Paraxial ray tracing
|
|
- Lilian Horton
- 6 years ago
- Views:
Transcription
1 Desig o ieal imagig ssems wi geomerical opics Paraxial ra-racig EE 566 OE Ssem Desig Paraxial ra racig Derivaio o reracio & raser eqaios φ, φ φ Paraxial ages Sbsie io i-les eqaio Reracio eqaio Traser eqaio Rober cleo Heig o ra a srace. & se [m] φ Power o srace [iopers] Paraxial ra agle icie o srace [raias] Paraxial ra agle exiig srace [raias] Toal isace bewee srace a [m] 7
2 Desig o ieal imagig ssems wi geomerical opics Paraxial ra-racig EE 566 OE Ssem Desig Paraxial ra racig Oe meo o rea iere iices Dealig wi iere iices o reracio: siθ siθ ) ) Sell s Law Paraxial approximaio Rece agle variable Gassia i les eqaio Rece isace variables We ca ow wrie eqaios ivolvig agle a isace b igorig cages i iex. Weever we eal wi problems wi several ierece iices, we simpl mae e above sbsiios. Rober cleo 73
3 Desig o ieal imagig ssems wi geomerical opics Paraxial ra-racig EE 566 OE Ssem Desig - racig A ablar meo obj 8 mm eepiece mm ee? Tbe leg 6 3 Qesio o be aswere: wa is e ro worig isace o a x, 8mm objecive we se wi a 6 mm be, as sow?. Fill i wa o ow. Fill i wa o o ow sig paraxial reracio a raser eqaios. Srace Ssem Axial ra φ / /8 8.4 g 84 e 68 -/ c -/ b 3 / - a a ose arbiraril b Reracio: ( ) c Traser: ( ) Reracio: ( ) Rober cleo e Traser: Reracio: g Traser: O Sea.3 ( )
4 Desig o ieal imagig ssems wi geomerical opics Sigle a compo les ssems EE 566 OE Ssem Desig Te elescope epleria Sow i e aocal geomer ( ). Relaxe ee ocses a ~m, s elescope are sall o aocal. Aalsis simpler, owever. Aocal: ssem as o power: ra o OA - oes o iersec OA i image space α β θ α β Deiiio o aglar magiicaio Via similar riagles Tis is bo impora a ameal. Rober cleo 75
5 Desig o ieal imagig ssems wi geomerical opics Sigle a compo les ssems EE 566 OE Ssem Desig Te elescope Galilea - ore compac, prig image. Same aocal coiio: - α β θ β α ( ) oe a ormla is ieical o epleria. Tis is e avaage o e sig coveio. Rober cleo 76
6 Desig o ieal imagig ssems wi geomerical opics Sigle a compo les ssems EE 566 OE Ssem Desig icroscope obj eepiece Focal ssem. Form image a iii or simplici o aalsis. be leg Saar be leg is 6 mm. Visal magiicaio o isrme is proc o liear magiicaio o objecive a visal magiicaio o eepiece: vmicroscope obj veepiece l be obj D p eepiece oe eq.s are approximae l be >> obj, D p >> eepice obj 4 6 obj [mm] Tpical A Rober cleo 77
7 Desig o ieal imagig ssems wi geomerical opics Sigle a compo les ssems EE 566 OE Ssem Desig Overea projecor Rober cleo 78
8 79 EE 566 OE Ssem Desig Rober cleo ABD marices arix ormlaio o paraxial ra-racig Desig o ieal imagig ssems wi geomerical opics Paraxial ra-racig T R φ Traser eqaio Reracio eqaio TR R T R Ssem marix R T T ojgae marix φ φ φ - φ
9 Desig o ieal imagig ssems wi geomerical opics Paraxial ra-racig EE 566 OE Ssem Desig R Properies o, A B AD B Deermia D T Wrie o e marix eqaio or : I plaes a are cojgaes, ial ra eig oes o epe o iiial ra agle: ojgae coiio I plae is e objec space ocal plae, e slope a e exi plae epes ol o e objec eig: Rober cleo Objec a ro ocal plae I plae is e image space ocal plae, e image-space ra eig epes ol o e erace agle: I e ssem is aocal, e irecio o e image-space ra epes ol o e irecio o e objec-space ra: Image a rear ocal plae Aocal coiio 8
10 8 EE 566 OE Ssem Desig Rober cleo Use o marices, Fi image plae give objec D A D A D B A D B A ) ( T T gives e image locaio D B A ojgae coiio Desig o ieal imagig ssems wi geomerical opics Paraxial ra-racig φ φ φ - ( ) φ φ E.g. sigle les
11 Desig o ieal imagig ssems wi geomerical opics Paraxial ra-racig EE 566 OE Ssem Desig Form o A EFL, irs ic-les cocep A I e is e magiicaio Deermia F Φ Eecive ocal leg & ssem power Φ Φ TR T φ φ E.g. sigle les φ ( φ ) φ Rober cleo 8
12 83 EE 566 OE Ssem Desig Rober cleo Opical ivaria A objec/image plae (special case) Desig o ieal imagig ssems wi geomerical opics Paraxial ra-racig φ Paraxial Sell s Law Sbsie io Triagles I a cascae ssem... H A coserve qai
Section 8. Paraxial Raytracing
Secio 8 Paraxial aracig 8- OPTI-5 Opical Desig ad Isrmeaio I oprigh 7 Joh E. Greiveamp YNU arace efracio (or reflecio) occrs a a ierface bewee wo opical spaces. The rasfer disace ' allows he ra heigh '
More informationChapter 6 - Work and Energy
Caper 6 - Work ad Eergy Rosedo Pysics 1-B Eploraory Aciviy Usig your book or e iere aswer e ollowig quesios: How is work doe? Deie work, joule, eergy, poeial ad kieic eergy. How does e work doe o a objec
More informationChapter 2: Time-Domain Representations of Linear Time-Invariant Systems. Chih-Wei Liu
Caper : Time-Domai Represeaios of Liear Time-Ivaria Sysems Ci-Wei Liu Oulie Iroucio Te Covoluio Sum Covoluio Sum Evaluaio Proceure Te Covoluio Iegral Covoluio Iegral Evaluaio Proceure Iercoecios of LTI
More informationUNIT 1: ANALYTICAL METHODS FOR ENGINEERS
UNIT : ANALYTICAL METHODS FOR ENGINEERS Ui code: A// QCF Level: Credi vale: OUTCOME TUTORIAL SERIES Ui coe Be able o aalyse ad model egieerig siaios ad solve problems sig algebraic mehods Algebraic mehods:
More informationSoftware Process Models there are many process model s in th e li t e ra t u re, s om e a r e prescriptions and some are descriptions you need to mode
Unit 2 : Software Process O b j ec t i ve This unit introduces software systems engineering through a discussion of software processes and their principal characteristics. In order to achieve the desireable
More information2.710 Optics Spring 09 Solutions to Problem Set #2 Due Wednesday, Feb. 25, 2009
MASSACHUSETTS INSTITUTE OF TECHNOLOGY.70 Optics Sprig 09 Solutios to Prolem Set # Due Weesay, Fe. 5, 009 Prolem : Wiper spee cotrol Figure shows a example o a optical system esige to etect the amout o
More informationNumerical KDV equation by the Adomian decomposition method
America Joral o oder Physics ; () : -5 Pblished olie ay (hp://wwwsciecepblishiggropcom/j/ajmp) doi: 648/jajmp merical KDV eqaio by he Adomia decomposiio mehod Adi B Sedra Uiversié Ib Toail Faclé des Scieces
More informationLenses and Imaging (Part II)
Lee ad Imagig (Part II) emider rom Part I Surace o poitive/egative power eal ad virtual image Imagig coditio Thick lee Pricipal plae 09/20/04 wk3-a- The power o urace Poitive power : eitig ray coverge
More informationSection 7. Gaussian Reduction
7- Sectio 7 Gaussia eductio Paraxial aytrace Equatios eractio occurs at a iterace betwee two optical spaces. The traser distace t' allows the ray height y' to be determied at ay plae withi a optical space
More information6.003: Signals and Systems
6.003: Sigals ad Sysems Lecure 8 March 2, 2010 6.003: Sigals ad Sysems Mid-erm Examiaio #1 Tomorrow, Wedesday, March 3, 7:30-9:30pm. No reciaios omorrow. Coverage: Represeaios of CT ad DT Sysems Lecures
More informationLecture 25 Outline: LTI Systems: Causality, Stability, Feedback
Lecure 5 Oulie: LTI Sye: Caualiy, Sabiliy, Feebac oucee: Reaig: 6: Lalace Trafor. 37-49.5, 53-63.5, 73; 7: 7: Feebac. -4.5, 8-7. W 8 oe, ue oay. Free -ay eeio W 9 will be oe oay, ue e Friay (o lae W) Fial
More informationLecture 7: Polar representation of complex numbers
Lecture 7: Polar represetatio of comple umbers See FLAP Module M3.1 Sectio.7 ad M3. Sectios 1 ad. 7.1 The Argad diagram I two dimesioal Cartesia coordiates (,), we are used to plottig the fuctio ( ) with
More informationλiv Av = 0 or ( λi Av ) = 0. In order for a vector v to be an eigenvector, it must be in the kernel of λi
Liear lgebra Lecure #9 Noes This week s lecure focuses o wha migh be called he srucural aalysis of liear rasformaios Wha are he irisic properies of a liear rasformaio? re here ay fixed direcios? The discussio
More informationDavid Randall. ( )e ikx. k = u x,t. u( x,t)e ikx dx L. x L /2. Recall that the proof of (1) and (2) involves use of the orthogonality condition.
! Revised April 21, 2010 1:27 P! 1 Fourier Series David Radall Assume ha u( x,) is real ad iegrable If he domai is periodic, wih period L, we ca express u( x,) exacly by a Fourier series expasio: ( ) =
More informationSection 12. Afocal Systems
OPTI-0/0 Geoetrical and Instruental Optics Copyrigt 08 Jon E. Greivenkap - Section Aocal Systes Gaussian Optics Teores In te initial discussion o Gaussian optics, one o te teores deined te two dierent
More informationAdministrivia. Administrivia. Visual motion. CMPSCI 370: Intro. to Computer Vision. Optical flow
Admiisriia Fial eam: Thrsda, Ma 5, -3pm, Hasbrock 3 Reiew sessio poll Thrsda, April 8, 4-5pm, Locaio: TDB Tesda, Ma 3, 4-5pm, Locaio: TDB CMPSC 370: ro. o Comper Visio Reiew oes are posed o Moodle Opical
More informationSingle Degree of Freedom System Free Vibration
Maa Kliah : Diamika Srkr & Pegaar Rekayasa Kegempaa Kode : TSP 30 SKS : 3 SKS Sigle Degree of Freedom Sysem Free Vibraio Perema - TIU : Mahasisa dapa mejelaska eag eori diamika srkr. Mahasisa dapa memba
More informationSingle Degree of Freedom System Free Vibration
Iegriy, Professioalism, & Erepreership Maa Kliah : Diamika Srkr & Pegaar Rekayasa Kegempaa Kode : CIV 308 SKS : 3 SKS Sigle Degree of Freedom Sysem Free Vibraio Perema - Iegriy, Professioalism, & Erepreership
More informationNumerical methods for ordinary differential equations
A Maser Scieiic copuig Nuerical ehos or oriar iereial equaios Oriar iereial equaios Le be a ocio o oe variable havig successive erivaives. A h orer oriar iereial equaio ODE is a equaio o he or: A s orer
More informationSection 5. Gaussian Imagery
OPTI-01/0 Geoetrical ad Istruetal Optics 5-1 Sectio 5 Gaussia Iagery Iagig Paraxial optics provides a sipliied etodology to deterie ray pats troug optical systes. Usig tis etod, te iage locatio or a geeral
More information2.710 Optics Spring 09 Solutions to Problem Set #3 Due Wednesday, March 4, 2009
MASSACHUSETTS INSTITUTE OF TECHNOLOGY.70 Optics Sprig 09 Solutios to Problem Set #3 Due Weesay, March 4, 009 Problem : Waa s worl a) The geometry or this problem is show i Figure. For part (a), the object
More informationSUMMATION OF INFINITE SERIES REVISITED
SUMMATION OF INFINITE SERIES REVISITED I several aricles over he las decade o his web page we have show how o sum cerai iiie series icludig he geomeric series. We wa here o eed his discussio o he geeral
More informationRepresenting Functions as Power Series. 3 n ...
Math Fall 7 Lab Represetig Fuctios as Power Series I. Itrouctio I sectio.8 we leare the series c c c c c... () is calle a power series. It is a uctio o whose omai is the set o all or which it coverges.
More informationCurvilinear Motion: Normal and Tangential Components
15 Crviliear Moio: Noral ad Tageial Copoe Ref: Hibbeler 1.7, Bedford & Fowler: Dyaic.3 Whe he pah of a paricle i kow, a - coordiae ye wih a origi a he locaio of he paricle (a a ia i ie) ca be helpfl i
More informationStability. Outline Stability Sab Stability of Digital Systems. Stability for Continuous-time Systems. system is its stability:
Oulie Sabiliy Sab Sabiliy of Digial Syem Ieral Sabiliy Exeral Sabiliy Example Roo Locu v ime Repoe Fir Orer Seco Orer Sabiliy e Jury e Rouh Crierio Example Sabiliy A very impora propery of a yamic yem
More informationOptical flow. Visual motion. Motion and perceptual organization. Motion and perceptual organization. Subhransu Maji. CMPSCI 670: Computer Vision
Visal moio Opical flow Sbhras Maji CMPSC 670: Comper Visio Ocober 0, 06 Ma slides adaped from S. Seiz, R. Szeliski, M. Pollefes CMPSC 670 Moio ad percepal orgaizaio Moio ad percepal orgaizaio Someimes,
More informationA L A BA M A L A W R E V IE W
A L A BA M A L A W R E V IE W Volume 52 Fall 2000 Number 1 B E F O R E D I S A B I L I T Y C I V I L R I G HT S : C I V I L W A R P E N S I O N S A N D TH E P O L I T I C S O F D I S A B I L I T Y I N
More informationI M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o
I M P O R T A N T S A F E T Y I N S T R U C T I O N S W h e n u s i n g t h i s e l e c t r o n i c d e v i c e, b a s i c p r e c a u t i o n s s h o u l d a l w a y s b e t a k e n, i n c l u d f o l
More informationWave Equation! ( ) with! b = 0; a =1; c = c 2. ( ) = det ( ) = 0. α = ±c. α = 1 2a b ± b2 4ac. c 2. u = f. v = f x ; t c v. t u. x t. t x = 2 f.
Compuaioal Fluid Dyamics p://www.d.edu/~gryggva/cfd-course/ Compuaioal Fluid Dyamics Wave equaio Wave Equaio c Firs wrie e equaio as a sysem o irs order equaios Iroduce u ; v ; Gréar Tryggvaso Sprig yieldig
More informationP a g e 5 1 of R e p o r t P B 4 / 0 9
P a g e 5 1 of R e p o r t P B 4 / 0 9 J A R T a l s o c o n c l u d e d t h a t a l t h o u g h t h e i n t e n t o f N e l s o n s r e h a b i l i t a t i o n p l a n i s t o e n h a n c e c o n n e
More informationDerivation of the Metal-Semiconductor Junction Current
.4.4. Derivio of e Mel-Seiouor uio Curre.4.4.1.Derivio of e iffuio urre We r fro e epreio for e ol urre e iegre i over e wi of e epleio regio: q( µ + D (.4.11 wi be rewrie b uig -/ uliplig bo ie of e equio
More informationNumerical Method for Ordinary Differential Equation
Numerical ehod for Ordiar Differeial Equaio. J. aro ad R. J. Lopez, Numerical Aalsis: A Pracical Approach, 3rd Ed., Wadsworh Publishig Co., Belmo, CA (99): Chap. 8.. Iiial Value Problem (IVP) d (IVP):
More informationMCR3U FINAL EXAM REVIEW (JANUARY 2015)
MCRU FINAL EXAM REVIEW (JANUARY 0) Iroducio: This review is composed of possible es quesios. The BEST wa o sud for mah is o do a wide selecio of quesios. This review should ake ou a oal of hours of work,
More informationCALCULUS BASIC SUMMER REVIEW
CALCULUS BASIC SUMMER REVIEW NAME rise y y y Slope of a o vertical lie: m ru Poit Slope Equatio: y y m( ) The slope is m ad a poit o your lie is, ). ( y Slope-Itercept Equatio: y m b slope= m y-itercept=
More informationME 321 Kinematics and Dynamics of Machines S. Lambert Winter 2002
ME 31 Kiemaic ad Dyamic o Machie S. Lamber Wier 6.. Forced Vibraio wih Dampig Coider ow he cae o orced vibraio wih dampig. Recall ha he goverig diereial equaio i: m && c& k F() ad ha we will aume ha he
More information02 - COMPLEX NUMBERS Page 1 ( Answers at the end of all questions ) l w l = 1, then z lies on
0 - COMPLEX NUMBERS Page ( ) If the cube roots of uity are,,, the the roots of the equatio ( x - ) + 8 = 0 are ( a ) -, - +, - - ( b ) -, -, -, ( c ) -, -, - ( d ) -, +, + [ AIEEE 005 ] ( ) If z ad z are
More informationDETAIL MEASURE EVALUATE
MEASURE EVALUATE B I M E q u i t y BIM Workflow Guide MEASURE EVALUATE Introduction We o e to ook 2 i t e BIM Workflow Guide i uide wi tr i you i re ti ore det i ed ode d do u e t tio u i r i d riou dd
More informationThe Moment Approximation of the First Passage Time For The Birth Death Diffusion Process with Immigraton to a Moving Linear Barrier
Rece Avaces i Auomaic Corol, oellig a Simulaio The ome Approximaio of he Firs Passage Time For The irh Deah Diffusio Process wih Immigrao o a ovig Liear arrier ASEL. AL-EIDEH Kuwai Uiversiy, College of
More information12 th Mathematics Objective Test Solutions
Maemaics Objecive Tes Soluios Differeiaio & H.O.D A oes idividual is saisfied wi imself as muc as oer are saisfied wi im. Name: Roll. No. Bac [Moda/Tuesda] Maimum Time: 90 Miues [Eac rig aswer carries
More informationH STO RY OF TH E SA NT
O RY OF E N G L R R VER ritten for the entennial of th e Foundin g of t lair oun t y on ay 8 82 Y EEL N E JEN K RP O N! R ENJ F ] jun E 3 1 92! Ph in t ed b y h e t l a i r R ep u b l i c a n O 4 1922
More informationElectrical Engineering Department Network Lab.
Par:- Elecrical Egieerig Deparme Nework Lab. Deermiaio of differe parameers of -por eworks ad verificaio of heir ierrelaio ships. Objecive: - To deermie Y, ad ABD parameers of sigle ad cascaded wo Por
More informationMITPress NewMath.cls LAT E X Book Style Size: 7x9 September 27, :04am. Contents
Coes 1 Temporal filers 1 1.1 Modelig sequeces 1 1.2 Temporal filers 3 1.2.1 Temporal Gaussia 5 1.2.2 Temporal derivaives 6 1.2.3 Spaioemporal Gabor filers 8 1.3 Velociy-ued filers 9 Bibliography 13 1
More informationECE 570 Session 7 IC 752-E Computer Aided Engineering for Integrated Circuits. Transient analysis. Discuss time marching methods used in SPICE
ECE 570 Sessio 7 IC 75-E Compuer Aided Egieerig for Iegraed Circuis Trasie aalysis Discuss ime marcig meods used i SPICE. Time marcig meods. Explici ad implici iegraio meods 3. Implici meods used i circui
More informationc. What is the average rate of change of f on the interval [, ]? Answer: d. What is a local minimum value of f? Answer: 5 e. On what interval(s) is f
Essential Skills Chapter f ( x + h) f ( x ). Simplifying the difference quotient Section. h f ( x + h) f ( x ) Example: For f ( x) = 4x 4 x, find and simplify completely. h Answer: 4 8x 4 h. Finding the
More informationAn Efficient Method to Reduce the Numerical Dispersion in the HIE-FDTD Scheme
Wireless Egieerig ad Techolog, 0,, 30-36 doi:0.436/we.0.005 Published Olie Jauar 0 (hp://www.scirp.org/joural/we) A Efficie Mehod o Reduce he umerical Dispersio i he IE- Scheme Jua Che, Aue Zhag School
More informationLINEAR APPROXIMATION OF THE BASELINE RBC MODEL JANUARY 29, 2013
LINEAR APPROXIMATION OF THE BASELINE RBC MODEL JANUARY 29, 203 Iroducio LINEARIZATION OF THE RBC MODEL For f( x, y, z ) = 0, mulivariable Taylor liear expasio aroud f( x, y, z) f( x, y, z) + f ( x, y,
More informationThe universal vector. Open Access Journal of Mathematical and Theoretical Physics [ ] Introduction [ ] ( 1)
Ope Access Joural of Mahemaical ad Theoreical Physics Mii Review The uiversal vecor Ope Access Absrac This paper akes Asroheology mahemaics ad pus some of i i erms of liear algebra. All of physics ca be
More informationF (u) du. or f(t) = t
8.3 Topic 9: Impulses and dela funcions. Auor: Jeremy Orloff Reading: EP 4.6 SN CG.3-4 pp.2-5. Warmup discussion abou inpu Consider e rae equaion d + k = f(). To be specific, assume is in unis of d kilograms.
More informationRuled surfaces are one of the most important topics of differential geometry. The
CONSTANT ANGLE RULED SURFACES IN EUCLIDEAN SPACES Yuuf YAYLI Ere ZIPLAR Deparme of Mahemaic Faculy of Sciece Uieriy of Aara Tadoğa Aara Turey yayli@cieceaaraedur Deparme of Mahemaic Faculy of Sciece Uieriy
More informationU8L1: Sec Equations of Lines in R 2
MCVU U8L: Sec. 8.9. Equatios of Lies i R Review of Equatios of a Straight Lie (-D) Cosider the lie passig through A (-,) with slope, as show i the diagram below. I poit slope form, the equatio of the lie
More informationImaging and Aberration Theory
Imagig a Aberratio Theor Lecture : Paraxial imagig --9 Herbert Gro Witer term www.iap.ui-ea.e Overview Time: ria,. 3.3 Locatio: Abbeaum, HS, röbeltieg Web page o IAP homepage uer learig/material provie
More informationMath-303 Chapter 7 Linear systems of ODE November 16, Chapter 7. Systems of 1 st Order Linear Differential Equations.
Mah-33 Chaper 7 Liear sysems of ODE November 6, 7 Chaper 7 Sysems of s Order Liear Differeial Equaios saddle poi λ >, λ < Mah-33 Chaper 7 Liear sysems of ODE November 6, 7 Mah-33 Chaper 7 Liear sysems
More informationCHEMISTRY 047 STUDY PACKAGE
CHEMISTRY 047 STUDY PACKAGE Tis maerial is inended as a review of skills you once learned. PREPARING TO WRITE THE ASSESSMENT VIU/CAP/D:\Users\carpenem\AppDaa\Local\Microsof\Windows\Temporary Inerne Files\Conen.Oulook\JTXREBLD\Cemisry
More information2 f(x) dx = 1, 0. 2f(x 1) dx d) 1 4t t6 t. t 2 dt i)
Mah PracTes Be sure o review Lab (ad all labs) There are los of good quesios o i a) Sae he Mea Value Theorem ad draw a graph ha illusraes b) Name a impora heorem where he Mea Value Theorem was used i he
More informationLINEAR APPROXIMATION OF THE BASELINE RBC MODEL SEPTEMBER 17, 2013
LINEAR APPROXIMATION OF THE BASELINE RBC MODEL SEPTEMBER 7, 203 Iroducio LINEARIZATION OF THE RBC MODEL For f( xyz,, ) = 0, mulivariable Taylor liear expasio aroud f( xyz,, ) f( xyz,, ) + f( xyz,, )( x
More informationU8L1: Sec Equations of Lines in R 2
MCVU Thursda Ma, Review of Equatios of a Straight Lie (-D) U8L Sec. 8.9. Equatios of Lies i R Cosider the lie passig through A (-,) with slope, as show i the diagram below. I poit slope form, the equatio
More informationChapter 13: Complex Numbers
Sectios 13.1 & 13.2 Comple umbers ad comple plae Comple cojugate Modulus of a comple umber 1. Comple umbers Comple umbers are of the form z = + iy,, y R, i 2 = 1. I the above defiitio, is the real part
More informationExecutive Committee and Officers ( )
Gifted and Talented International V o l u m e 2 4, N u m b e r 2, D e c e m b e r, 2 0 0 9. G i f t e d a n d T a l e n t e d I n t e r n a t i o n a2 l 4 ( 2), D e c e m b e r, 2 0 0 9. 1 T h e W o r
More information2 tel
Us. Timeless, sophisticated wall decor that is classic yet modern. Our style has no limitations; from traditional to contemporar y, with global design inspiration. The attention to detail and hand- craf
More information1. Complex numbers. Chapter 13: Complex Numbers. Modulus of a complex number. Complex conjugate. Complex numbers are of the form
Comple umbers ad comple plae Comple cojugate Modulus of a comple umber Comple umbers Comple umbers are of the form Sectios 3 & 32 z = + i,, R, i 2 = I the above defiitio, is the real part of z ad is the
More informationNATIONAL SENIOR CERTIFICATE GRADE 12
NATIONAL SENIOR CERTIFICATE GRADE 1 MATHEMATICS P FEBRUARY/MARCH 014 MARKS: 150 TIME: 3 hours This questio paper cosists of 1 pages, 3 diagram sheets ad 1 iformatio sheet. Please tur over Mathematics/P
More informationSHOCK AND VIBRATION RESPONSE SPECTRA COURSE Unit 21 Base Excitation Shock: Classical Pulse
SHOCK AND VIBRAION RESPONSE SPECRA COURSE Ui 1 Base Exciaio Shock: Classical Pulse By om Irvie Email: omirvie@aol.com Iroucio Cosier a srucure subjece o a base exciaio shock pulse. Base exciaio is also
More informationBeechwood Music Department Staff
Beechwood Music Department Staff MRS SARAH KERSHAW - HEAD OF MUSIC S a ra h K e rs h a w t r a i n e d a t t h e R oy a l We ls h C o l le g e of M u s i c a n d D ra m a w h e re s h e ob t a i n e d
More informationREPETITIVE CONTROL FOR LINEAR TIME VARYING SYSTEMS. Zongxuan Sun. Research and Development Center General Motors Corporation Warren, MI 48090
roceeigs of IMECE SME Ieraioal Mechaical Egieerig roceeigs Cogress of IMECE & Exosiio SME Ieraioal Mechaical New Orleas Egieerig Loisiaa Cogress November & Exosiio 7- November 7 New Orleas Loisiaa IMECE-3344
More informationControl Systems. Transient and Steady State Response.
Corol Sym Trai a Say Sa Ro chibum@oulch.ac.kr Ouli Tim Domai Aalyi orr ym Ui ro Ui ram ro Ui imul ro Chibum L -Soulch Corol Sym Tim Domai Aalyi Afr h mahmaical mol of h ym i obai, aalyi of ym rformac i.
More informationThe Eigen Function of Linear Systems
1/25/211 The Eige Fucio of Liear Sysems.doc 1/7 The Eige Fucio of Liear Sysems Recall ha ha we ca express (expad) a ime-limied sigal wih a weighed summaio of basis fucios: v ( ) a ψ ( ) = where v ( ) =
More informationCHAPTER 2. Problem 2.1. Given: m k = k 1. Determine the weight of the table sec (b)
CHPTER Problem. Give: m T π 0. 5 sec (a) T m 50 g π. Deermie he weigh of he able. 075. sec (b) Taig he raio of Eq. (b) o Eq. (a) ad sqarig he resl gives or T T mg m 50 g m 50 5. 40 lbs 50 0.75. 5 m g 0.5.
More informationIntroduction. ENCE 455 Design of Steel Structures. IV. Laterally Support Beams. Introduction (cont.)
ENCE 455 Desig o Seel Srucures V. Laerall Suppor Beams C. C. u, P.D., P.E. Civil ad Eviromeal Egieerig Deparme Uiversi o arlad roducio olloig sujecs are covered: roducio Saili Laerall suppored eams Serviceaili
More informationOn The Geometrıc Interpretatıons of The Kleın-Gordon Equatıon And Solution of The Equation by Homotopy Perturbation Method
Available a hp://pvam.ed/aam Appl. Appl. Mah. SSN: 9-9466 Vol. 7, sse (December ), pp. 69-65 Applicaios ad Applied Mahemaics: A eraioal Joral (AAM) O The Geomerıc erpreaıos of The Kleı-Gordo Eqaıo Ad Solio
More informationREFLECTION AND REFRACTION
REFLECTION AND REFRACTION REFLECTION AND TRANSMISSION FOR NORMAL INCIDENCE ON A DIELECTRIC MEDIUM Assumptios: No-magetic media which meas that B H. No dampig, purely dielectric media. No free surface charges.
More informationd y f f dy Numerical Solution of Ordinary Differential Equations Consider the 1 st order ordinary differential equation (ODE) . dx
umerical Solutio o Ordiar Dieretial Equatios Cosider te st order ordiar dieretial equatio ODE d. d Te iitial coditio ca be tae as. Te we could use a Talor series about ad obtai te complete solutio or......!!!
More informationSection 9. Paraxial Raytracing
OPTI-/ Geometrical and Instrmental Optics Copright 8 John E. Greivenkamp 9- Section 9 Paraxial atracing YNU atrace efraction (or reflection) occrs at an interface between two optical spaces. The transfer
More informationODEs II, Supplement to Lectures 6 & 7: The Jordan Normal Form: Solving Autonomous, Homogeneous Linear Systems. April 2, 2003
ODEs II, Suppleme o Lecures 6 & 7: The Jorda Normal Form: Solvig Auoomous, Homogeeous Liear Sysems April 2, 23 I his oe, we describe he Jorda ormal form of a marix ad use i o solve a geeral homogeeous
More informationAdditional Exercises for Chapter What is the slope-intercept form of the equation of the line given by 3x + 5y + 2 = 0?
ddiional Eercises for Caper 5 bou Lines, Slopes, and Tangen Lines 39. Find an equaion for e line roug e wo poins (, 7) and (5, ). 4. Wa is e slope-inercep form of e equaion of e line given by 3 + 5y +
More informationEE757 Numerical Techniques in Electromagnetics Lecture 8
757 Numerical Techiques i lecromageics Lecure 8 2 757, 206, Dr. Mohamed Bakr 2D FDTD e i J e i J e i J T TM 3 757, 206, Dr. Mohamed Bakr T Case wo elecric field compoes ad oe mageic compoe e i J e i J
More informationIf we want to add up the area of four rectangles, we could find the area of each rectangle and then write this sum symbolically as:
Sigma Notatio: If we wat to add up the area of four rectagles, we could fid the area of each rectagle ad the write this sum symbolically as: Sum A A A A Liewise, the sum of the areas of te triagles could
More information176 5 t h Fl oo r. 337 P o ly me r Ma te ri al s
A g la di ou s F. L. 462 E l ec tr on ic D ev el op me nt A i ng er A.W.S. 371 C. A. M. A l ex an de r 236 A d mi ni st ra ti on R. H. (M rs ) A n dr ew s P. V. 326 O p ti ca l Tr an sm is si on A p ps
More informationChapter 2 Feedback Control Theory Continued
Chapter Feedback Cotrol Theor Cotiued. Itroductio I the previous chapter, the respose characteristic of simple first ad secod order trasfer fuctios were studied. It was show that first order trasfer fuctio,
More informationChemistry 1B, Fall 2016 Topics 21-22
Cheisry B, Fall 6 Topics - STRUCTURE ad DYNAMICS Cheisry B Fall 6 Cheisry B so far: STRUCTURE of aos ad olecules Topics - Cheical Kieics Cheisry B ow: DYNAMICS cheical kieics herodyaics (che C, 6B) ad
More informationDepartment of Mathematical and Statistical Sciences University of Alberta
MATH 4 (R) Wier 008 Iermediae Calculus I Soluios o Problem Se # Due: Friday Jauary 8, 008 Deparme of Mahemaical ad Saisical Scieces Uiversiy of Albera Quesio. [Sec.., #] Fid a formula for he geeral erm
More informationPartial Differential Equations
EE 84 Matematical Metods i Egieerig Partial Differetial Eqatios Followig are some classical partial differetial eqatios were is assmed to be a fctio of two or more variables t (time) ad y (spatial coordiates).
More informationChapter 10 Light- Reflectiion & Refraction
Capter 0 Ligt- Relectiion & Reraction Intext Questions On Page 68 Question : Deine te principal ocus o a concae irror. Principal ocus o te concae irror: A point on principal axis on wic parallel ligt rays
More informationUnit 3 B Outcome Assessment Pythagorean Triple a set of three nonzero whole numbers that satisfy the Pythagorean Theorem
a Pythagorea Theorem c a + b = c b Uit Outcome ssessmet Pythagorea Triple a set of three ozero whole umbers that satisfy the Pythagorea Theorem If a + b = c the the triagle is right If a + b > c the the
More informationLinear System Theory
Naioal Tsig Hua Uiversiy Dearme of Power Mechaical Egieerig Mid-Term Eamiaio 3 November 11.5 Hours Liear Sysem Theory (Secio B o Secio E) [11PME 51] This aer coais eigh quesios You may aswer he quesios
More informationSection 6. Object-Image Relationships
6-1 Section 6 Object-Image elationships Object-Image elationships The purpose o this study is to examine the imaging properties o the general system that has been deined by its Gaussian properties and
More information07 - SEQUENCES AND SERIES Page 1 ( Answers at he end of all questions ) b, z = n
07 - SEQUENCES AND SERIES Page ( Aswers at he ed of all questios ) ( ) If = a, y = b, z = c, where a, b, c are i A.P. ad = 0 = 0 = 0 l a l
More informationCHATTERJEA CONTRACTION MAPPING THEOREM IN CONE HEPTAGONAL METRIC SPACE
Fameal Joal of Mahemaic a Mahemaical Sciece Vol. 7 Ie 07 Page 5- Thi pape i aailable olie a hp://.fi.com/ Pblihe olie Jaa 0 07 CHATTERJEA CONTRACTION MAPPING THEOREM IN CONE HEPTAGONAL METRIC SPACE Caolo
More informationFour equations describe the dynamic solution to RBC model. Consumption-leisure efficiency condition. Consumption-investment efficiency condition
LINEARIZING AND APPROXIMATING THE RBC MODEL SEPTEMBER 7, 200 For f( x, y, z ), mulivariable Taylor liear expasio aroud ( x, yz, ) f ( x, y, z) f( x, y, z) + f ( x, y, z)( x x) + f ( x, y, z)( y y) + f
More informationEffect of Thickness Stress in Stretch-Bending
h Numiorm Coerece, Pohag, Korea, Jue -7 2 Eec o Thickess Sress i Srech-Beig A.H. va e Boogaar a, W.C. Emmes b * a J. Huéik a a: Uiv. o Twee,P.O.Box 27, 75 AE Eschee, he Neherlas b: CORUS R&D, P.O.Box.,
More informationAn Insight into Differentiation and Integration
Differetiatio A Isigt ito Differetiatio a Itegratio Differetiatio is basically a task to fi out ow oe variable is cagig i relatio to aoter variable, te latter is usually take as a cause of te cage. For
More informationMODERN CONTROL SYSTEMS
MODERN CONTROL SYSTEMS Lecure 9, Sae Space Repreeaio Emam Fahy Deparme of Elecrical ad Corol Egieerig email: emfmz@aa.edu hp://www.aa.edu/cv.php?dip_ui=346&er=6855 Trafer Fucio Limiaio TF = O/P I/P ZIC
More informationMinimizing the Total Late Work on an Unbounded Batch Machine
The 7h Ieraioal Symposium o Operaios Research ad Is Applicaios (ISORA 08) Lijiag, Chia, Ocober 31 Novemver 3, 2008 Copyrigh 2008 ORSC & APORC, pp. 74 81 Miimizig he Toal Lae Work o a Ubouded Bach Machie
More informationF D D D D F. smoothed value of the data including Y t the most recent data.
Module 2 Forecasig 1. Wha is forecasig? Forecasig is defied as esimaig he fuure value ha a parameer will ake. Mos scieific forecasig mehods forecas he fuure value usig pas daa. I Operaios Maageme forecasig
More informationSAFE HANDS & IIT-ian's PACE EDT-10 (JEE) SOLUTIONS
. If their mea positios coicide with each other, maimum separatio will be A. Now from phasor diagram, we ca clearly see the phase differece. SAFE HANDS & IIT-ia's PACE ad Aswer : Optio (4) 5. Aswer : Optio
More informationThe Ability C ongress held at the Shoreham Hotel Decem ber 29 to 31, was a reco rd breaker for winter C ongresses.
The Ability C ongress held at the Shoreham Hotel Decem ber 29 to 31, was a reco rd breaker for winter C ongresses. Attended by m ore than 3 00 people, all seem ed delighted, with the lectu res and sem
More informationResearch Design - - Topic 2 Inferential Statistics: The t-test 2010 R.C. Gardner, Ph.D. Independent t-test
Research Desig - - Topic Ifereial aisics: The -es 00 R.C. Garer, Ph.D. Geeral Raioale Uerlyig he -es (Garer & Tremblay, 007, Ch. ) The Iepee -es The Correlae (paire) -es Effec ize a Power (Kirk, 995, pp
More information9. Point mode plotting with more than two images 2 hours
Lecure 9 - - // Cocep Hell/feiffer Februar 9. oi mode ploig wih more ha wo images hours aim: iersecio of more ha wo ras wih orieaed images Theor: Applicaio co lieari equaio 9.. Spaial Resecio ad Iersecio
More informationPAIR OF STRAIGHT LINES.
PAIR OF STRAIGHT LINES PREVIOUS EAMCET BITS 1. The value of λ with λ < 16 suh that x 1xy + 1y + 5x + λy 3 = represets a pair of straight lies, is [EAMCET 9] 1) 1 ) 9 3) 1 4)9 As: Sol. Δ= λ= 9. The area
More informationDIFFERENCE EQUATIONS
DIFFERECE EQUATIOS Lier Cos-Coeffiie Differee Eqios Differee Eqios I disree-ime ssems, esseil feres of ip d op sigls pper ol speifi iss of ime, d he m o e defied ewee disree ime seps or he m e os. These
More informationECE 350 Matlab-Based Project #3
ECE 350 Malab-Based Projec #3 Due Dae: Nov. 26, 2008 Read he aached Malab uorial ad read he help files abou fucio i, subs, sem, bar, sum, aa2. he wrie a sigle Malab M file o complee he followig ask for
More information