Errata for Problems and Answers in Wave Optics (PM216)

Size: px
Start display at page:

Download "Errata for Problems and Answers in Wave Optics (PM216)"

Transcription

1 Contents Errata for Problems and Answers n Wave Opts (PM6) Frst Prntng Seton 3 Seton 35 Seton Seton ttle should be Lnear polarzers and retarder plates Seton ttle should be Indued optal ansotropy Seton ttle should be Interferene of monohromat and mutually oherent lght Chapter Problem In the frst lne, F should not be n tals Problem 3 In fgure E should be n tals Problem In the seond lne, a laser beam s desrbed should be a laser beam n ar (n = ) s desrbed Chapter Problem The supersrpt ndes P and S should be lowerase Problem In the frst lne, parallel beam should be ollmated beam Problem 9 The supersrpt ndes P and S should be lowerase Problem The supersrpt ndes P and S should be lowerase Problem 6 The supersrpt ndes P and S should be lowerase Problem 7 The supersrpt ndes P and S should be lowerase Problem 9 In the frst lne, should be max Chapter 3 Seton 3 Seton ttle should be Lnear polarzers and retarder plates Problem 38 In the fourth lne, 5 deg should be deg Problem 33 In the frst lne, A beam of natural lght should be A beam of lnearly polarzed lght Seton 35 Seton ttle should be Indued optal ansotropy

2 Chapter Seton Seton ttle should be Interferene of monohromat and mutually oherent lght Problem 5 Pont P should not be n tals Problem 6 In the seond lne, at one pont should be at one pont P Problem 8 Pont P should not be n tals Problem 8 In the seond lne, 63 should be 63 m Problem 9 In the fourth lne, dstanes should be dstanes z Problem Pont P should not be n tals Problem 6 In the seond lne, 63 nm should be 63 nm Problem 7 In the fourth lne, photodode should be photodetetor Problem 8 In the fgure, L and L should be n tals Problem 3 Pont soure S should not be n tals Problem 35 In the thrd lne, nsert a omma between optal axs and z Problem 37 In the thrd lne, P mm Hg should be P mm Hg In the last lne, B MPa - should be B Pa - Problem Pont soure S should not be n tals Problem 5 In the frst lne, parallel should be ollmated Problem 9 In the frst and seond lnes, quas-parallel should be quas-ollmated Problem 5 In the ffth lne, quas-parallel should be quas-ollmated Problem 5 In the frst lne, quas-parallel should be quas-ollmated 3 In the fourth lne, rad/nm should be 3 rad/nm Problem 6 In the seond to last lne, a spae should be nserted between S and Problem 6 In the sxth lne, quas-parallel should be quas-ollmated Problem 63 In the last lne, 85 should be 93 с

3 Problem 6 The text should read as follows: Determne the longtudnal oherene length L of an optal feld from a spatally noherent lght soure n the bak foal plane F ' of a olletng lens L and n the plane of the real mage of the soure ( S ') The soure S s loated at dstane z 6 mm from the front foal plane F of the lens L and radates lght wth mean wavelength 55 μm and frequeny spetrum wdth μm The transverse sze of the soure s D mm, the dameter of the lens aperture s Da mm, and the foal length of the lens s f 8 mm Problem 67 Replae the fgure wth the followng: s Problem 7 Add the followng sentene after the seond sentene: Dspersng prsm P s nstalled n the output arm of the nterferometer, and the spetrum of lght I at the nterferometer output s observed In the fgure, the dspersng prsm should be labeled P Problem 7 In the last lne, I should be 5 I Problem 7 In the last sentene, f the perod of ntensty osllaton I z s 6 μm should be f the perod z of ntensty osllaton I z s z 3μm Problem 73 In the last lne, 6 should be 6 nm Problem 7 In the thrd lne, z 5mm should be z 5 m Problem 75 In the seond lne, z should be d Problem 78 In the seond to last sentene, z m should be z m Problem 8 In the thrd lne, h 6mm should be h 6m In the seventh lne, 6 5nm should be 6 5m Problem 83 In the seond to last sentene, from maxmum to mnmum should be from maxmum to the next maxmum Problem 8 Replae the fgure wth the followng:

4 Problem 85 The seond sentene should read as follows: Plot the transmsson oeffent T h of the nterferometer n the normal dreton (along the optal axs of the lens) versus the thkness h of the ar gap between the plates for the radaton wth two wave omponents of equal ntensty wth wavelengths 56nm and 56 nm n the range of the ar gap thkness values h μm and h μm Chapter 5 Problem 5 In the fourth lne, b 98 mm should be b 98 mm Problem 55 In the fourth lne, a 5 should be a 5 m Problem 57 In the frst lne, the rad nterval r m should be the rad r m Problem 58 In the seond lne, f 8 should be f 8 m Problem 57 In the last lne, s Ix, y I should be s Ix, y I and a z In the fgure, varable D should be a Problem 58 In the last lne, s Ix, y I should be s Ix, y I and d f Problem 59 In the frst lne, before ntegral, ( x should be x ( z z under ntegral, ( x x should be ( x x z z Problem 56 In the thrd lne, the dameter should be the dameter d Problem 53 In the frst lne, The maxmal pupl dameter should be The pupl dameter Problem 53 In the frst lne, the resoluton of should be the lnear resoluton Problem 538 In the fgure, should be x of

5 Problem 5 In the seond lne, m should be m Problem 55 In the frst lne, the resoluton of a gratng should be the resoluton R of a gratng Problem 55 In the seond lne, on a plane, refletng dffraton gratng should be on a refletng dffraton gratng Chapter 6 Problem 6 In the seond to last lne, 3 should be 3 Problem 66 In the ffth lne, and + should be + and The sxth lne, v 6 mm/s should be v 6 mm/s Problem 68 In the frst lne, A parallel beam should be A ollmated beam In the last two lnes, may be onsdered a soure of seondary dffrated lght beams should be may be onsdered as a seondary soure of dffrated lght beams Problem 6 In the fgure, V should be v Chapter 7 (Answers) Chapter 8 3 v 89 m/s 8 should be v 897 m/s x xsn should be x x = x os α/λ should be = x os(α)/λ fz = ω os γ/π should be fz = ω os(γ)/π should be 7 I( ) 5E should be I( ) ~ E 8 I( ) E should be I( ) ~ E 9 I( ) should be I () ~ ln / should be ln E 3 I ( ) should be I( ) ~ E 6 sn

6 33 E ox E oy should be E x E y 35 E E should be E E ox oy x y 37 I n v should be I 5 n v x 3 should be x 6 3 should be 39 Chapter 5 6 deg should be 5 6 deg; orthogonal to the ndene plane 6 59 deg should be 59 deg should be p and p, p are ampltude refleton and transmsson oeffents should be s and p, s are ampltude refleton and transmsson oeffents 3 R 75, T 95 should be R 7, T 96 7 should be 3 7 T 97 should be T 93 6 The answer should read as follows: tg p sn n n n nos, tg os n sn s n sn n os n tg n sn n, 7 s 6 rad should be 67 lowerase 9 max μm should be max rad, 5 8deg 3 The answer should read as follows: E E expz n sn n, deg Chapter 3 3 v should be v o rad, and supersrpt ndes P and S should be

7 3 u should be u o 8 8 ue 5 m/s should be ue 86 m/s deg should be 7 deg 37 d 7 mm should be d 8 mm I os os sn sn sn sn os n n d 8 mw/mm 38 I o e deg should be deg should be I ( t) I sn t, I ( t) I os t should be I ( t) I sn t, I ( t) I os t o e o e 33 I ( ) os sn os os o t I t t t t, I ( ) sn e t I t should be I ( ) os sn o t I t t, I ( ) 5sn e t I t Chapter 5 I 7 W/m should be I 9 W/m 8 d n sn should be d n sn r 3mm should be r mm V should be V 8 5 sn should be sn 6 6 μm, V 5 should be 69 μm, V nm should be 85 nm 5μm, N should be 3 μm, N 3 7 μm should be 6 6m l mm should be l 5 mm D mm should be D mm

8 5 I II should be I II The followng equatons should be added: Er,t E exp t r, E r,t E exp t r, I ~ E E I I EE os t r, f ; 6 f 5MHz should be f v 8 m/s should be v 55 3 should be 35 8 n both formulae should be should be 5 should be 5 3 mm should be 59 mm 5 l mm should be l mm 5 l mm should be l mm 56 x, у z z MHz z z m/s sn ax sn bx should be ax z bx z sn ax sn by x, у ax z by z 6 с 37 μm should be с 37 μm () 5μm, (d) 9 μm should be () с μm, (d) ñ ñ3 с 3 63 z 6 μm, L μm should be z 5 μm, L 7 6 μm 6 9 should be 7 μm L 3μm should be L 39μm L 37 μm should be L 8 μm 65 A spae should be added between E(t) and I 7 I should be 5I 7 d 3 6 mm should be D 3 6 mm 78 z z nd mm should be z z nd 33 mm μm

9 z 79 6 mm; z 9 3mm should be D D D f 6 mm; z 9 3mm D D D 8 deg should be arse 8 T 55 nm should be T nm should be 3 59nm 83 h 5 μm should be h 5 μm 8 R mm should be R 8 mm m Chapter 5 53 b 3 mm should be z 6 55mm m 5 b 7mm, b 3 mm should be b mm, b 8 3mm 58 r mm should be r 3 mm 5 m m should be R R m r r f m should be f m m 5 r 9 mm should be r 9 mm 55 x 67 mm, x 33mm, x mm should be x 67 mm, x 33mm, x3 mm 56 a 9 should be a Add the followng: x mm 59 exp should be exp z z 53 d z 5 6mm should be d z 5 5mm 56 d 7 8mm should be d 7 7 mm 58 d 5 8mm should be d mm 59 R 6 lnes/mm should be R lnes/mm

10 53 x 3 μm, 6 armn, x 5mm should be x 6 μm, 9 armn, x mm d d 535 In the denomnator, sn should be sn sn 536 x mm should be x 7 5 m 7 should be m 9 mm 5 arsn sn 3deg should be should be R mn 555 deg should be deg 557 Add a omma after deg Chapter should be 6 66 ( ) 8 μm, ( ) 8 μm, 8 arsn sn 3deg ( ) μm should be 8 ( ) μm 6 L L should be 8 63 N N T should be T n L d dt L d dt 6 6 rad should be 56 rad 65 f 5 Hz should be f 5 Hz

Title: Radiative transitions and spectral broadening

Title: Radiative transitions and spectral broadening Lecture 6 Ttle: Radatve transtons and spectral broadenng Objectves The spectral lnes emtted by atomc vapors at moderate temperature and pressure show the wavelength spread around the central frequency.

More information

Introduction to Antennas & Arrays

Introduction to Antennas & Arrays Introducton to Antennas & Arrays Antenna transton regon (structure) between guded eaves (.e. coaxal cable) and free space waves. On transmsson, antenna accepts energy from TL and radates t nto space. J.D.

More information

Introductory Optomechanical Engineering. 2) First order optics

Introductory Optomechanical Engineering. 2) First order optics Introductory Optomechancal Engneerng 2) Frst order optcs Moton of optcal elements affects the optcal performance? 1. by movng the mage 2. hgher order thngs (aberratons) The frst order effects are most

More information

Implementation of the Matrix Method

Implementation of the Matrix Method Computatonal Photoncs, Prof. Thomas Pertsch, Abbe School of Photoncs, FSU Jena Computatonal Photoncs Semnar 0 Implementaton of the Matr Method calculaton of the transfer matr calculaton of reflecton and

More information

GEL 446: Applied Environmental Geology

GEL 446: Applied Environmental Geology GE 446: ppled Envronmental Geology Watershed Delneaton and Geomorphology Watershed Geomorphology Watersheds are fundamental geospatal unts that provde a physal and oneptual framewor wdely used by sentsts,

More information

425. Calculation of stresses in the coating of a vibrating beam

425. Calculation of stresses in the coating of a vibrating beam 45. CALCULAION OF SRESSES IN HE COAING OF A VIBRAING BEAM. 45. Calulaton of stresses n the oatng of a vbratng beam M. Ragulsks,a, V. Kravčenken,b, K. Plkauskas,, R. Maskelunas,a, L. Zubavčus,b, P. Paškevčus,d

More information

ˆ (0.10 m) E ( N m /C ) 36 ˆj ( j C m)

ˆ (0.10 m) E ( N m /C ) 36 ˆj ( j C m) 7.. = = 3 = 4 = 5. The electrc feld s constant everywhere between the plates. Ths s ndcated by the electrc feld vectors, whch are all the same length and n the same drecton. 7.5. Model: The dstances to

More information

Implementation of the Matrix Method

Implementation of the Matrix Method Computatonal Photoncs, Prof. Thomas Pertsch, Abbe School of Photoncs, FSU Jena Computatonal Photoncs Semnar 0 Implementaton of the Matr Method calculaton of the transfer matr calculaton of reflecton and

More information

ELG4179: Wireless Communication Fundamentals S.Loyka. Frequency-Selective and Time-Varying Channels

ELG4179: Wireless Communication Fundamentals S.Loyka. Frequency-Selective and Time-Varying Channels Frequeny-Seletve and Tme-Varyng Channels Ampltude flutuatons are not the only effet. Wreless hannel an be frequeny seletve (.e. not flat) and tmevaryng. Frequeny flat/frequeny-seletve hannels Frequeny

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION do: 0.08/nature09 I. Resonant absorpton of XUV pulses n Kr + usng the reduced densty matrx approach The quantum beats nvestgated n ths paper are the result of nterference between two exctaton paths of

More information

Microlens quality assessment using the Extended Nijboer-Zernike diffraction theory

Microlens quality assessment using the Extended Nijboer-Zernike diffraction theory Mcrolens qualty assessment usng the Extended Njboer-Zernke dracton theory J.J.M. Braat, S. van Haver, S.F. Perera Delt Unversty o Technology Department o Imagng Scence and Technology Optcs Research Group

More information

СOMPENSATION OF LASER BEAM WAVEFRONT ABERRATIONS BASED ON ATMOSPHERIC BACKSCATTERING. Viktor Banakh, Igor Smalikho

СOMPENSATION OF LASER BEAM WAVEFRONT ABERRATIONS BASED ON ATMOSPHERIC BACKSCATTERING. Viktor Banakh, Igor Smalikho Wave Propagaton Lab СOMPENSATION OF LASER BEAM WAVEFRONT ABERRATIONS BASED ON ATMOSPHERIC BACKSCATTERING Vktor Banakh, Igor Smalkho Insttute of Atmospherc Optcs of the Russan Academy of Scences Wave Propagaton

More information

Example

Example Chapter Example.- ------------------------------------------------------------------------------ sold slab of 5.5 wt% agar gel at 78 o K s.6 mm thk and ontans a unform onentraton of urea of. kmol/m 3.

More information

ˆ A = A 0 e i (k r ωt) + c.c. ( ωt) e ikr. + c.c. k,j

ˆ A = A 0 e i (k r ωt) + c.c. ( ωt) e ikr. + c.c. k,j p. Supp. 9- Suppleent to Rate of Absorpton and Stulated Esson Here are a ouple of ore detaled dervatons: Let s look a lttle ore arefully at the rate of absorpton w k ndued by an sotrop, broadband lght

More information

A Theorem of Mass Being Derived From Electrical Standing Waves (As Applied to Jean Louis Naudin's Test)

A Theorem of Mass Being Derived From Electrical Standing Waves (As Applied to Jean Louis Naudin's Test) A Theorem of Mass Beng Derved From Eletral Standng Waves (As Appled to Jean Lous Naudn's Test) - by - Jerry E Bayles Aprl 4, 000 Ths paper formalzes a onept presented n my book, "Eletrogravtaton As A Unfed

More information

Introduction to Molecular Spectroscopy

Introduction to Molecular Spectroscopy Chem 5.6, Fall 004 Leture #36 Page Introduton to Moleular Spetrosopy QM s essental for understandng moleular spetra and spetrosopy. In ths leture we delneate some features of NMR as an ntrodutory example

More information

APPENDIX 2 FITTING A STRAIGHT LINE TO OBSERVATIONS

APPENDIX 2 FITTING A STRAIGHT LINE TO OBSERVATIONS Unversty of Oulu Student Laboratory n Physcs Laboratory Exercses n Physcs 1 1 APPEDIX FITTIG A STRAIGHT LIE TO OBSERVATIOS In the physcal measurements we often make a seres of measurements of the dependent

More information

Implementation of the Matrix Method

Implementation of the Matrix Method Computatonal Photoncs, Summer Term 01, Abbe School of Photoncs, FSU Jena, Prof. Thomas Pertsch Computatonal Photoncs Semnar 03, 7 May 01 Implementaton of the Matr Method calculaton of the transfer matr

More information

Math1110 (Spring 2009) Prelim 3 - Solutions

Math1110 (Spring 2009) Prelim 3 - Solutions Math 1110 (Sprng 2009) Solutons to Prelm 3 (04/21/2009) 1 Queston 1. (16 ponts) Short answer. Math1110 (Sprng 2009) Prelm 3 - Solutons x a 1 (a) (4 ponts) Please evaluate lm, where a and b are postve numbers.

More information

Channel model. Free space propagation

Channel model. Free space propagation //06 Channel model Free spae rado propagaton Terrestral propagaton - refleton, dffraton, satterng arge-sale fadng Empral models Small-sale fadng Nose and nterferene Wreless Systems 06 Free spae propagaton

More information

kq r 2 2kQ 2kQ (A) (B) (C) (D)

kq r 2 2kQ 2kQ (A) (B) (C) (D) PHYS 1202W MULTIPL CHOIC QUSTIONS QUIZ #1 Answer the followng multple choce questons on the bubble sheet. Choose the best answer, 5 pts each. MC1 An uncharged metal sphere wll (A) be repelled by a charged

More information

arxiv: v2 [physics.optics] 17 Mar 2016

arxiv: v2 [physics.optics] 17 Mar 2016 Pulse-ompresson ghost magng ldar va oherent deteton arxv:1603.04143v2 [physs.opts] 17 Mar 2016 Chenjn Deng, Wenln Gong and Shensheng Han Key Laboratory for Quantum Opts and Center for Cold Atom Physs,

More information

APPENDIX F A DISPLACEMENT-BASED BEAM ELEMENT WITH SHEAR DEFORMATIONS. Never use a Cubic Function Approximation for a Non-Prismatic Beam

APPENDIX F A DISPLACEMENT-BASED BEAM ELEMENT WITH SHEAR DEFORMATIONS. Never use a Cubic Function Approximation for a Non-Prismatic Beam APPENDIX F A DISPACEMENT-BASED BEAM EEMENT WITH SHEAR DEFORMATIONS Never use a Cubc Functon Approxmaton for a Non-Prsmatc Beam F. INTRODUCTION { XE "Shearng Deformatons" }In ths appendx a unque development

More information

Module 2. Random Processes. Version 2 ECE IIT, Kharagpur

Module 2. Random Processes. Version 2 ECE IIT, Kharagpur Module Random Processes Lesson 6 Functons of Random Varables After readng ths lesson, ou wll learn about cdf of functon of a random varable. Formula for determnng the pdf of a random varable. Let, X be

More information

Calculation of time complexity (3%)

Calculation of time complexity (3%) Problem 1. (30%) Calculaton of tme complexty (3%) Gven n ctes, usng exhaust search to see every result takes O(n!). Calculaton of tme needed to solve the problem (2%) 40 ctes:40! dfferent tours 40 add

More information

Matrix Mechanics Exercises Using Polarized Light

Matrix Mechanics Exercises Using Polarized Light Matrx Mechancs Exercses Usng Polarzed Lght Frank Roux Egenstates and operators are provded for a seres of matrx mechancs exercses nvolvng polarzed lght. Egenstate for a -polarzed lght: Θ( θ) ( ) smplfy

More information

Green s function for the wave equation

Green s function for the wave equation Green s funtion for the wave equation Non relativisti ase 1 The wave equations In the Lorentz Gauge, the wave equations for the potentials in Lorentz Gauge Gaussian units are: r 2 A 1 2 A 2 t = 4π 2 j

More information

The Schrödinger Equation

The Schrödinger Equation Chapter 1 The Schrödnger Equaton 1.1 (a) F; () T; (c) T. 1. (a) Ephoton = hν = hc/ λ =(6.66 1 34 J s)(.998 1 8 m/s)/(164 1 9 m) = 1.867 1 19 J. () E = (5 1 6 J/s)( 1 8 s) =.1 J = n(1.867 1 19 J) and n

More information

Geometrical Optics Mirrors and Prisms

Geometrical Optics Mirrors and Prisms Phy 322 Lecture 4 Chapter 5 Geometrcal Optc Mrror and Prm Optcal bench http://webphyc.davdon.edu/applet/optc4/default.html Mrror Ancent bronze mrror Hubble telecope mrror Lqud mercury mrror Planar mrror

More information

DOAEstimationforCoherentSourcesinBeamspace UsingSpatialSmoothing

DOAEstimationforCoherentSourcesinBeamspace UsingSpatialSmoothing DOAEstmatonorCoherentSouresneamspae UsngSpatalSmoothng YnYang,ChunruWan,ChaoSun,QngWang ShooloEletralandEletronEngneerng NanangehnologalUnverst,Sngapore,639798 InsttuteoAoustEngneerng NorthwesternPoltehnalUnverst,X

More information

Boundaries, Near-field Optics

Boundaries, Near-field Optics Boundares, Near-feld Optcs Fve boundary condtons at an nterface Fresnel Equatons : Transmsson and Reflecton Coeffcents Transmttance and Reflectance Brewster s condton a consequence of Impedance matchng

More information

Circuits II EE221. Instructor: Kevin D. Donohue. Instantaneous, Average, RMS, and Apparent Power, and, Maximum Power Transfer, and Power Factors

Circuits II EE221. Instructor: Kevin D. Donohue. Instantaneous, Average, RMS, and Apparent Power, and, Maximum Power Transfer, and Power Factors Crcuts II EE1 Unt 3 Instructor: Ken D. Donohue Instantaneous, Aerage, RMS, and Apparent Power, and, Maxmum Power pp ransfer, and Power Factors Power Defntons/Unts: Work s n unts of newton-meters or joules

More information

e a = 12.4 i a = 13.5i h a = xi + yj 3 a Let r a = 25cos(20) i + 25sin(20) j b = 15cos(55) i + 15sin(55) j

e a = 12.4 i a = 13.5i h a = xi + yj 3 a Let r a = 25cos(20) i + 25sin(20) j b = 15cos(55) i + 15sin(55) j Vetors MC Qld-3 49 Chapter 3 Vetors Exerse 3A Revew of vetors a d e f e a x + y omponent: x a os(θ 6 os(80 + 39 6 os(9.4 omponent: y a sn(θ 6 sn(9 0. a.4 0. f a x + y omponent: x a os(θ 5 os( 5 3.6 omponent:

More information

is the calculated value of the dependent variable at point i. The best parameters have values that minimize the squares of the errors

is the calculated value of the dependent variable at point i. The best parameters have values that minimize the squares of the errors Multple Lnear and Polynomal Regresson wth Statstcal Analyss Gven a set of data of measured (or observed) values of a dependent varable: y versus n ndependent varables x 1, x, x n, multple lnear regresson

More information

ERRATA For the book A farewell to Entropy, Statistical Thermodynamics Based on Information

ERRATA For the book A farewell to Entropy, Statistical Thermodynamics Based on Information ERRAA For the book A farewell to Entropy, Statstcal hermodynamcs Based on Informaton Chapter : Page, lnes 4-6 of paragraph should be revsed to: hs defnton s vald wthout any reference to the atomc consttuency

More information

Tensor Analysis. For orthogonal curvilinear coordinates, ˆ ˆ (98) Expanding the derivative, we have, ˆ. h q. . h q h q

Tensor Analysis. For orthogonal curvilinear coordinates, ˆ ˆ (98) Expanding the derivative, we have, ˆ. h q. . h q h q For orthogonal curvlnear coordnates, eˆ grad a a= ( aˆ ˆ e). h q (98) Expandng the dervatve, we have, eˆ aˆ ˆ e a= ˆ ˆ a h e + q q 1 aˆ ˆ ˆ a e = ee ˆˆ ˆ + e. h q h q Now expandng eˆ / q (some of the detals

More information

Course Electron Microprobe Analysis

Course Electron Microprobe Analysis Course 12.141 Electron Mcroprobe Analyss THE ELECTROMAGNETIC SPECTRUM Electron Probe X-ray Mcro-Analyss A) quanttatve chemcal analyss of solds: Be to U 1 mcrometer resoluton up to 10 ppm B) hgh-resoluton

More information

Module 14: THE INTEGRAL Exploring Calculus

Module 14: THE INTEGRAL Exploring Calculus Module 14: THE INTEGRAL Explorng Calculus Part I Approxmatons and the Defnte Integral It was known n the 1600s before the calculus was developed that the area of an rregularly shaped regon could be approxmated

More information

A Theorem of Mass Being Derived From Electrical Standing Waves (As Applied to Jean Louis Naudin's Test)

A Theorem of Mass Being Derived From Electrical Standing Waves (As Applied to Jean Louis Naudin's Test) A Theorem of Mass Beng Derved From Eletral Standng Waves (As Appled to Jean Lous Naudn's Test) - by - Jerry E Bayles Aprl 5, 000 Ths Analyss Proposes The Neessary Changes Requred For A Workng Test Ths

More information

Derivation of results in section 8-9 of Quantum Mechanics and Path Integrals by Richard P. Feynman and Albert R. Hibbs (McGraw-Hill, New York, 1965).

Derivation of results in section 8-9 of Quantum Mechanics and Path Integrals by Richard P. Feynman and Albert R. Hibbs (McGraw-Hill, New York, 1965). The forced harmonc oscllator: Feynman-Hbbs secton 8-9 Dan Styer, Oberln College Physcs Department, Oberln, Oho 4474 17 October 5 Dervaton of results n secton 8-9 of Quantum Mechancs and Path Integrals

More information

EXAM INFORMATION. Harmonic Oscillator. Anharmonic Oscillator 1 ~ 1. Rigid Rotor

EXAM INFORMATION. Harmonic Oscillator. Anharmonic Oscillator 1 ~ 1. Rigid Rotor EXAM INFORMATION Harmonc Oscllator Hamltonan: H d dx 1 kx Energy Levels: 1 k mm 1 En n n 0,1,, c m m 1 Anharmonc Oscllator Energy Levels: E n 1 ~ 1 n hc n hcx ~ e n 0,1,,... Rgd Rotor Quantum Numbers:

More information

Statistics MINITAB - Lab 2

Statistics MINITAB - Lab 2 Statstcs 20080 MINITAB - Lab 2 1. Smple Lnear Regresson In smple lnear regresson we attempt to model a lnear relatonshp between two varables wth a straght lne and make statstcal nferences concernng that

More information

Class: Life-Science Subject: Physics

Class: Life-Science Subject: Physics Class: Lfe-Scence Subject: Physcs Frst year (6 pts): Graphc desgn of an energy exchange A partcle (B) of ass =g oves on an nclned plane of an nclned angle α = 3 relatve to the horzontal. We want to study

More information

( ) = ( ) + ( 0) ) ( )

( ) = ( ) + ( 0) ) ( ) EETOMAGNETI OMPATIBIITY HANDBOOK 1 hapter 9: Transent Behavor n the Tme Doman 9.1 Desgn a crcut usng reasonable values for the components that s capable of provdng a tme delay of 100 ms to a dgtal sgnal.

More information

Supplementary Information for Observation of Parity-Time Symmetry in. Optically Induced Atomic Lattices

Supplementary Information for Observation of Parity-Time Symmetry in. Optically Induced Atomic Lattices Supplementary Informaton for Observaton of Party-Tme Symmetry n Optcally Induced Atomc attces Zhaoyang Zhang 1,, Yq Zhang, Jteng Sheng 3, u Yang 1, 4, Mohammad-Al Mr 5, Demetros N. Chrstodouldes 5, Bng

More information

Georgia Tech PHYS 6124 Mathematical Methods of Physics I

Georgia Tech PHYS 6124 Mathematical Methods of Physics I Georga Tech PHYS 624 Mathematcal Methods of Physcs I Instructor: Predrag Cvtanovć Fall semester 202 Homework Set #7 due October 30 202 == show all your work for maxmum credt == put labels ttle legends

More information

( T) Blackbody Radiation. S hν. hν exp kt MODEL

( T) Blackbody Radiation. S hν. hν exp kt MODEL Let us use nsten's approach to relate gan and spontaneous emsson. ccordng to Plank:.The probablty o radaton takng place rom a black body decreased as the requency o the radaton ncreased.. The black body

More information

ERRATA. COMPUTER-AIDED ANALYSIS OF MECHANICAL SYSTEMS Parviz E. Nikravesh Prentice-Hall, (Corrections as of November 2014)

ERRATA. COMPUTER-AIDED ANALYSIS OF MECHANICAL SYSTEMS Parviz E. Nikravesh Prentice-Hall, (Corrections as of November 2014) ERRATA COMPUTER-AIDED ANALYSIS OF MECHANICAL SYSTEMS Parvz E. Nkravesh Prentce-Hall, 1988 (Correctons as of November 2014 Address to an error s gven n the frst column by the page number and n the second

More information

Homework Math 180: Introduction to GR Temple-Winter (3) Summarize the article:

Homework Math 180: Introduction to GR Temple-Winter (3) Summarize the article: Homework Math 80: Introduton to GR Temple-Wnter 208 (3) Summarze the artle: https://www.udas.edu/news/dongwthout-dark-energy/ (4) Assume only the transformaton laws for etors. Let X P = a = a α y = Y α

More information

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity Week3, Chapter 4 Moton n Two Dmensons Lecture Quz A partcle confned to moton along the x axs moves wth constant acceleraton from x =.0 m to x = 8.0 m durng a 1-s tme nterval. The velocty of the partcle

More information

CHAPTER 13. Exercises. E13.1 The emitter current is given by the Shockley equation:

CHAPTER 13. Exercises. E13.1 The emitter current is given by the Shockley equation: HPT 3 xercses 3. The emtter current s gen by the Shockley equaton: S exp VT For operaton wth, we hae exp >> S >>, and we can wrte VT S exp VT Solng for, we hae 3. 0 6ln 78.4 mv 0 0.784 5 4.86 V VT ln 4

More information

2010 vds-3d. Professor Kyongsu Yi. Vehicle Dynamics and Control Laboratory

2010 vds-3d. Professor Kyongsu Yi. Vehicle Dynamics and Control Laboratory 3D Dnamcs 2010 vds-3d Professor Kongsu Y 2010 VDCL Vehcle Dnamcs and Control Laborator 1 Knetcs of Rgd Bodes n Three Dmensons ma G Translatonal Dnamc Equaton of Rgd Bod (Newton Equaton F ma G Rotatonal

More information

PHYS 1101 Practice problem set 12, Chapter 32: 21, 22, 24, 57, 61, 83 Chapter 33: 7, 12, 32, 38, 44, 49, 76

PHYS 1101 Practice problem set 12, Chapter 32: 21, 22, 24, 57, 61, 83 Chapter 33: 7, 12, 32, 38, 44, 49, 76 PHYS 1101 Practce problem set 1, Chapter 3: 1,, 4, 57, 61, 83 Chapter 33: 7, 1, 3, 38, 44, 49, 76 3.1. Vsualze: Please reer to Fgure Ex3.1. Solve: Because B s n the same drecton as the ntegraton path s

More information

Four Bar Linkages in Two Dimensions. A link has fixed length and is joined to other links and also possibly to a fixed point.

Four Bar Linkages in Two Dimensions. A link has fixed length and is joined to other links and also possibly to a fixed point. Four bar lnkages 1 Four Bar Lnkages n Two Dmensons lnk has fed length and s oned to other lnks and also possbly to a fed pont. The relatve velocty of end B wth regard to s gven by V B = ω r y v B B = +y

More information

COMPLEX NUMBERS AND QUADRATIC EQUATIONS

COMPLEX NUMBERS AND QUADRATIC EQUATIONS COMPLEX NUMBERS AND QUADRATIC EQUATIONS INTRODUCTION We know that x 0 for all x R e the square of a real number (whether postve, negatve or ero) s non-negatve Hence the equatons x, x, x + 7 0 etc are not

More information

PHYSICS - CLUTCH 1E CH 28: INDUCTION AND INDUCTANCE.

PHYSICS - CLUTCH 1E CH 28: INDUCTION AND INDUCTANCE. !! www.clutchprep.com CONCEPT: ELECTROMAGNETIC INDUCTION A col of wre wth a VOLTAGE across each end wll have a current n t - Wre doesn t HAVE to have voltage source, voltage can be INDUCED V Common ways

More information

1. Definition of a Polynomial

1. Definition of a Polynomial 1. Definition of a Polynomial What is a polynomial? A polynomial P(x) is an algebraic expression of the form Degree P(x) = a n x n + a n 1 x n 1 + a n 2 x n 2 + + a 3 x 3 + a 2 x 2 + a 1 x + a 0 Leading

More information

n α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0

n α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0 MODULE 2 Topcs: Lnear ndependence, bass and dmenson We have seen that f n a set of vectors one vector s a lnear combnaton of the remanng vectors n the set then the span of the set s unchanged f that vector

More information

Perron Vectors of an Irreducible Nonnegative Interval Matrix

Perron Vectors of an Irreducible Nonnegative Interval Matrix Perron Vectors of an Irreducble Nonnegatve Interval Matrx Jr Rohn August 4 2005 Abstract As s well known an rreducble nonnegatve matrx possesses a unquely determned Perron vector. As the man result of

More information

8.1 Arc Length. What is the length of a curve? How can we approximate it? We could do it following the pattern we ve used before

8.1 Arc Length. What is the length of a curve? How can we approximate it? We could do it following the pattern we ve used before .1 Arc Length hat s the length of a curve? How can we approxmate t? e could do t followng the pattern we ve used before Use a sequence of ncreasngly short segments to approxmate the curve: As the segments

More information

Summary ELECTROMAGNETIC FIELDS AT THE WORKPLACES. System layout: exposure to magnetic field only. Quasi-static dosimetric analysis: system layout

Summary ELECTROMAGNETIC FIELDS AT THE WORKPLACES. System layout: exposure to magnetic field only. Quasi-static dosimetric analysis: system layout Internatonal Workshop on LCTROMGNTIC FILDS T TH WORKPLCS 5-7 September 5 Warszawa POLND 3d approah to numeral dosmetr n quas-stat ondtons: problems and eample of solutons Dr. Nola Zoppett - IFC-CNR, Florene,

More information

π e ax2 dx = x 2 e ax2 dx or x 3 e ax2 dx = 1 x 4 e ax2 dx = 3 π 8a 5/2 (a) We are considering the Maxwell velocity distribution function: 2πτ/m

π e ax2 dx = x 2 e ax2 dx or x 3 e ax2 dx = 1 x 4 e ax2 dx = 3 π 8a 5/2 (a) We are considering the Maxwell velocity distribution function: 2πτ/m Homework Solutons Problem In solvng ths problem, we wll need to calculate some moments of the Gaussan dstrbuton. The brute-force method s to ntegrate by parts but there s a nce trck. The followng ntegrals

More information

Narayana IIT Academy INDIA Sec: Sr. IIT_IZ JEE-MAIN Date: Time: 07:30 AM to 10:30 AM Cumulative Test Max.Marks: 360

Narayana IIT Academy INDIA Sec: Sr. IIT_IZ JEE-MAIN Date: Time: 07:30 AM to 10:30 AM Cumulative Test Max.Marks: 360 INDIA Sec: Sr. IIT_IZ JEE-MAIN Date: 11-0-18 Tme: 07:30 AM to 10:30 AM Cumulatve Test Max.Marks: 360 KEY SHEET PHYSICS 1 4 1 3 4 5 4 6 3 7 8 3 9 10 1 11 3 1 4 13 14 15 1 16 4 17 1 18 19 1 0 1 1 3 3 3 4

More information

ENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15

ENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15 NGN 40 ynamcs and Vbratons Homework # 7 ue: Frday, Aprl 15 1. Consder a concal hostng drum used n the mnng ndustry to host a mass up/down. A cable of dameter d has the mass connected at one end and s wound/unwound

More information

Turbulence classification of load data by the frequency and severity of wind gusts. Oscar Moñux, DEWI GmbH Kevin Bleibler, DEWI GmbH

Turbulence classification of load data by the frequency and severity of wind gusts. Oscar Moñux, DEWI GmbH Kevin Bleibler, DEWI GmbH Turbulence classfcaton of load data by the frequency and severty of wnd gusts Introducton Oscar Moñux, DEWI GmbH Kevn Blebler, DEWI GmbH Durng the wnd turbne developng process, one of the most mportant

More information

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.mt.edu 6.13/ESD.13J Electromagnetcs and Applcatons, Fall 5 Please use the followng ctaton format: Markus Zahn, Erch Ippen, and Davd Staeln, 6.13/ESD.13J Electromagnetcs and

More information

Physics 3 (PHYF144) Chap 2: Heat and the First Law of Thermodynamics System. Quantity Positive Negative

Physics 3 (PHYF144) Chap 2: Heat and the First Law of Thermodynamics System. Quantity Positive Negative Physcs (PHYF hap : Heat and the Frst aw of hermodynamcs -. Work and Heat n hermodynamc Processes A thermodynamc system s a system that may exchange energy wth ts surroundngs by means of heat and work.

More information

SPECTRAL RECONSTRUCTION IN CASE OF DIFFERENT ILLUMINANTS

SPECTRAL RECONSTRUCTION IN CASE OF DIFFERENT ILLUMINANTS AALS of Faulty Engneerng Hunedoara Internatonal Journal of Engneerng Tome XIV [6] Fasule [February] ISS: 584-665 [prnt; onlne] ISS: 584-673 [CD-Rom; onlne] a free-aess multdsplnary publaton of the Faulty

More information

2010 Black Engineering Building, Department of Mechanical Engineering. Iowa State University, Ames, IA, 50011

2010 Black Engineering Building, Department of Mechanical Engineering. Iowa State University, Ames, IA, 50011 Interface Energy Couplng between -tungsten Nanoflm and Few-layered Graphene Meng Han a, Pengyu Yuan a, Jng Lu a, Shuyao S b, Xaolong Zhao b, Yanan Yue c, Xnwe Wang a,*, Xangheng Xao b,* a 2010 Black Engneerng

More information

PHYSICS - CLUTCH CH 28: INDUCTION AND INDUCTANCE.

PHYSICS - CLUTCH CH 28: INDUCTION AND INDUCTANCE. !! www.clutchprep.com CONCEPT: ELECTROMAGNETIC INDUCTION A col of wre wth a VOLTAGE across each end wll have a current n t - Wre doesn t HAVE to have voltage source, voltage can be INDUCED V Common ways

More information

Maximum Likelihood Estimation of Binary Dependent Variables Models: Probit and Logit. 1. General Formulation of Binary Dependent Variables Models

Maximum Likelihood Estimation of Binary Dependent Variables Models: Probit and Logit. 1. General Formulation of Binary Dependent Variables Models ECO 452 -- OE 4: Probt and Logt Models ECO 452 -- OE 4 Maxmum Lkelhood Estmaton of Bnary Dependent Varables Models: Probt and Logt hs note demonstrates how to formulate bnary dependent varables models

More information

Chapter 4. Velocity analysis

Chapter 4. Velocity analysis 1 Chapter 4 Velocty analyss Introducton The objectve of velocty analyss s to determne the sesmc veloctes of layers n the subsurface. Sesmc veloctes are used n many processng and nterpretaton stages such

More information

THE CURRENT BALANCE Physics 258/259

THE CURRENT BALANCE Physics 258/259 DSH 1988, 005 THE CURRENT BALANCE Physcs 58/59 The tme average force between two parallel conductors carryng an alternatng current s measured by balancng ths force aganst the gravtatonal force on a set

More information

Robot Modeling and Kinematics Errata R. Manseur. List of errors and typos reported as of 4/1/2007:

Robot Modeling and Kinematics Errata R. Manseur. List of errors and typos reported as of 4/1/2007: Robot Modelng and Knematcs Errata R. Manseur. Lst of errors and typos reported as of 4//7:. Fle CF4.wrl mentoned on page 45 s not on the CD. Fle ZYZ_Sm.wrl mentoned on page 67 s not on the CD. 3. Pg. 43.

More information

ECE 6602 Assignment 6 Solutions for Spring 2003

ECE 6602 Assignment 6 Solutions for Spring 2003 ECE 660 Assgnment 6 Solutons for Sprng 003 1. Wrte a matlab ode to do the modulaton and demodulaton for a bnary FSK usng a) oherent detetor and b) a nonoherent detetor. Modfy the programs that are posted

More information

2016 Wiley. Study Session 2: Ethical and Professional Standards Application

2016 Wiley. Study Session 2: Ethical and Professional Standards Application 6 Wley Study Sesson : Ethcal and Professonal Standards Applcaton LESSON : CORRECTION ANALYSIS Readng 9: Correlaton and Regresson LOS 9a: Calculate and nterpret a sample covarance and a sample correlaton

More information

Phase Transition in Collective Motion

Phase Transition in Collective Motion Phase Transton n Colletve Moton Hefe Hu May 4, 2008 Abstrat There has been a hgh nterest n studyng the olletve behavor of organsms n reent years. When the densty of lvng systems s nreased, a phase transton

More information

PHY2049 Exam 2 solutions Fall 2016 Solution:

PHY2049 Exam 2 solutions Fall 2016 Solution: PHY2049 Exam 2 solutons Fall 2016 General strategy: Fnd two resstors, one par at a tme, that are connected ether n SERIES or n PARALLEL; replace these two resstors wth one of an equvalent resstance. Now

More information

SYNCHROTRON X-RAY QUASI-FAR-FIELD IMAGING ON LUMINESCENT LITHIUM FLUORIDE DETECTORS

SYNCHROTRON X-RAY QUASI-FAR-FIELD IMAGING ON LUMINESCENT LITHIUM FLUORIDE DETECTORS ENRI CO NI CHELATTI D pa r t ment ofus oneet e nol og eperl as ur ez z anu l ea r e D v s onet e nol og ef s heperl as ur ez z ael asal ut e Labor at or om r oenanos t r ut t ur eperl afot on a Cent r

More information

Electrical Circuits II (ECE233b)

Electrical Circuits II (ECE233b) Electrcal Crcuts (ECE33b SteadyState Power Analyss Anests Dounas The Unersty of Western Ontaro Faculty of Engneerng Scence SteadyState Power Analyss (t AC crcut: The steady state oltage and current can

More information

( ) + + REFLECTION FROM A METALLIC SURFACE

( ) + + REFLECTION FROM A METALLIC SURFACE REFLECTION FROM A METALLIC SURFACE For a metallc medum the delectrc functon and the ndex of refracton are complex valued functons. Ths s also the case for semconductors and nsulators n certan frequency

More information

Grundkonzepte der Optik Sommersemester 2014

Grundkonzepte der Optik Sommersemester 2014 Srpt "Grundkonepte der Optk", FSU Jena, Prof. T. Pertsh, GdO3_Srpt_4-6-s.dox Grundkonepte der Optk Sommersemester 4 Prof. Thomas Pertsh Abbe Shool of Photons, Fredrh-Shller-Unverstät Jena Table of ontent.

More information

The equation of motion of a dynamical system is given by a set of differential equations. That is (1)

The equation of motion of a dynamical system is given by a set of differential equations. That is (1) Dynamcal Systems Many engneerng and natural systems are dynamcal systems. For example a pendulum s a dynamcal system. State l The state of the dynamcal system specfes t condtons. For a pendulum n the absence

More information

Analytical Chemistry Calibration Curve Handout

Analytical Chemistry Calibration Curve Handout I. Quck-and Drty Excel Tutoral Analytcal Chemstry Calbraton Curve Handout For those of you wth lttle experence wth Excel, I ve provded some key technques that should help you use the program both for problem

More information

= = = (a) Use the MATLAB command rref to solve the system. (b) Let A be the coefficient matrix and B be the right-hand side of the system.

= = = (a) Use the MATLAB command rref to solve the system. (b) Let A be the coefficient matrix and B be the right-hand side of the system. Chapter Matlab Exercses Chapter Matlab Exercses. Consder the lnear system of Example n Secton.. x x x y z y y z (a) Use the MATLAB command rref to solve the system. (b) Let A be the coeffcent matrx and

More information

Field and Wave Electromagnetic. Chapter.4

Field and Wave Electromagnetic. Chapter.4 Fel an Wave Electromagnetc Chapter.4 Soluton of electrostatc Problems Posson s s an Laplace s Equatons D = ρ E = E = V D = ε E : Two funamental equatons for electrostatc problem Where, V s scalar electrc

More information

Lecture Notes on Linear Regression

Lecture Notes on Linear Regression Lecture Notes on Lnear Regresson Feng L fl@sdueducn Shandong Unversty, Chna Lnear Regresson Problem In regresson problem, we am at predct a contnuous target value gven an nput feature vector We assume

More information

5.04, Principles of Inorganic Chemistry II MIT Department of Chemistry Lecture 32: Vibrational Spectroscopy and the IR

5.04, Principles of Inorganic Chemistry II MIT Department of Chemistry Lecture 32: Vibrational Spectroscopy and the IR 5.0, Prncples of Inorganc Chemstry II MIT Department of Chemstry Lecture 3: Vbratonal Spectroscopy and the IR Vbratonal spectroscopy s confned to the 00-5000 cm - spectral regon. The absorpton of a photon

More information

Learning Theory: Lecture Notes

Learning Theory: Lecture Notes Learnng Theory: Lecture Notes Lecturer: Kamalka Chaudhur Scrbe: Qush Wang October 27, 2012 1 The Agnostc PAC Model Recall that one of the constrants of the PAC model s that the data dstrbuton has to be

More information

ERRATUM Joseph John Bevelacqua Contemporary Health Physics 2nd, updated and enlarged edition

ERRATUM Joseph John Bevelacqua Contemporary Health Physics 2nd, updated and enlarged edition ERRATUM Joseph John Bevelacqua Contemporary Health Physcs 2nd, updated and enlarged edton Page XXIII, Contents, Solutons for Chapter 7 Add the entry: Scenaro 7.4 504 Page 14, 2 nd Lne, Scenaro 1.14, Item

More information

Finite Wings Steady, incompressible flow

Finite Wings Steady, incompressible flow Steady, ncompressble flow Geometrc propertes of a wng - Fnte thckness much smaller than the span and the chord - Defnton of wng geometry: a) Planform (varaton of chord and sweep angle) b) Secton/Arfol

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION do:10.1038/nature09901 Supplementary Informaton: Sample propertes The nvestgated sample was a 30 nm Gd 25 Fe 65.6 Co 9.4 thn flm deposted by magnetron sputterng on a free-standng Al fol of 500 nm thckness.

More information

PHYSICS 212 MIDTERM II 19 February 2003

PHYSICS 212 MIDTERM II 19 February 2003 PHYSICS 1 MIDERM II 19 Feruary 003 Exam s losed ook, losed notes. Use only your formula sheet. Wrte all work and answers n exam ooklets. he aks of pages wll not e graded unless you so request on the front

More information

4.5. QUANTIZED RADIATION FIELD

4.5. QUANTIZED RADIATION FIELD 4-1 4.5. QUANTIZED RADIATION FIELD Baground Our treatent of the vetor potental has drawn on the onohroat plane-wave soluton to the wave-euaton for A. The uantu treatent of lght as a partle desrbes the

More information

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system

Transfer Functions. Convenient representation of a linear, dynamic model. A transfer function (TF) relates one input and one output: ( ) system Transfer Functons Convenent representaton of a lnear, dynamc model. A transfer functon (TF) relates one nput and one output: x t X s y t system Y s The followng termnology s used: x y nput output forcng

More information

2 Finite difference basics

2 Finite difference basics Numersche Methoden 1, WS 11/12 B.J.P. Kaus 2 Fnte dfference bascs Consder the one- The bascs of the fnte dfference method are best understood wth an example. dmensonal transent heat conducton equaton T

More information

Physics 114 Exam 2 Spring Name:

Physics 114 Exam 2 Spring Name: Physcs 114 Exam Sprng 013 Name: For gradng purposes (do not wrte here): Queston 1. 1... 3. 3. Problem Answer each of the followng questons. Ponts for each queston are ndcated n red wth the amount beng

More information

Chapter 3 Describing Data Using Numerical Measures

Chapter 3 Describing Data Using Numerical Measures Chapter 3 Student Lecture Notes 3-1 Chapter 3 Descrbng Data Usng Numercal Measures Fall 2006 Fundamentals of Busness Statstcs 1 Chapter Goals To establsh the usefulness of summary measures of data. The

More information

Amplification and Relaxation of Electron Spin Polarization in Semiconductor Devices

Amplification and Relaxation of Electron Spin Polarization in Semiconductor Devices Amplfcaton and Relaxaton of Electron Spn Polarzaton n Semconductor Devces Yury V. Pershn and Vladmr Prvman Center for Quantum Devce Technology, Clarkson Unversty, Potsdam, New York 13699-570, USA Spn Relaxaton

More information

FUZZY FINITE ELEMENT METHOD

FUZZY FINITE ELEMENT METHOD FUZZY FINITE ELEMENT METHOD RELIABILITY TRUCTURE ANALYI UING PROBABILITY 3.. Maxmum Normal tress Internal force s the shear force, V has a magntude equal to the load P and bendng moment, M. Bendng moments

More information