body fuse, comply with GB13539/IEC60269/UL-248/VDE-0636 Protection: ar (GB\IEC), short circuit or backup Rated : 250-4000VAC Very low I 2 t/high current-limiting/high
Διαβάστε περισσότεραIf ABC is any oblique triangle with sides a, b, and c, the following equations are valid. 2bc. (a) a 2 b 2 c 2 2bc cos A or cos A b2 c 2 a 2.
etion 6. Lw of osines 59 etion 6. Lw of osines If is ny oblique tringle with sides, b, nd, the following equtions re vlid. () b b os or os b b (b) b os or os b () b b os or os b b You should be ble to
Διαβάστε περισσότεραElectrical Specifications at T AMB =25 C DC VOLTS (V) MAXIMUM POWER (dbm) DYNAMIC RANGE IP3 (dbm) (db) Output (1 db Comp.) at 2 f U. Typ.
Surface Mount Monolithic Amplifiers High Directivity, 50Ω, 0.5 to 5.9 GHz Features 3V & 5V operation micro-miniature size.1"x.1" no external biasing circuit required internal DC blocking at RF input &
Διαβάστε περισσότεραBounding Nonsplitting Enumeration Degrees
Bounding Nonsplitting Enumeration Degrees Thomas F. Kent Andrea Sorbi Università degli Studi di Siena Italia July 18, 2007 Goal: Introduce a form of Σ 0 2-permitting for the enumeration degrees. Till now,
Διαβάστε περισσότεραQUICKTRONIC PROFESSIONAL QTP5
osram.com QUICKTRONIC PROFESSIONA QTP5 ECG for T5/ 16mm, T8/ 26mm, DUUX fluorescent lamps QTP5 i.e. UMIUX T5 HO ES 01 Product Features: Up to 100.000 hours lifetime 1 amp start with optimized filament
Διαβάστε περισσότεραDesign Method of Ball Mill by Discrete Element Method
Design Method of Ball Mill by Discrete Element Method Sumitomo Chemical Co., Ltd. Process & Production Technology Center Makio KIMURA Masayuki NARUMI Tomonari KOBAYASHI The grinding rate of gibbsite in
Διαβάστε περισσότεραCable Systems - Postive/Negative Seq Impedance
Cable Systems - Postive/Negative Seq Impedance Nomenclature: GMD GMR - geometrical mead distance between conductors; depends on construction of the T-line or cable feeder - geometric mean raduius of conductor
Διαβάστε περισσότεραReview of Single-Phase AC Circuits
Single-Phase AC Circuits in a DC Circuit In a DC circuit, we deal with one type of power. P = I I W = t2 t 1 Pdt = P(t 2 t 1 ) = P t (J) DC CIRCUIT in an AC Circuit Instantaneous : p(t) v(t)i(t) i(t)=i
Διαβάστε περισσότεραSpectrum Representation (5A) Young Won Lim 11/3/16
Spectrum (5A) Copyright (c) 2009-2016 Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any later
Διαβάστε περισσότεραΘΕΩΡΙΑ ΤΩΝ ΗΜΙΑΓΩΓΩΝ ΔΕΥΤΕΡΗ ΕΝΟΤΗΤΑ ΟΜΟΓΕΝΕΙΣ ΗΜΙΑΓΩΓΟΙ ΦΑΙΝΟΜΕΝΑ ΜΕΤΑΦΟΡΑΣ
ΘΕΩΡΙΑ ΤΩΝ ΗΜΙΑΓΩΓΩΝ ΔΕΥΤΕΡΗ ΕΝΟΤΗΤΑ ΟΜΟΓΕΝΕΙΣ ΗΜΙΑΓΩΓΟΙ ΦΑΙΝΟΜΕΝΑ ΜΕΤΑΦΟΡΑΣ 1. Μηχανισμοί σκέδασης των φορέων (ηλεκτρόνια οπές) 2. Ηλεκτρική Αγωγιμότητα 3. Ολίσθηση φορέων (ρεύμα ολίσθησης) 4. Διάχυση
Διαβάστε περισσότεραDissertation for the degree philosophiae doctor (PhD) at the University of Bergen
Dissertation for the degree philosophiae doctor (PhD) at the University of Bergen Dissertation date: GF F GF F SLE GF F D Ĉ = C { } Ĉ \ D D D = {z : z < 1} f : D D D D = D D, D = D D f f : D D
Διαβάστε περισσότεραExample 1: THE ELECTRIC DIPOLE
Example 1: THE ELECTRIC DIPOLE 1 The Electic Dipole: z + P + θ d _ Φ = Q 4πε + Q = Q 4πε 4πε 1 + 1 2 The Electic Dipole: d + _ z + Law of Cosines: θ A B α C A 2 = B 2 + C 2 2ABcosα P ± = 2 ( + d ) 2 2
Διαβάστε περισσότεραDurbin-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
Διαβάστε περισσότεραRectangular Polar Parametric
Harold s Precalculus Rectangular Polar Parametric Cheat Sheet 15 October 2017 Point Line Rectangular Polar Parametric f(x) = y (x, y) (a, b) Slope-Intercept Form: y = mx + b Point-Slope Form: y y 0 = m
Διαβάστε περισσότεραEquations. BSU Math 275 sec 002,003 Fall 2018 (Ultman) Final Exam Notes 1. du dv. FTLI : f (B) f (A) = f dr. F dr = Green s Theorem : y da
BSU Math 275 sec 002,003 Fall 2018 (Ultman) Final Exam Notes 1 Equations r(t) = x(t) î + y(t) ĵ + z(t) k r = r (t) t s = r = r (t) t r(u, v) = x(u, v) î + y(u, v) ĵ + z(u, v) k S = ( ( ) r r u r v = u
Διαβάστε περισσότεραWestfalia Bedienungsanleitung. Nr
Westfalia Bedienungsanleitung Nr. 108230 Erich Schäfer KG Tel. 02737/5010 Seite 1/8 RATED VALUES STARTING VALUES EFF 2 MOTOR OUTPUT SPEED CURRENT MOMENT CURRENT TORQUE TYPE I A / I N M A / M N Mk/ Mn %
Διαβάστε περισσότεραReminders: linear functions
Reminders: linear functions Let U and V be vector spaces over the same field F. Definition A function f : U V is linear if for every u 1, u 2 U, f (u 1 + u 2 ) = f (u 1 ) + f (u 2 ), and for every u U
Διαβάστε περισσότεραECE 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[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
Διαβάστε περισσότεραw o = R 1 p. (1) R = p =. = 1
Πανεπιστήµιο Κρήτης - Τµήµα Επιστήµης Υπολογιστών ΗΥ-570: Στατιστική Επεξεργασία Σήµατος 205 ιδάσκων : Α. Μουχτάρης Τριτη Σειρά Ασκήσεων Λύσεις Ασκηση 3. 5.2 (a) From the Wiener-Hopf equation we have:
Διαβάστε περισσότεραWritten Examination. Antennas and Propagation (AA ) April 26, 2017.
Written Examination Antennas and Propagation (AA. 6-7) April 6, 7. Problem ( points) Let us consider a wire antenna as in Fig. characterized by a z-oriented linear filamentary current I(z) = I cos(kz)ẑ
Διαβάστε περισσότεραPart III - Pricing A Down-And-Out Call Option
Part III - Pricing A Down-And-Out Call Option Gary Schurman MBE, CFA March 202 In Part I we examined the reflection principle and a scaled random walk in discrete time and then extended the reflection
Διαβάστε περισσότεραwave energy Superposition of linear plane progressive waves Marine Hydrodynamics Lecture Oblique Plane Waves:
3.0 Marine Hydrodynamics, Fall 004 Lecture 0 Copyriht c 004 MIT - Department of Ocean Enineerin, All rihts reserved. 3.0 - Marine Hydrodynamics Lecture 0 Free-surface waves: wave enery linear superposition,
Διαβάστε περισσότεραAffine 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
Διαβάστε περισσότεραSampling Basics (1B) Young Won Lim 9/21/13
Sampling Basics (1B) Copyright (c) 2009-2013 Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any
Διαβάστε περισσότεραFerrite Chip Beads For Automotive Use
FETURES RUGGED CONSTRUCTION IN STNDRD EI SIZES EC Q-200 QULIFIED EFFECTIVE EM/RFI SUPPRESSION UP TO 1GHz CURRENT RTINGS UP TO 2.2 MPS SHRP ND HIGH IMPEDNCES VILLE OPERTING TEMPERTURE RNGE: -55 C TO +125C
Διαβάστε περισσότερα0.635mm Pitch Board to Board Docking Connector. Lead-Free Compliance
.635mm Pitch Board to Board Docking Connector Lead-Free Compliance MINIDOCK SERIES MINIDOCK SERIES Features Specifications Application.635mm Pitch Connector protected by Diecasted Zinc Alloy Metal Shell
Διαβάστε περισσότεραDerivation 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
Διαβάστε περισσότεραSecond Order Partial Differential Equations
Chapter 7 Second Order Partial Differential Equations 7.1 Introduction A second order linear PDE in two independent variables (x, y Ω can be written as A(x, y u x + B(x, y u xy + C(x, y u u u + D(x, y
Διαβάστε περισσότεραΣΗΜΑΤΑ ΔΙΑΚΡΙΤΟΥ ΧΡΟΝΟΥ
ΣΗΜΑΤΑ ΔΙΑΚΡΙΤΟΥ ΧΡΟΝΟΥ y t x Α. ΣΚΟΔΡΑΣ ΣΗΜΑΤΑ ΚΑΙ ΣΥΣΤΗΜΑΤΑ ΙΙ (22Y603) ΕΝΟΤΗΤΑ 1 ΔΙΑΛΕΞΗ 2 ΔΙΑΦΑΝΕΙΑ 1 ΤΥΠΟΙ ΣΗΜΑΤΩΝ Analog: Continuous Time & Continuous Amplitude Sampled: Discrete Time & Continuous
Διαβάστε περισσότεραMATH423 String Theory Solutions 4. = 0 τ = f(s). (1) dτ ds = dxµ dτ f (s) (2) dτ 2 [f (s)] 2 + dxµ. dτ f (s) (3)
1. MATH43 String Theory Solutions 4 x = 0 τ = fs). 1) = = f s) ) x = x [f s)] + f s) 3) equation of motion is x = 0 if an only if f s) = 0 i.e. fs) = As + B with A, B constants. i.e. allowe reparametrisations
Διαβάστε περισσότεραStrain gauge and rosettes
Strain gauge and rosettes Introduction A strain gauge is a device which is used to measure strain (deformation) on an object subjected to forces. Strain can be measured using various types of devices classified
Διαβάστε περισσότεραAdvanced Subsidiary Unit 1: Understanding and Written Response
Write your name here Surname Other names Edexcel GE entre Number andidate Number Greek dvanced Subsidiary Unit 1: Understanding and Written Response Thursday 16 May 2013 Morning Time: 2 hours 45 minutes
Διαβάστε περισσότεραPhysics/Astronomy 226, Problem set 5, Due 2/17 Solutions
Physics/Astronomy 6, Problem set 5, Due /17 Solutions Reding: Ch. 3, strt Ch. 4 1. Prove tht R λναβ + R λαβν + R λβνα = 0. Solution: We cn evlute this in locl inertil frme, in which the Christoffel symbols
Διαβάστε περισσότεραTerminal Contact UL Insulation Designation (provided with) style form system approval Flux tight
eatures A miniature PCB Power Relay. form A contact configuration with quick terminal type. 5KV dielectric strength, K surge voltage between coils to contact. Ideal for high rating Home Appliances of heating
Διαβάστε περισσότεραSolving 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 περισσότερα10.7 Performance of Second-Order System (Unit Step Response)
Lecture Notes on Control Systems/D. Ghose/0 57 0.7 Performance of Second-Order System (Unit Step Response) Consider the second order system a ÿ + a ẏ + a 0 y = b 0 r So, Y (s) R(s) = b 0 a s + a s + a
Διαβάστε περισσότεραPhysique 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 περισσότεραQ 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 περισσότεραu = 0 u = ϕ t + Π) = 0 t + Π = C(t) C(t) C(t) = K K C(t) ϕ = ϕ 1 + C(t) dt Kt 2 ϕ = 0
u = (u, v, w) ω ω = u = 0 ϕ u u = ϕ u = 0 ϕ 2 ϕ = 0 u t = u ω 1 ρ Π + ν 2 u Π = p + (1/2)ρ u 2 + ρgz ω = 0 ( ϕ t + Π) = 0 ϕ t + Π = C(t) C(t) C(t) = K K C(t) ϕ = ϕ 1 + C(t) dt Kt C(t) ϕ ϕ 1 ϕ = ϕ 1 p ρ
Διαβάστε περισσότεραProblem 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 περισσότεραAnswers to practice exercises
Answers to practice exercises Chapter Exercise (Page 5). 9 kg 2. 479 mm. 66 4. 565 5. 225 6. 26 7. 07,70 8. 4 9. 487 0. 70872. $5, Exercise 2 (Page 6). (a) 468 (b) 868 2. (a) 827 (b) 458. (a) 86 kg (b)
Διαβάστε περισσότερα= (2)det (1)det ( 5)det 1 2. u
www.maths.gr, Ενδεικτικές Λύσεις ης Εργασίας ΦΥΕ4 έτους -. Οι Λύσεις είναι για την βοήθεια των φοιτητών, σε ΘΕΜΑ ο 5 6 4 6 4 5 det 4 5 6 ()det ()det ()det 8 9 7 9 7 8 7 8 9 ()( ) ()( 6 ) ()( ) 5 4 4 det
Διαβάστε περισσότεραMicroelectronic Circuit Design Third Edition - Part I Solutions to Exercises
Microelectronic Circuit Design Third Edition - Part I Solutions to Exercises Page 11 CHAPTER 1 V LSB 5.1V 10 bits 5.1V 104bits 5.00 mv V 5.1V MSB.560V 1100010001 9 + 8 + 4 + 0 785 10 V O 786 5.00mV or
Διαβάστε περισσότεραSurface Mount Multilayer Chip Capacitors for Commodity Solutions
Surface Mount Multilayer Chip Capacitors for Commodity Solutions Below tables are test procedures and requirements unless specified in detail datasheet. 1) Visual and mechanical 2) Capacitance 3) Q/DF
Διαβάστε περισσότεραAppendix A. Curvilinear coordinates. A.1 Lamé coefficients. Consider set of equations. ξ i = ξ i (x 1,x 2,x 3 ), i = 1,2,3
Appendix A Curvilinear coordinates A. Lamé coefficients Consider set of equations ξ i = ξ i x,x 2,x 3, i =,2,3 where ξ,ξ 2,ξ 3 independent, single-valued and continuous x,x 2,x 3 : coordinates of point
Διαβάστε περισσότεραParametrized Surfaces
Parametrized Surfaces Recall from our unit on vector-valued functions at the beginning of the semester that an R 3 -valued function c(t) in one parameter is a mapping of the form c : I R 3 where I is some
Διαβάστε περισσότεραW τ R W j N H = 2 F obj b q N F aug F obj b q Ψ F aug Ψ ( ) ϱ t + + p = 0 = 0 Ω f = Γ Γ b ϱ = (, t) = (, t) Ω f Γ b ( ) ϱ t + + p = V max 4 3 2 1 0-1 -2-3 -4-4 -3-2 -1 0 1 2 3 4 x 4 x 1 V mn V max
Διαβάστε περισσότερα