Light. Topics. Page 1. Visible electromagnetic radiation Power spectrum. Polarization Photon (quantum effects) Wave (interference, diffraction)
|
|
- Patricia Tate
- 5 years ago
- Views:
Transcription
1 Light Visible electmagnetic adiatin Pwe spectum Pwe Heat Radi Ulta- X-Rays Gamma Csmic Infa- Red Vilet Rays Rays Wavelength (NM) IR R G B UV Plaizatin Phtn (quantum effects) Wave (intefeence, diffactin) Fm Lndn and Uptn Tpics Radimety and phtmety Measuing spatial ppeties f light Radiant pwe Radiant intensity Iadiance Invese squae law and csine law Radiance Radiant exitance (adisity) Page 1
2 Radimety and Phtmety Radiant Enegy and Pwe Pwe: Watts (adimety) Φ vs. Lumens (phtmety) Enegy efficiency Spectal efficacy Enegy: Jules vs. Talbt Expsue Film espnse Luminance Skin - sunbun Y V( λ) L( λ) dλ Page
3 Radiant Intensity Radiant Intensity Definitin: The adiant (luminus) intensity is the pwe pe unit slid angle emanating fm a pint suce. I( ω) dφ W lm cd candela s s Page 3
4 Angles and Slid Angles Angle l cicle has π adians A Slid angle Ω R sphee has 4π steadians Diffeential Slid Angles sin dφ φ d ( d )( sin dφ ) sin d dφ sin d dφ Page 4
5 Diffeential Slid Angles sin dφ φ d sinddφ Ω S π π π 1 0 4π sin d dφ dcs dφ Sphee S Istpic Pint Suce Φ S 4π I I I Φ 4π Page 5
6 Wan s Sptlight ω ÂA s I ( ω) cs ( ω Aˆ ) s π 1 Φ I ( ω ) dcs dϕ 0 0 Wan s Sptlight ω ÂA s I ( ω) cs ( ω Aˆ ) s π 1 1 s π Φ I ( ω ) dcs dϕ π cs dcs s Page 6
7 Wan s Sptlight ω ÂA s I ( ω) cs ( ω Aˆ ) s π 1 1 s π Φ I ( ω ) dcs dϕ π cs dcs s s + 1 s I( ω) Φ cs π Light Suce Gnimetic Diagams Page 7
8 PIXAR Pint Light Suce Shadws Shadw Matte Pjected Slide Textue UbeLight( ) { Clip t nea/fa planes Clip t shape bunday feach supeelliptical blcke atten * feach ckie textue atten * feach slide textue cl * feach nise textue atten, cl * feach shadw map atten, cl * Calculate intensity fall-ff Calculate beam distibutin } Iadiance Page 8
9 Iadiance Definitin: The iadiance (illuminance) is the pwe pe unit aea incident n a suface. dφi Ex () W lm lux m m Smetimes efeed t as the adiant (luminus) incidence. Lambet s Csine Law ΦEA A E A Φ Page 9
10 Lambet s Csine Law A A /cs Φ Φ Φ E cs A /cs A Iadiance: Istpic Pint Suce h I Φ 4π Page 10
11 Iadiance: Istpic Pint Suce h I Φ 4π dφ I Iadiance: Istpic Pint Suce h I Φ 4π cs Page 11
12 Iadiance: Istpic Pint Suce h I Φ 4π I Φ cs 4π Iadiance: Istpic Pint Suce h I Φ 4π Φ cs I E 4π Φ cs E 4π Page 1
13 Iadiance: Istpic Pint Suce Φ I 4π h cs E Φ cs Φ cs 4π 4π h 3 The Inventin f Phtmety Bugue s classic expeiment Cmpae a light suce and a candle Mve until they bth appea equally bight Intensity is pptinal t ati f distances squaed Definitin f a candela Oiginally a standad candle Cuently 550 nm lase w/ 1/683 W/s 1 f 6 fundamental SI units Page 13
14 Typical Values f Illuminance [lm/m ] Sunlight plus skylight 100,000 lux Sunlight plus skylight (vecast) 10,000 Intei nea windw (daylight) 1,000 Atificial light (minimum) 100 Mnlight (full) 0.0 Stalight Radiance Page 14
15 Aea Lights Suface Radiance Definitin: The suface adiance (luminance) is the intensity pe unit aea leaving a suface Lxω (, ) di( x, ω) Lx (, ω) d Φ( x, ω) W cd lm nit s m m s m Pwe Leaving a Suface Lxω (, ) d Φ ( x, ω) L( x, ω) Page 15
16 Typical Values f Luminance [cd/m ] Suface f the sun,000,000,000 nit Sunlight cluds 30,000 Clea day 3,000 Ovecast day 300 Mn 0.03 Radiant Exitance (Radisity) Page 16
17 Radiant Exitance Definitin: The adiant (luminus) exitance is the enegy pe unit aea leaving a suface. dφ Mx ( ) W lm lux m m In cmpute gaphics, this quantity is ften efeed t as the adisity (B) Pwe Leaving a Suface Lxω (, ) d Φ ( x, ω) L( x, ω) Page 17
18 Diectinal Pwe Leaving a Suface L (, x ω ) d Φ ( x, ω) L ( x, ω)cs d Φ (, x ω ) Nte csine Aea Light Suce d Φ ( x, ω) L ( x, ω)cs L (, x ω ) Same f all diectins Page 18
19 Aea Light Suce d Φ( x, ω) dm ( x, ω) L ( x, ω)cs L (, x ω ) Same f all diectins Aea Light Suce dm ( x, ω) L ( x, ω)cs L (, x ω ) Same f all diectins Page 19
20 Aea Light Suce M dm ( x, ω) L ( x, ω)cs H H L (, x ω ) H Hemisphee Unifm Diffuse Emitte M L cs H L H cs L ( x, ω ) L Page 0
21 Pjected Slid Angle Ω cs Ω cs Pjected Slid Angle Ω cs Ω cs Ω cs π CS348B Lectue 4 H Pat Hanahan, 008 Page 1
22 Unifm Diffuse Emitte M L cs H L πl cs H M L L M π Radimety and Phtmety Summay Page
23 Radimetic and Phtmetic Tems Physics Radimety Phtmety Enegy Radiant Enegy Luminus Enegy Flux (Pwe) Radiant Pwe Luminus Pwe Flux Density Iadiance Radisity Illuminance Luminsity Angula Flux Density Radiance Luminance Intensity Radiant Intensity Luminus Intensity Phtmetic Units Phtmety Units Luminus Enegy Talbt MKS CGS Bitish Luminus Pwe Illuminance Luminsity Lumen Lux Pht Ftcandle Luminance Nit Stilb Apstilb, Blndel Lambet Ftlambet Luminus Intensity Candela (Candle, Candlepwe, Cacel, Hefne) Thus ne nit is ne lux pe steadian is ne candela pe squae mete is ne lumen pe squae mete pe steadian. Gt it?, James Kajiya Page 3
Rays. CS348B Lecture 4 Pat Hanrahan, 2004
Page 1 Light Visible electomagnetic adiation Powe spectum 1 10 10 4 10 6 10 8 10 10 10 1 10 14 10 16 10 18 10 0 10 10 4 10 6 Powe Heat Radio Ulta- X-Rays Gamma Cosmic Infa- Red Violet Rays Rays 10 16 10
More informationRadiometry and Photometry
Radiometry and Photometry Measuring spatial properties of light Radiant power Radiant intensity Irradiance Inverse square law and cosine law Radiance Radiant exitance (radiosity) From London and Upton
More informationRadiometry and Photometry
Light Visible electromagnetic radiation Power spectrum Polarization Photon (quantum effects) Wave (interference, diffraction) From London and Upton Radiometry and Photometry Measuring spatial properties
More informationLight Sources and Illumination. Blackbody. Page 1
Light Sources and Illumination Properties of light sources Power Spectrum Radiant and luminous intensity Directional distribution goniometric diagram Shape Illumination Irradiance and illuminance Area
More informationDefinition: The radiant (luminous) intensity is the power per unit solid angle from a point. CS348B Lecture 5 Pat Hanrahan, Spring 2000
Radant and Lumnous Intensty Defnton: The adant (lumnous) ntensty s the powe pe unt sold angle fom a pont. dφ I(ω) Φ S I( ω) W candela cd s lm s The Inventon of Photomety Bougue s Classc expement Compae
More informationBlack Body Radiation and Radiometric Parameters:
Black Body Radiation and Radiometic Paametes: All mateials absob and emit adiation to some extent. A blackbody is an idealization of how mateials emit and absob adiation. It can be used as a efeence fo
More informationElectromagnetic Waves
Chapte 3 lectmagnetic Waves 3.1 Maxwell s quatins and ectmagnetic Waves A. Gauss s Law: # clsed suface aea " da Q enc lectic fields may be geneated by electic chages. lectic field lines stat at psitive
More informationKey objectives in Lighting design
Key objectives in Lighting design Visual performance Physiological conditions Visual quality no strong "contrasts" good "color rendering" adequate "light levels" no "disturbing reflections" no direct "glare"
More informationFundamentals of light
Fundamentals of light CHAPTER 1 Introduction Environmental issues Limited resources. Consumption. Sustainability Environmental damage will result in environmental changes (climate change, global warming,
More informationFundamentals of light
Fundamentals of light CHAPTER 1 Introduction Environmental issues Limited resources. Consumption. Sustainability Environmental damage will result in environmental changes (climate change, global warming,
More informationSection 22. Radiative Transfer
OPTI-01/0 Geometrical and Instrumental Optics Copyright 018 John E. Greivenkamp -1 Section Radiative Transfer Radiometry Radiometry characterizes the propagation of radiant energy through an optical system.
More informationVI. Terminology for Display
Special Topics in Display Technology 1 st semester, 2015 VI. Terminology for Display * Reference books: [Light Measurement Handbook] (http://www.intl-light.com) [ 응용광학 ] ( 두양사 ) 21 장 Radiometry and Photometry
More informationSection 10. Radiative Transfer
Section 10 Radiative Transfer 10-1 OPTI-50 Optical Design and Instrumentation I Copyright 017 John E. Greivenkamp Radiometry Radiometry characterizes the propagation of radiant energy through an optical
More informationELECTROMAGNETIC RADIATION
ELECTROMAGNETIC RADIATION 1. Types of electromagnetic radiation Use different resources to sort the types of electromagnetic radiation according to rising wavelength, find sources, uses and mention if
More information1) Emits radiation at the maximum intensity possible for every wavelength. 2) Completely absorbs all incident radiation (hence the term black ).
Radiation laws Blackbody adiation Planck s Law Any substance (solid, liquid o gas) emits adiation accoding to its absolute tempeatue, measued in units of Kelvin (K = o C + 73.5). The efficiency at which
More informationOptics.
Optics www.optics.rochester.edu/classes/opt100/opt100page.html Course outline Light is a Ray (Geometrical Optics) 1. Nature of light 2. Production and measurement of light 3. Geometrical optics 4. Matrix
More informationLUMINOUS MEASUREMENTS
Chapter 5. LUMINOUS MEASUREMENTS 5.. Luminous flux (luminous output)............................ 47 5.2. Amount of light (luminous energy)........................... 48 5.3. Luminous intensity.......................................
More informationRadiometry. Energy & Power
Radiometry Radiometry is the measurement of optical radiation, corresponding to wavelengths between 0.01 and 1000 μm, and includes the regions commonly called the ultraviolet, the visible and the infrared.
More informationVIII. Further Aspects of Edge Diffraction
VIII. Futhe Aspects f Edge Diffactin Othe Diffactin Cefficients Oblique Incidence Spheical Wave Diffactin by an Edge Path Gain Diffactin by Tw Edges Numeical Examples Septembe 3 3 by H.L. Betni Othe Diffactin
More informationMathieu Hébert, Thierry Lépine
1 Introduction to Radiometry Mathieu Hébert, Thierry Lépine Program 2 Radiometry and Color science IOGS CIMET MINASP 3DMT Introduction to radiometry Advanced radiometry (2 nd semester) x x x x x o o Color
More informationGeneral Information. Vishay Semiconductors. Explanation of Technical Data. Type Designation Code for LEDs
General Information Explanation of Technical Data Vishay light emitting diodes and displays are generally designated in accordance with the Vishay designation system: TL... = Light emitting diode TD...
More informationIntroduction. Electrostatics
UNIVESITY OF TECHNOLOGY, SYDNEY FACULTY OF ENGINEEING 4853 Electmechanical Systems Electstatics Tpics t cve:. Culmb's Law 5. Mateial Ppeties. Electic Field Stength 6. Gauss' Theem 3. Electic Ptential 7.
More informationFundamentals of Rendering - Radiometry / Photometry
Fundamentals of Rendering - Radiometry / Photometry CMPT 461/761 Image Synthesis Torsten Möller Today The physics of light Radiometric quantities Photometry vs/ Radiometry 2 Reading Chapter 5 of Physically
More informationFundamentals of Rendering - Radiometry / Photometry
Fundamentals of Rendering - Radiometry / Photometry Image Synthesis Torsten Möller Today The physics of light Radiometric quantities Photometry vs/ Radiometry 2 Reading Chapter 5 of Physically Based Rendering
More informationRadiometry, photometry, measuring color
Radiometry, photometry, measuring color Lecture notes are done by Géza Várady, based on the lecture notes of Prof. János Schanda varady.geza@mik.pte.hu University of Pécs, Faculty of Engineering and Information
More informationCHAPTER 24 GAUSS LAW
CHAPTR 4 GAUSS LAW LCTRIC FLUX lectic flux is a measue f the numbe f electic filed lines penetating sme suface in a diectin pependicula t that suface. Φ = A = A csθ with θ is the angle between the and
More informationEpisode 315: The inverse square law
Episode 315: The invese squae law This episode consides the ways in which the intensity o adiation deceases with distance om the souce. Summay Demonstation + discussion: adiation speading out, and an analogy.
More informationSolution: (a) C 4 1 AI IC 4. (b) IBC 4
C A C C R A C R C R C sin 9 sin. A cuent f is maintaine in a single cicula lp f cicumfeence C. A magnetic fiel f is iecte paallel t the plane f the lp. (a) Calculate the magnetic mment f the lp. (b) What
More informationOPAC 101 Introduction to Optics
OPAC 101 Introduction to Optics Topic 3 Introductory Photometry Department of http://www1.gantep.edu.tr/~bingul/opac101 Optical & Acustical Engineering Gaziantep University Sep 017 Sayfa 1 Introduction
More informationLight. E.M. waves electromagnetic both electric and magnetic characteristics travels at 3.0 x 10 8 m/s in a vacuum slower in material mediums
Light E.M. waves electromagnetic both electric and magnetic characteristics travels at 3.0 x 10 8 m/s in a vacuum slower in material mediums 1) requires no medium but can travel through them 2) is energy
More informationThe nature of electromagnetic radiation.
Lectue 3 The natue of electomagnetic adiation. Objectives: 1. Basic intoduction to the electomagnetic field: Definitions Dual natue of electomagnetic adiation lectomagnetic spectum. Main adiometic quantities:
More informationCHAPTER GAUSS'S LAW
lutins--ch 14 (Gauss's Law CHAPTE 14 -- GAU' LAW 141 This pblem is ticky An electic field line that flws int, then ut f the cap (see Figue I pduces a negative flux when enteing and an equal psitive flux
More informationELECTROMAGNETIC INDUCTION PREVIOUS EAMCET BITS
P P Methd EECTOMAGNETIC INDUCTION PEVIOUS EAMCET BITS [ENGINEEING PAPE]. A cnduct d f length tates with angula speed ω in a unifm magnetic field f inductin B which is pependicula t its mtin. The induced
More informationENVIRONMENTAL SYSTEMS
LIGHT http://map.gsfc.nasa.gov/media/ Ball State Architecture ENVIRONMENTAL SYSTEMS 1 Grondzik 1 study carrel in Phillips Exeter Library; a celebration of light and of material (by L. Kahn) Kahn on Light
More informationTECHNICAL NOTE. Relating Photochemical and Photobiological Quantities to Photometric Quantities
TECHNICAL NOTE Relating Photochemical and Photobiological Quantities to Photometric Quantities CIE TN 002:2014 CIE Technical Notes (TN) are short technical papers summarizing information of fundamental
More informationB. Spherical Wave Propagation
11/8/007 Spheical Wave Popagation notes 1/1 B. Spheical Wave Popagation Evey antenna launches a spheical wave, thus its powe density educes as a function of 1, whee is the distance fom the antenna. We
More informationDescribing the Potency of Light
Describing the Potency of Light Douglas A. Kerr, P.E. (Ret.) Issue 3 September 19, 2013 INTRODUCTION In many types of technical work it is necessary to quantify the potency 1 of light. The matter is complicated
More informationBasic Optical Concepts. Oliver Dross, LPI Europe
Basic Optical Concepts Oliver Dross, LPI Europe 1 Refraction- Snell's Law Snell s Law: Sin( φi ) Sin( φ ) f = n n f i n i Media Boundary φ i n f φ φ f angle of exitance 90 80 70 60 50 40 30 20 10 0 internal
More informationElectric Charge. Electric charge is quantized. Electric charge is conserved
lectstatics lectic Chage lectic chage is uantized Chage cmes in incements f the elementay chage e = ne, whee n is an intege, and e =.6 x 0-9 C lectic chage is cnseved Chage (electns) can be mved fm ne
More informationThe Electromagnetic Spectrum
The Electromagnetic Spectrum A Brief History of Light 1000 AD It was proposed that light consisted of tiny particles Newton Used this particle model to explain reflection and refraction Huygens 1678 Explained
More informationComputer Graphics III Radiometry. Jaroslav Křivánek, MFF UK
Computer Graphics III Radiometry Jaroslav Křivánek, MFF UK Jaroslav.Krivanek@mff.cuni.cz Direction, solid angle, spherical integrals Direction in 3D Direction = unit vector in 3D Cartesian coordinates
More informationME 3600 Control Systems Frequency Domain Analysis
ME 3600 Cntl Systems Fequency Dmain Analysis The fequency espnse f a system is defined as the steady-state espnse f the system t a sinusidal (hamnic) input. F linea systems, the esulting utput is itself
More informationA*STAR Seminar on LED and Solid State Lighting. Standards and Technologies. Measurements. 05 August LIU Yuanjie National Metrology Centre
A*STAR Seminar on LED and Solid State Lighting Standards and Technologies available at NMC for LED Measurements 05 August 2011 LIU Yuanjie National Metrology Centre Outline NMC overview Basic optical quantities
More informationn Power transmission, X rays, lightning protection n Solid-state Electronics: resistors, capacitors, FET n Computer peripherals: touch pads, LCD, CRT
.. Cu-Pl, INE 45- Electmagnetics I Electstatic fields anda Cu-Pl, Ph.. INE 45 ch 4 ECE UPM Maagüe, P me applicatins n Pwe tansmissin, X as, lightning ptectin n lid-state Electnics: esists, capacits, FET
More informationIntroduction to Computer Vision Radiometry
Radiometry Image: two-dimensional array of 'brightness' values. Geometry: where in an image a point will project. Radiometry: what the brightness of the point will be. Brightness: informal notion used
More informationSec. 9.1 Lines and Angles
Sec. 9. Line and Angle Leaning Objective:. Identify line, line egment, ay, and angle.. Claify angel a acute, igt, btue, taigt.. Identify cmplementay and upplementay angle. 4. Find meaue f angle. 5. Key
More informationAIR FORCE RESEARCH LABORATORY
AIR FORC RSARCH LABORATORY The xtinctin Theem as an xample f Reseach Vistas in Mathematical Optics Mach Richad A. Albanese Infmatin Opeatins and Applied Mathematics Human ffectiveness Diectate Bks City-Base
More informationPhys-272 Lecture 17. Motional Electromotive Force (emf) Induced Electric Fields Displacement Currents Maxwell s Equations
Phys-7 Lectue 17 Motional Electomotive Foce (emf) Induced Electic Fields Displacement Cuents Maxwell s Equations Fom Faaday's Law to Displacement Cuent AC geneato Magnetic Levitation Tain Review of Souces
More informationMarch 15. Induction and Inductance Chapter 31
Mach 15 Inductin and Inductance Chapte 31 > Fces due t B fields Lentz fce τ On a mving chage F B On a cuent F il B Cuent caying cil feels a tque = µ B Review > Cuents geneate B field Bit-Savat law = qv
More informationDescribing the Strength of Visible Light
Describing the Strength of Visible Light Douglas A. Kerr, P.E. Issue 2 August 31, 2003 INTRODUCTION In many types of technical work it is necessary to describe the strength 1 of visible light. The matter
More informationFoundations of Chemical Kinetics. Lecture 9: Generalizing collision theory
Foundations of Chemical Kinetics Lectue 9: Genealizing collision theoy Mac R. Roussel Depatment of Chemisty and Biochemisty Spheical pola coodinates z θ φ y x Angles and solid angles θ a A Ω θ=a/ unit:
More informationASSESSMENT OF NON-COHERENT LIGHT SOURCES
ASSESSMENT OF NON-COHERENT LIGHT SOURCES David Egan Snr Team Leader Laser Science Support Orion Laser Facility AWE, UK Page 1 Introduction Laser safety is accepted However there is a certain reticence
More informationA) (0.46 î ) N B) (0.17 î ) N
Phys10 Secnd Maj-14 Ze Vesin Cdinat: xyz Thusday, Apil 3, 015 Page: 1 Q1. Thee chages, 1 = =.0 μc and Q = 4.0 μc, ae fixed in thei places as shwn in Figue 1. Find the net electstatic fce n Q due t 1 and.
More informationNature of Light. What is light? Sources of light. an electromagnetic radiation capable of stimulating the retina of the eye.
Nature of Light What is light? an electromagnetic radiation capable of stimulating the retina of the eye. electrons Nucleus Electron gains energy When it moves to a higher level Photon bundle (quantum)
More informationChapter 29: Maxwell s Equation and EM Waves. Slide 29-1
Chapter 29: Maxwell s Equation and EM Waves Slide 29-1 Equations of electromagnetism: a review We ve now seen the four fundamental equations of electromagnetism, here listed together for the first time.
More informationSection 4.2 Radians, Arc Length, and Area of a Sector
Sectin 4.2 Radian, Ac Length, and Aea f a Sect An angle i fmed by tw ay that have a cmmn endpint (vetex). One ay i the initial ide and the the i the teminal ide. We typically will daw angle in the cdinate
More informationOutline. Steady Heat Transfer with Conduction and Convection. Review Steady, 1-D, Review Heat Generation. Review Heat Generation II
Steady Heat ansfe ebuay, 7 Steady Heat ansfe wit Cnductin and Cnvectin ay Caett Mecanical Engineeing 375 Heat ansfe ebuay, 7 Outline eview last lectue Equivalent cicuit analyses eview basic cncept pplicatin
More informationWork, Energy, and Power. AP Physics C
k, Eneg, and Pwe AP Phsics C Thee ae man diffeent TYPES f Eneg. Eneg is expessed in JOULES (J) 4.19 J = 1 calie Eneg can be expessed me specificall b using the tem ORK() k = The Scala Dt Pduct between
More informationChapter 13: Gravitation
v m m F G Chapte 13: Gavitation The foce that makes an apple fall is the same foce that holds moon in obit. Newton s law of gavitation: Evey paticle attacts any othe paticle with a gavitation foce given
More informationThe geometric construction of Ewald sphere and Bragg condition:
The geometic constuction of Ewald sphee and Bagg condition: The constuction of Ewald sphee must be done such that the Bagg condition is satisfied. This can be done as follows: i) Daw a wave vecto k in
More informationFri. 10/23 (C14) Linear Dielectrics (read rest at your discretion) Mon. (C 17) , E to B; Lorentz Force Law: fields
Fi. 0/23 (C4) 4.4. Linea ielectics (ead est at yu discetin) Mn. (C 7) 2..-..2, 2.3. t B; 5..-..2 Lentz Fce Law: fields Wed. and fces Thus. (C 7) 5..3 Lentz Fce Law: cuents Fi. (C 7) 5.2 Bit-Savat Law HW6
More informationINTRODUCTION TO MICROWAVE REMOTE SENSING - II. Dr. A. Bhattacharya
1 INTRODUCTION TO MICROWAVE REMOTE SENSING - II Dr. A. Bhattacharya The Radiation Framework The information about features on the Earth s surface using RS depends on measuring energy emanating from the
More informationComputer Graphics III Radiometry. Jaroslav Křivánek, MFF UK
Computer Graphics III Radiometry Jaroslav Křivánek, MFF UK Jaroslav.Krivanek@mff.cuni.cz Direction, solid angle, spherical integrals Direction in 3D Direction = unit vector in 3D Cartesian coordinates
More informationChapter. s r. check whether your calculator is in all other parts of the body. When a rigid body rotates through a given angle, all
conveted to adians. Also, be sue to vanced to a new position (Fig. 7.2b). In this inteval, the line OP has moved check whethe you calculato is in all othe pats of the body. When a igid body otates though
More informationPhotobiological Safety of Luminaires: Refining the New Approach
Photobiological Safety of Luminaires: Refining the New Approach Leslie Lyons Bentham Instruments Limited Reading, UK llyons@bentham.co.uk We are all familiar with the visual characteristics of lighting
More informationIntroductory Photometry
Vesion 2.1 Noman Wittels 121 Clak oad Bookline MA 2169 wittels@wold.std.com 1986-97 Noman Wittels Light This note intoduces the concepts and methods used to measue light. adiant tansfe of enegy happens
More informationSTUDY OVER LUMINOUS CHARACTERISTICS OF THE TRACER COMPOSITIONS
STUDY OVER LUMINOUS CHARACTERISTICS OF THE TRACER COMPOSITIONS BOGDAN GABRIEL LUCIAN, ENG. S. C. UZINA MECANICA SADU S. A. e-mail: lucianbog@yahoo.com ABSTRACT: The study of the evolution of the luminous
More informationIntroduction CHAPTER 01. Light and opto-semiconductors. Opto-semiconductor lineup. Manufacturing process of opto-semiconductors.
CHAPTER 0 Light and opto-semiconductors - -2 Light Opto-semiconductors P. 0 P. 3 2 Opto-semiconductor lineup P. 5 3 Manufacturing process of opto-semiconductors P. 6 9 CHAPTER 0. Light and opto-semiconductors
More informationOn Skylight and Aerial Perspective. A.J. Preetham ATI Research
On Skylight and Aerial Perspective A.J. Preetham ATI Research (preetham@ati.com) Introduction Outline Atmosphere Skylight Simulation models Analytic models Aerial Perspective Scattering using graphics
More informationChapter 5 Trigonometric Functions
Chapte 5 Tignmetic Functins Sectin 5.2 Tignmetic Functins 5-5. Angles Basic Teminlgy Degee Measue Standad Psitin Cteminal Angles Key Tems: vetex f an angle, initial side, teminal side, psitive angle, negative
More information10. Force is inversely proportional to distance between the centers squared. R 4 = F 16 E 11.
NSWRS - P Physics Multiple hoice Pactice Gavitation Solution nswe 1. m mv Obital speed is found fom setting which gives v whee M is the object being obited. Notice that satellite mass does not affect obital
More informationModule 1 LIGHT SOURCES Lecture 1. Introduction. Basic principles of Light and Vision
Module 1 LIGHT SOURCES Lecture 1. Introduction. Basic principles of Light and Vision After the mid-17th century, scientists were divided into two sides. One side, including Isaac Newton, believed in the
More informationMagnetism. Chapter 21
1.1 Magnetic Fields Chapte 1 Magnetism The needle f a cmpass is pemanent magnet that has a nth magnetic ple (N) at ne end and a suth magnetic ple (S) at the the. 1.1 Magnetic Fields 1.1 Magnetic Fields
More informationOBJECTIVE To investigate the parallel connection of R, L, and C. 1 Electricity & Electronics Constructor EEC470
Assignment 7 Paallel Resnance OBJECTIVE T investigate the paallel cnnectin f R,, and C. EQUIPMENT REQUIRED Qty Appaatus 1 Electicity & Electnics Cnstuct EEC470 1 Basic Electicity and Electnics Kit EEC471-1
More informationSummary chapter 4. Electric field s can distort charge distributions in atoms and molecules by stretching and rotating:
Summa chapte 4. In chapte 4 dielectics ae discussed. In thse mateials the electns ae nded t the atms mlecules and cannt am fee thugh the mateial: the electns in insulats ae n a tight leash and all the
More informationPhys 332 Electricity & Magnetism Day 3. Note: I should have recommended reading section 1.5 (delta function) as well. rˆ rˆ
Phs 33 lecticit & Magnetism Da 3 Mn. 9/9 Wed. 9/ Thus 9/ Fi. 9/3 (C.-.5,.8). &.5;..-.. Gauss & Div, T Numeical Quadatue (C.-.5,.8)..3 Using Gauss (C.-.5,.8)..3-.. Using Gauss HW quipment Bing in ppt s
More informationA Guide to Integrating Sphere Theory and Applications
A Guide to Integrating Sphere Theory and Applications Leadership in Reflectance Technology T E C H G U I D E TABLE OF CONTENTS 1.0 Integrating Sphere Theory...2-5 1.1 Radiation Exchange Within a Spherical
More informationAnnouncements Candidates Visiting Next Monday 11 12:20 Class 4pm Research Talk Opportunity to learn a little about what physicists do
Wed., /11 Thus., /1 Fi., /13 Mn., /16 Tues., /17 Wed., /18 Thus., /19 Fi., / 17.7-9 Magnetic Field F Distibutins Lab 5: Bit-Savat B fields f mving chages (n quiz) 17.1-11 Pemanent Magnets 18.1-3 Mic. View
More informationA) N B) 0.0 N C) N D) N E) N
Cdinat: H Bahluli Sunday, Nvembe, 015 Page: 1 Q1. Five identical pint chages each with chage =10 nc ae lcated at the cnes f a egula hexagn, as shwn in Figue 1. Find the magnitude f the net electic fce
More informationIllumination, Radiometry, and a (Very Brief) Introduction to the Physics of Remote Sensing!
Illumination, Radiometry, and a (Very Brief) Introduction to the Physics of Remote Sensing! Course Philosophy" Rendering! Computer graphics! Estimation! Computer vision! Robot vision" Remote sensing! lhm
More informationSensors and Actuators Introduction to sensors
Senss and Actuats Intductin t senss Sande Stuij (s.stuij@tue.nl) Depatment f Electical Engineeing Electnic Systems AMPLIFIES (Chapte 5.) Infmatin pcessing system nncntact sens cntact sens abslute sens
More informationLighting fundamentals
Lighting fundamentals About light and photometrics Generation of light Human vision Black body Colour Basic principles of lighting Light sources Light Vision Colour What is light? Light is electromagnetic
More informationUIUC Physics 435 EM Fields & Sources I Fall Semester, 2007 Lecture Notes 1 Prof. Steven Errede LECTURE NOTES 1
UIUC Physics 435 EM Fields & Suces I Fall Semeste, 007 Lectue Ntes 1 Pf. Steen Eede Intductin: LECTURE NOTES 1 In this cuse, we will study/inestigate the natue f the ELECTROMAGNETIC INTERACTION (at {ey}
More informationChapter 5. Daylighting
Chapter 5. Daylighting 5.1. History of Daylighting The history of daylighting and the history of architecture were one. The major structural changes in buildings reflected the goal of increasing the amount
More informationBasic Interference and. Classes of of Interferometers
Basic Intefeence and Classes of Intefeometes Basic Intefeence Two plane waves Two spheical waves Plane wave and and spheical wave Classes of of Intefeometes Division of of wavefont Division of of amplitude
More informationOptics for Engineers Chapter 12
Optics for Engineers Chapter 12 Charles A. DiMarzio Northeastern University Apr. 214 Radiometry Power is Proportional to Area of Aperture Stop Area of Field Stop Brightness of the Source (Radiance) Apr.
More informationThe condition for maximum intensity by the transmitted light in a plane parallel air film is. For an air film, μ = 1. (2-1)
hapte Two Faby--Peot ntefeomete A Faby-Peot intefeomete consists of two plane paallel glass plates A and B, sepaated by a distance d. The inne sufaces of these plates ae optically plane and thinly silveed
More informationIslamic University of Gaza - Palestine. Department of Industrial Engineering
Department of Industrial Engineering Ergonomics Human Machine Work Environment Greatest Goal: Humanization of Work Design with E & E : Ease and Efficiency The Basics of Ergonomics Core courses (The Three
More informationAST 121S: The origin and evolution of the Universe. Introduction to Mathematical Handout 1
Please ead this fist... AST S: The oigin and evolution of the Univese Intoduction to Mathematical Handout This is an unusually long hand-out and one which uses in places mathematics that you may not be
More informationPrinciples of Planetary Photometry
Daft Nov. 4, 24 Chapte 1. Pinciples of Planetay Photomety 1. Intoduction. The subject of planetay photomety is, in substantial pat, a subset of that banch of mathematical physics known as adiative tansfe,
More informationModeling of Environmental Systems
Modeling of Environmental Systems While the modeling of predator-prey dynamics is certainly simulating an environmental system, there is more to the environment than just organisms Recall our definition
More information5/20/2011. HITT An electron moves from point i to point f, in the direction of a uniform electric field. During this displacement:
5/0/011 Chapte 5 In the last lectue: CapacitanceII we calculated the capacitance C f a system f tw islated cnducts. We als calculated the capacitance f sme simple gemeties. In this chapte we will cve the
More informationLED STREET LIGHT SLIP FITTER MOUNT
WARRANTY PART NO: GT-S-G07-CT3A1-BRPAM40 PART NO: GT-S-G07-CT3A1-BRPAM57 DESCRIPTION These lights are the top of the line in quality and price. These fixture are easy to installation and operate and are
More informationb) (5) What average force magnitude was applied by the students working together?
Geneal Physics I Exam 3 - Chs. 7,8,9 - Momentum, Rotation, Equilibium Nov. 3, 2010 Name Rec. Inst. Rec. Time Fo full cedit, make you wok clea to the gade. Show fomulas used, essential steps, and esults
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department. Problem Set 10 Solutions. r s
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Depatment Physics 8.033 Decembe 5, 003 Poblem Set 10 Solutions Poblem 1 M s y x test paticle The figue above depicts the geomety of the poblem. The position
More informationTA/TI survey. Phy Phy
TA/TI survey https://webapps.pas.rochester.edu/secure/phpq/ Phy121 7 60 73 Phy123 1 6 11 Chapter 34 The Wave Nature of Light; Interference Units of Chapter 34 34-5 Interference in Thin Films 34-6 Michelson
More informationMath Section 4.2 Radians, Arc Length, and Area of a Sector
Math 1330 - Section 4. Radians, Ac Length, and Aea of a Secto The wod tigonomety comes fom two Geek oots, tigonon, meaning having thee sides, and mete, meaning measue. We have aleady defined the six basic
More informationINVERSE QUANTUM STATES OF HYDROGEN
INVERSE QUANTUM STATES OF HYDROGEN Rnald C. Bugin Edgecmbe Cmmunity Cllege Rcky Munt, Nth Calina 780 bugin@edgecmbe.edu ABSTRACT The pssible existence f factinal quantum states in the hydgen atm has been
More informationWHY STRONG WHITE GOLD FULL SPECTRUM CAN GROW ANY SPECIES EVOLUTION OF THE GOLDEN GLOW SPECTRA
GOLDEN GLOW TM SPECTRA WHY STRONG WHITE GOLD FULL SPECTRUM CAN GROW ANY SPECIES GOLDEN GLOW SPECTRA TM Smart Grow Systems has been developing and testing LED technologies with commercial cannabis growers
More informationPhysics 1114: Unit 5 Hand-out Homework (Answers)
Physics 1114: Unit 5 Hand-out Homewok (Answes) Poblem set 1 1. The flywheel on an expeimental bus is otating at 420 RPM (evolutions pe minute). To find (a) the angula velocity in ad/s (adians/second),
More information