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Understand the concepts of specular and diffuse reflection, Lambertian BRDF, Specular BRDF, and shape recovery from a single image. Explore techniques like Photometric Stereo to recover 3D shape from intensity variations.
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Computer Vision Spring 2010 15-385,-685 Instructor: S. Narasimhan PH A18B T-R 10:30am – 11:50am Lecture #13
Mechanisms of Reflection source incident direction surface reflection body reflection surface • Surface Reflection: • Specular Reflection • Glossy Appearance • Highlights • Dominant for Metals • Body Reflection: • Diffuse Reflection • Matte Appearance • Non-Homogeneous Medium • Clay, paper, etc Image Intensity = Body Reflection + Surface Reflection
Example Surfaces Surface Reflection: Specular Reflection Glossy Appearance Highlights Dominant for Metals Body Reflection: Diffuse Reflection Matte Appearance Non-Homogeneous Medium Clay, paper, etc Many materials exhibit both Reflections:
Diffuse Reflection and Lambertian BRDF source intensity I incident direction normal viewing direction surface element • Surface appears equally bright from ALL directions! (independent of ) albedo • Lambertian BRDF is simply a constant : • Surface Radiance : source intensity • Commonly used in Vision and Graphics!
White-out: Snow and Overcast Skies CAN’T perceive the shape of the snow covered terrain! CAN perceive shape in regions lit by the street lamp!! WHY?
Specular Reflection and Mirror BRDF source intensity I specular/mirror direction incident direction normal viewing direction surface element • Valid for very smooth surfaces. • All incident light energy reflected in a SINGLE direction (only when = ). • Mirror BRDF is simply a double-delta function : specular albedo • Surface Radiance :
Combing Specular and Diffuse: Dichromatic Reflection Observed Image Color = a x Body Color + b x Specular Reflection Color Klinker-Shafer-Kanade 1988 R Color of Source (Specular reflection) Does not specify any specific model for Diffuse/specular reflection G Color of Surface (Diffuse/Body Reflection) B
Diffuse and Specular Reflection diffuse specular diffuse+specular
Photometric Stereo Lecture #9
Image Intensity and 3D Geometry • Shading as a cue for shape reconstruction • What is the relation between intensity and shape? • Reflectance Map
Equation of plane or Let Surface normal Surface Normal surface normal
Normal vector Source vector plane is called the Gradient Space (pq plane) • Every point on it corresponds to a particular surface orientation Gradient Space
: source brightness : surface albedo (reflectance) : constant (optical system) Image irradiance: Let then Reflectance Map • Relates image irradiance I(x,y) to surface orientation (p,q) for given source direction and surface reflectance • Lambertian case:
Reflectance Map (Lambertian) Iso-brightness contour cone of constant Reflectance Map • Lambertian case
Reflectance Map iso-brightness contour • Lambertian case Note: is maximum when
Diffuse peak Specular peak Reflectance Map • Glossy surfaces (Torrance-Sparrow reflectance model) diffuse term specular term
Shape from a Single Image? • Given a single image of an object with known surface reflectance taken under a known light source, can we recover the shape of the object? • Given R(p,q) ( (pS,qS) and surface reflectance) can we determine (p,q) uniquely for each image point? NO
Solution • Take more images • Photometric stereo • Add more constraints • Shape-from-shading (next class)
Photometric Stereo Lambertian case: Image irradiance: • We can write this in matrix form:
inverse Solving the Equations
Least squares solution: Moore-Penrose pseudo inverse • Solve for as before More than Three Light Sources • Get better results by using more lights
Color Images • The case of RGB images • get three sets of equations, one per color channel: • Simple solution: first solve for using one channel • Then substitute known into above equations to get • Or combine three channels and solve for
Computing light source directions • Trick: place a chrome sphere in the scene • the location of the highlight tells you the source direction
Specular Reflection - Recap • For a perfect mirror, light is reflected about N • We see a highlight when • Then is given as follows:
Computing the Light Source Direction Chrome sphere that has a highlight at position h in the image • Can compute N by studying this figure • Hints: • use this equation: • can measure c, h, and r in the image N h H rN c C sphere in 3D image plane
Limitations • Big problems • Doesn’t work for shiny things, semi-translucent things • Shadows, inter-reflections • Smaller problems • Camera and lights have to be distant • Calibration requirements • measure light source directions, intensities • camera response function
Trick for Handling Shadows • Weight each equation by the pixel brightness: • Gives weighted least-squares matrix equation: • Solve for as before
Results: Lambertian Sphere Input Images Needles are projections of surface normals on image plane Estimated Surface Normals Estimated Albedo
Results: Lambertian Toy I.2 Input Images Estimated Surface Normals Estimated Albedo
V2 V1 N Depth from Normals • Get a similar equation for V2 • Each normal gives us two linear constraints on z • compute z values by solving a matrix equation
Results • Estimate light source directions • Compute surface normals • Compute albedo values • Estimate depth from surface normals • Relight the object (with original texture and uniform albedo)
Results - Albedo No Shading Information
Results - Shape Shallow reconstruction (effect of interreflections) Accurate reconstruction (after removing interreflections)
Next Class • Shape from Shading • Reading: Horn, Chapter 11.