Light
Visible electromagnetic radiation Power spectrum
2 4 6 8 10 12 14 16 18 20 22 24 26 11010 10 10 10 10 10 10 10 10 10 10 10
Power Heat Radio Infra- Ultra- X-Rays Gamma Cosmic Red Violet Rays Rays
16 14 12 10 8 6 4 2 -2 -4 -6 -8 10 10 10 10 10 10 10 10 11010 10 10 Wavelength (NM)
IR R G B UV
700600 500 400
Polarization Photon (quantum effects) From London and Upton Wave (interference, diffraction)
CS348B Lecture 4 Pat Hanrahan, 2004
Topics
Light sources and illumination Radiometry and photometry Quantify spatial energy distribution Radiant intensity Irradiance and radiant exitance (radiosity) Inverse square law and cosine law Radiance Illumination calculations Irradiance from environment
CS348B Lecture 4 Pat Hanrahan, 2004
Page 1 Radiometry and Photometry
Radiant Energy and Power
Power: Watts vs. Lumens Φ Energy efficiency Spectral efficacy
Energy: Joules vs. Talbot Exposure Film response Skin - sunburn Luminance YVLd= ∫ ()()λ λλ
CS348B Lecture 4 Pat Hanrahan, 2004
Page 2 Radiometry vs. Photometry
Radiometry [Units = Watts] Physical measurement of electromagnetic energy Photometry and Colorimetry [Lumen] Sensation as a function of wavelength Relative perceptual measurement 1 Brightness [Brils] BY= 3 Sensation at different brightness levels Absolute perceptual measurement Obeys Steven’s Power Law
CS348B Lecture 4 Pat Hanrahan, 2004
Blackbody
CS348B Lecture 4 Pat Hanrahan, 2004
Page 3 Tungsten
CS348B Lecture 4 Pat Hanrahan, 2004
Fluorescent
CS348B Lecture 4 Pat Hanrahan, 2004
Page 4 Sunlight
CS348B Lecture 4 Pat Hanrahan, 2004
Radiant Intensity
Page 5 Radiant Intensity
Definition: The radiant (luminous) intensity is the power per unit solid angle emanating from a point source.
dΦ I()ω ≡ dω
Wlm ==cd candela sr sr
CS348B Lecture 4 Pat Hanrahan, 2004
Angles and Solid Angles
l Angle θ = r
⇒ circle has 2π radians
A Solid angle Ω= R2
⇒ sphere has 4π steradians
CS348B Lecture 4 Pat Hanrahan, 2004
Page 6 Differential Solid Angles
rsinθ
dφ r dA= ()(sin) r dθ rθφ d dθ θ = rdd2 sinθθφ
φ dA dddω ==sinθθφ r 2
CS348B Lecture 4 Pat Hanrahan, 2004
Differential Solid Angles
dA dddω ==sinθθφ rsinθ r 2
dφ r Ω=∫ dω dθ 2 θ S ππ2 = ∫∫sinθ ddθφ φ 00 12π = ∫∫ddcosθ φ −10 = 4π
CS348B Lecture 4 Pat Hanrahan, 2004
Page 7 Isotropic Point Source
Φ=∫ I dω S2 = 4π I
Φ I = 4π
CS348B Lecture 4 Pat Hanrahan, 2004
Warn’s Spotlight ω θ Aˆ I()ωθω==• cosss(Aˆ )
21π Φ= ∫∫I()cosω ddθϕ 00
CS348B Lecture 4 Pat Hanrahan, 2004
Page 8 Warn’s Spotlight ω θ Aˆ I()ωθω==• cosss(Aˆ )
21π 1 2π Φ=∫∫Id(ωθϕπθθ ) cos d = 2 ∫ coss d cos = 00 0 s +1 s +1 I()ω =Φ coss θ 2π
CS348B Lecture 4 Pat Hanrahan, 2004
Light Source Goniometric Diagrams
CS348B Lecture 4 Pat Hanrahan, 2004
Page 9 PIXAR Light Source
UberLight( ) { Clip to near/far planes Clip to shape boundary foreach superelliptical blocker Shadows atten *= … foreach cookie texture atten *= … foreach slide texture color *= … foreach noise texture Shadow Matte atten, color *= … foreach shadow map atten, color *= … Calculate intensity fall-off Calculate beam distribution } Projected Slide Texture CS348B Lecture 4 Pat Hanrahan, 2004
Radiance
Page 10 Radiance
Definition: The surface radiance (luminance) is the intensity per unit area leaving a surface Lx(,ω ) dI(, x ω ) Lx(,ω )≡ dA dω dx2Φ(,ω ) = ddAω Wcdlm 22== 2nit dA sr m m sr m
CS348B Lecture 4 Pat Hanrahan, 2004
Typical Values of Luminance [cd/m2]
Surface of the sun 2,000,000,000 nit Sunlight clouds 30,000 Clear day 3,000 Overcast day 300 Moon 0.03
CS348B Lecture 4 Pat Hanrahan, 2004
Page 11 Irradiance
The Invention of Photometry
Bouguer’s classic experiment Compare a light source and a candle Intensity is proportional to ratio of distances squared
Definition of a candela Originally a “standard” candle Currently 550 nm laser w/ 1/683 W/sr 1 of 6 fundamental SI units
CS348B Lecture 4 Pat Hanrahan, 2004
Page 12 Irradiance
Definition: The irradiance (illuminance) is the power per unit area incident on a surface. dΦ Ex()≡ i dA
Wlm = lux mm22
Sometimes referred to as the radiant (luminous) incidence.
CS348B Lecture 4 Pat Hanrahan, 2004
Lambert’s Cosine Law
A
Φ=EA
Φ E = A
CS348B Lecture 4 Pat Hanrahan, 2004
Page 13 Lambert’s Cosine Law
A A /cosθ
Φ
θ
Φ Φ E ==cosθ AA/cosθ
CS348B Lecture 4 Pat Hanrahan, 2004
Irradiance: Isotropic Point Source
Φ I = 4π θ h r
CS348B Lecture 4 Pat Hanrahan, 2004
Page 14 Irradiance: Isotropic Point Source
Φ I = dω 4π θ h r dA
dIdEdAΦ ==ω
CS348B Lecture 4 Pat Hanrahan, 2004
Irradiance: Isotropic Point Source
Φ I = dω 4π θ h r dA
cosθ ddAω = r 2
CS348B Lecture 4 Pat Hanrahan, 2004
Page 15 Irradiance: Isotropic Point Source
Φ I = dω 4π θ h r dA Φ cosθ I ddAω = 4π r 2
CS348B Lecture 4 Pat Hanrahan, 2004
Irradiance: Isotropic Point Source
Φ I = dω 4π θ h r dA Φ cosθ I ddAEdAω == 4π r 2 Φ cosθ E = 2 CS348B Lecture 44π r Pat Hanrahan, 2004
Page 16 Irradiance: Isotropic Point Source
Φ I = dω 4π θ hr= cosθ r dA
ΦΦcosθ cos3 θ E == 44ππrh22
CS348B Lecture 4 Pat Hanrahan, 2004
Directional Power Arriving at a Surface
Lx(,ω ) i dω dA 2 θ dxΦ=ii(,ω ) Lx (,ωθω )cos dAd = Lxi (,ωω ) dAdi dx2Φ (,ω ) i dAi dω = cosθω dAd
CS348B Lecture 4 Pat Hanrahan, 2004
Page 17 Irradiance from the Environment
2 dxΦ=ii(,ω ) Lx (,ωθ )cos dAd ω Lxi (,ω ) dE( x ,ω )= Li ( x ,ωθω )cos d dω θ
dA E()xLxd= (,ω )cosθω Light meter ∫ i H2 CS348B Lecture 4 Pat Hanrahan, 2004
Typical Values of Illuminance [lm/m2]
Sunlight plus skylight 100,000 lux Sunlight plus skylight (overcast) 10,000 Interior near window (daylight) 1,000 Artificial light (minimum) 100 Moonlight (full) 0.02 Starlight 0.0003
CS348B Lecture 4 Pat Hanrahan, 2004
Page 18 The Sky Radiance Distribution
From Greenler, Rainbows, halos and glories
CS348B Lecture 4 Pat Hanrahan, 2004
Gazing Ball ⇒ Environment Maps
Miller and Hoffman, 1984
Photograph of mirror ball Maps all directions to a to circle Reflection indexed by normal Resolution function of orientation
CS348B Lecture 4 Pat Hanrahan, 2004
Page 19 Environment Maps
Interface, Chou and Williams (ca. 1985) CS348B Lecture 4 Pat Hanrahan, 2004
Irradiance Environment Maps
L(,θ ϕ ) R E(,θ ϕ ) N
Radiance Irradiance Environment Map Environment Map
CS348B Lecture 4 Pat Hanrahan, 2004
Page 20 Irradiance Map or Light Map
Isolux contours CS348B Lecture 4 Pat Hanrahan, 2004
Radiant Exitance (Radiosity)
Page 21 Radiant Exitance
Definition: The radiant (luminous) exitance is the energy per unit area leaving a surface. dΦ Mx()≡ o dA Wlm = lux mm22
In computer graphics, this quantity is often referred to as the radiosity (B)
CS348B Lecture 4 Pat Hanrahan, 2004
Directional Power Leaving a Surface
Lx(,ω ) o dω dA 2 θ dxΦ=oo(,ω ) Lx (,ωθω )cos dAd = Lxo (,ωω ) dAdi
2 dxΦo (,ω )
CS348B Lecture 4 Pat Hanrahan, 2004
Page 22 Uniform Diffuse Emitter
M = Ldcosθ ω ∫ o H2 Lo(,x ω ) = L cosθ dω o ∫ H2 dω
= πLo θ
M L = o π dA
CS348B Lecture 4 Pat Hanrahan, 2004
Projected Solid Angle Ω≡ ∫ cosθ dω Ω dω θ
cosθ dω Ω= ∫ cosθ dωπ = 2 CS348B Lecture 4H Pat Hanrahan, 2004
Page 23 Radiometry and Photometry Summary
Radiometric and Photometric Terms
Physics Radiometry Photometry
Energy Radiant Energy Luminous Energy
Flux (Power) Radiant Power Luminous Power
Flux Density Irradiance Illuminance
Radiosity Luminosity
Angular Flux Density Radiance Luminance
Intensity Radiant Intensity Luminous Intensity
CS348B Lecture 4 Pat Hanrahan, 2004
Page 24 Photometric Units
Photometry Units
MKS CGS British Luminous Energy Talbot
Luminous Power Lumen
Illuminance Lux Phot Footcandle Luminosity Luminance Nit Stilb Apostilb, Blondel Lambert Footlambert
Luminous Intensity Candela (Candle, Candlepower, Carcel, Hefner)
“Thus one nit is one lux per steradian is one candela per square meter is one lumen per square meter per steradian. Got it?”, James Kajiya
CS348B Lecture 4 Pat Hanrahan, 2004
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