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Image formation
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Camera: optical system
da=a -a 2 1 curvature radius r r Z 1 2 thin lens small angles:
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Y incident light beam lens refraction index: n deviated beam Z deviation angle ? Dq = q’’-q
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Thin lens rules a) Y=0 Dq = 0 f Dq
beams through lens center: undeviated b) f Dq = Y independent of y parallel rays converge onto a focal plane Y f Dq
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f r Where do all rays starting from a scene point P converge ? P Y O Z
Fresnel law Obs. For Z ∞, r f
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f d if d ≠ r … image of a point = blurring circle image plane Z P O a
F(blurring circle)=a (d-r)/r r focussed image: F(blurring circle) <image resolution d depth of field: range [Z1, Z2] where image is focussed
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Hp: Z >> a r f the image of a point P belongs to the line (P,O) P image plane O p p = image of P = image plane ∩ line(O,P) interpretation line of p: line(O,p) = locus of the scene points projecting onto image point p
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Until here: where goes light ? But: how much light does reach an image point?
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Image Formation: Reflectance Map
Simplified model: light originates at a source light is reflected by an object light collected by camera lens and focused to image [adapted from Hemant D. Tagare]
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Reflectance Map dA at P receives flux of d watt: Irradiance at P:
(watt/meter2, spatial density of flux at P)
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reflectance map ctd. d infinitesimal solid angle, centered along incident direction infinitesimal flux d2 passes through it, incident on dA ,: zenith,azimuth dA cos : fore-shortened area dAf Radiance of incident flux: Units: watt per m2 per steradian
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reflectance map ctd. Radiant intensity of flux: Object is a point (no area) flux d incident on it from solid angle d units: watt per steradian
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Solid Angle Solid angle d: solid angle centered around direction ,
spherical geometry: dA = r2 sin dd
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Computation of flux Flux :
irradiance E and radiance L are derivatives of flux flux comp. as integral L(P,,): radiance along , at any point P of surface E(P): irradiance at P : net flux received by object and,
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Generalization: Reflected Light
so far: radiance and radiant intensity defined in terms of incident light definitions also apply to reflected / emitted light flux d is assumed to have reverse direction (leaves surface) radiance of reflected light (dA through d) :
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a f Z image intensity: proportional to irradiance E where is the radiance reflected towards the lens
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