Geometrical Optics Mirrors and Prisms

Similar documents
Ch 35 Images. Eunil Won Department of Physics Korea University. Fundamentals of Physics by Eunil Won, Korea University 1

Introductory Optomechanical Engineering. 2) First order optics

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

Chapter 6 The Effect of the GPS Systematic Errors on Deformation Parameters

Lecturer: Ivan Kassamakov, Docent Assistant: Kalle Hanhijärvi. Course webpage:

Math1110 (Spring 2009) Prelim 3 - Solutions

Physics 120. Exam #1. April 15, 2011

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

Chapter K - Problems

Harmonic oscillator approximation

CHAPTER 9 LINEAR MOMENTUM, IMPULSE AND COLLISIONS

COMPLEX NUMBERS AND QUADRATIC EQUATIONS

Verification of Selected Precision Parameters of the Trimble S8 DR Plus Robotic Total Station

Unit 5: Quadratic Equations & Functions

COMPOSITE BEAM WITH WEAK SHEAR CONNECTION SUBJECTED TO THERMAL LOAD

Scattering of two identical particles in the center-of. of-mass frame. (b)

An easy way to relate optical element motion to system pointing stability

Electromagnetic scattering. Graduate Course Electrical Engineering (Communications) 1 st Semester, Sharif University of Technology

Problem Do any of the following determine homomorphisms from GL n (C) to GL n (C)?

CS4495/6495 Introduction to Computer Vision. 3C-L3 Calibrating cameras

Module 14: THE INTEGRAL Exploring Calculus

Formal solvers of the RT equation

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

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

ECE 472/572 - Digital Image Processing. Roadmap. Questions. Lecture 6 Geometric and Radiometric Transformation 09/27/11

Module 5. Cables and Arches. Version 2 CE IIT, Kharagpur

Phys 402: Raman Scattering. Spring Introduction: Brillouin and Raman spectroscopy. Raman scattering: how does it look like?

Root Locus Techniques

Lecture Topics VMSC Prof. Dr.-Ing. habil. Hermann Lödding Prof. Dr.-Ing. Wolfgang Hintze. PD Dr.-Ing. habil.

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

Chapter 7 Four-Wave Mixing phenomena

Title: Radiative transitions and spectral broadening

AP Statistics Ch 3 Examining Relationships

Boundaries, Near-field Optics

Spectral Graph Theory and its Applications September 16, Lecture 5

Chapter 11. Supplemental Text Material. The method of steepest ascent can be derived as follows. Suppose that we have fit a firstorder

Fresnel's Equations for Reflection and Refraction

Indeterminate pin-jointed frames (trusses)

p 1 c 2 + p 2 c 2 + p 3 c p m c 2

Introduction to Antennas & Arrays

6) Derivatives, gradients and Hessian matrices

Some modelling aspects for the Matlab implementation of MMA

Additional File 1 - Detailed explanation of the expression level CPD

w ). Then use the Cauchy-Schwartz inequality ( v w v w ).] = in R 4. Can you find a vector u 4 in R 4 such that the

5.76 Lecture #21 2/28/94 Page 1. Lecture #21: Rotation of Polyatomic Molecules I

HO 40 Solutions ( ) ˆ. j, and B v. F m x 10-3 kg = i + ( 4.19 x 10 4 m/s)ˆ. (( )ˆ i + ( 4.19 x 10 4 m/s )ˆ j ) ( 1.40 T )ˆ k.

CHAPTER II THEORETICAL BACKGROUND

Statistical Properties of the OLS Coefficient Estimators. 1. Introduction

Section 8.1 Exercises

Lecture 3: Probability Distributions

Programming Project 1: Molecular Geometry and Rotational Constants

Graphical Analysis of a BJT Amplifier

Norms, Condition Numbers, Eigenvalues and Eigenvectors

New approach to Fully Nonlinear Adiabatic TWM Theory

Line Drawing and Clipping Week 1, Lecture 2

Electric Potential Energy & Potential. Electric Potential Energy. Potential Energy. Potential Energy. Example: Charge launcher

Lecture 3. Interaction of radiation with surfaces. Upcoming classes

U.C. Berkeley CS294: Beyond Worst-Case Analysis Luca Trevisan September 5, 2017

PHYS 705: Classical Mechanics. Calculus of Variations II

Section 8.3 Polar Form of Complex Numbers

Generalized Linear Methods

From Biot-Savart Law to Divergence of B (1)

Electric and magnetic field sensor and integrator equations

Physics 2A Chapter 3 HW Solutions

11. Dynamics in Rotating Frames of Reference

Ionization fronts in HII regions

E40M Device Models, Resistors, Voltage and Current Sources, Diodes, Solar Cells. M. Horowitz, J. Plummer, R. Howe 1

Specification -- Assumptions of the Simple Classical Linear Regression Model (CLRM) 1. Introduction

APPENDIX A Some Linear Algebra

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

Report on Image warping

Introduction to circuit analysis. Classification of Materials

The Geometry of Logit and Probit

NEWTON S LAWS. These laws only apply when viewed from an inertial coordinate system (unaccelerated system).

Physics 5153 Classical Mechanics. Principle of Virtual Work-1

3. Be able to derive the chemical equilibrium constants from statistical mechanics.

For all questions, answer choice E) NOTA" means none of the above answers is correct.

MiniBooNE Event Reconstruction and Particle Identification

CHAPTER 14 GENERAL PERTURBATION THEORY

Least Squares Fitting of Data

Causal Diamonds. M. Aghili, L. Bombelli, B. Pilgrim

Lecture 12: Discrete Laplacian

FE REVIEW OPERATIONAL AMPLIFIERS (OP-AMPS)( ) 8/25/2010

σ τ τ τ σ τ τ τ σ Review Chapter Four States of Stress Part Three Review Review

16 Reflection and transmission, TE mode

Modeling curves. Graphs: y = ax+b, y = sin(x) Implicit ax + by + c = 0, x 2 +y 2 =r 2 Parametric:

PY2101 Classical Mechanics Dr. Síle Nic Chormaic, Room 215 D Kane Bldg

Please initial the statement below to show that you have read it

PHYS 100 Worked Examples Week 05: Newton s 2 nd Law

Finite Element Modelling of truss/cable structures

EECE 301 Signals & Systems Prof. Mark Fowler

VEKTORANALYS GAUSS THEOREM STOKES THEOREM. and. Kursvecka 3. Kapitel 6 7 Sidor 51 82

Team. Outline. Statistics and Art: Sampling, Response Error, Mixed Models, Missing Data, and Inference

Lecture 3. Camera Models 2 & Camera Calibration. Professor Silvio Savarese Computational Vision and Geometry Lab. 13- Jan- 15.

Week 9 Chapter 10 Section 1-5

Numerical Algorithms for Visual Computing 2008/09 Example Solutions for Assignment 4. Problem 1 (Shift invariance of the Laplace operator)

Multilayer Perceptrons and Backpropagation. Perceptrons. Recap: Perceptrons. Informatics 1 CG: Lecture 6. Mirella Lapata

Module 1 : The equation of continuity. Lecture 1: Equation of Continuity

The General Nonlinear Constrained Optimization Problem

Complex Numbers. x = B B 2 4AC 2A. or x = x = 2 ± 4 4 (1) (5) 2 (1)

Transcription:

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 alo called plane, or flat mrror r = - o Sgn conventon: on the object de potve, and negatve on the oppote de

Planar mrror Sgn conventon: on the object de potve, and negatve on the oppote de = - o For a plane mrror, a pont ource and t mage are at the ame dtance from the mrror on oppote de; both le on the ame normal lne. Image vrtual, up-rght, and lfe-ze (M T = +) The equaton for len work: M T y y o o

Exerce: plane mrror heght How hgh hould be the mrror for a peron to ee a full mage of hm/her-elf? Soluton: A B D C Trangle ABC twce a mall a ADE E BC half DE (the heght of the guy). Mrror (BC) hould be at leat half of the guy heght (DE) 2. It bottom hould /2 of the heght of guy eye from the ground

Mrror mage Mrror mage of left hand a rght hand Inveron: convertng rght-handed coordnate ytem nto left-handed one Even number of mrror can be ued to avod nveron

Applcaton: teerng lght DLP projecton TV reflex camera (SLR) http://www.plu-amerca.com/paper.html Atomc force mcrocope

Parabolc aphercal mrror V Make a mrror that wll converge plane wave nto a pont Fermat prncple: OPL W A A F W2 A2 A2 F Applcaton: headlght, W A A D W2 A2 A2 D2 flahlght, A F A D A2 F A2 D radar, 2 dh antenna, In general: AF AD. Th the urface of parabolod: y 2 = 4fx (orgn at vertext V)

Aphercal mrror dvergngdvergng convergngdvergng off-ax parabolc Collect lght from one pont to another convergngconvergng dvergngconvergng

Sphercal mrror y 2 4 fx Parabolod and phere are mlar n paraxal approxmaton y y 2 2 x 2 2 x R R 2 2 2 y x 2xR 2 2 2xR R R mall when cloe to ax x

Sphercal mrror formula SAP bected by AC: SC SA CP PA Paraxal approxmaton: o R o o R 2 R SA o PA Focal length: f lm/ / f 2/ R o o o f lm/ / f 2/ R o SC o R CP Sgn conventon: R R<0 n real object pace o >0 n real object pace >0 n real mage pace f >0 concave mrror Mrror Formula 2 f R o

Sphercal mrror o f 2 R Note: Both mrror and len equaton are the ame, except the real mage n front of mrror, but t behnd the len Magnfcaton equaton are the ame a well.

Concave mrror: prncpal axe and mage Prncpal ray for concave mrror: ) Parallel to prncpal ax reflect through F. o f 2 R 2) Through F, reflect parallel to prncpal ax. 3) Through center. S # #3 f Image : C Real (lght ray actually cro) Inverted (Arrow pont n oppote drecton) Dmnhed (maller than object, only f object further than C) NOTE: Any other ray from object tp whch ht mrror wll reflect through mage tp #2

Convex mrror: prncpal axe and mage Prncpal ray for convex mrror: ) Parallel to prncpal ax appear to orgnate from F after reflecton. 2) Through F, reflect parallel to prncpal ax. 3) Through center. # S #2 #3 P Image : f Vrtual (lght ray don t really cro) Uprght (ame drecton a object) Dmnhed (maller than object) **For a real object, mage alway vrtual, uprght and dmnhed F C

Exerce: can a concave mrror form a vrtual mage? o f o Concave mrror: o and f are alway potve, want to get negatve f o 0 vrtual mage o f An object mut be between mrror and t focal plane F o

Sphercal mrror

Example

Dperng prm n n n t n t Bendng depend on wavelength: dperng prm,.e. n=n() Can we ue optcal flat for dperng lght? Ray emerge parallel to each other. Practcally we don t ee them (focued by the eye at the ame pot).

Dperng prm equaton n n n t n t t2 Example n = n t =n Total devaton a functon of refracton ndex: 2 2 arcn n n n t n co Mnmum devaton mn occur when = t2 n n mn / 2 n / 2 can ue to determne n

Spectral analyzer And th arrangement map poton to angle: out xn

Prm pectrometer Drawback: () - nonlnear dependence Low pectral reoluton Small aperture

Contant-devaton dperng prm Pelln-Broca prm: Abbe prm: mn =90 o alway! Pelln, Ph. and Broca, André (899), "A Spectrocope of Fxed Devaton". Atrophycal Journal 0 337 Ernt Abbe 840-905 mn =60 o alway! Fx nput-output at 90 o or 60 o and rotate prm for dfferent wavelength

Reflectng prm Reflect the beam wth no dperon ung total nternal reflecton If we make t = 2 - lke n flat gla plate = 2 + achromatc prm

Reflectng prm The rght-angle prm The Porro prm The penta prm The Dove prm