Shapes

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Shapes. Digital Image Synthesis Yung-Yu Chuang 10/04/2007. with slides by Pat Hanrahan. Announcements. One break or two breaks. Please do read the textbook and trace code. LootAt issue. No class on 10/18 because of attending CGW 2007. - PowerPoint PPT Presentation

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Shapes

Digital Image SynthesisYung-Yu Chuang10/04/2007

with slides by Pat Hanrahan

Announcements

• One break or two breaks.• Please do read the textbook and trace code.• LootAt issue.• No class on 10/18 because of attending CGW 2

007.• Assignment #1 will be handed out today. Due t

hree weeks later.

Shapes

• One advantages of ray tracing is it can support various kinds of shapes as long as we can find ray-shape intersection.

• Careful abstraction of geometric shapes is a key component for a ray tracer. Ideal candidate for object-oriented design. Scan conversion may not have such a neat interface.

• All shape classes implement the same interface and the other parts of the ray tracer just use this interface without knowing the details about this shape.

Shapes

• Primitive=Shape+Material• Shape: raw geometry properties of the primitiv

e, implements interface such as surface area and bounding box.

• Source code in core/shape.* and shapes/*

Shapes

• pbrt provides the following shape plug-ins: – quadrics: sphere, cone, cylinder, disk, hyperboloid

(雙曲面 ), paraboloid(拋物面 ) (surface described by quadratic polynomials in x, y, z)

– triangle mesh– height field– NURBS– Loop subdivision surface

• Some possible extensions: other subdivision schemes, fractals, CSG, point-sampled geometry

Shapes

class Shape : public ReferenceCounted {public: <Shape Interface> all are virtual functions const Transform ObjectToWorld, WorldToObject; const bool reverseOrientation, transformSwapsHandedness;}

• All shapes are defined in object coordinate space

Shape interface: bounding

• BBox ObjectBound() const=0;pure virtual function• BBox WorldBound() { left to individual shape default implementation; can be overridden return ObjectToWorld(ObjectBound());

}

Shape interface: intersecting

• bool CanIntersect() returns whether this shape can do intersection test; if not, the shape must provide

void Refine(vector<Reference<Shape>>&refined)

examples include complex surfaces (which need to be tessellated first) or placeholders (which store geometry information in the disk)

• bool Intersect(const Ray &ray,

float *tHit, DifferentialGeometry *dg)• bool IntersectP(const Ray &ray)

not pure virtual functions so that non-intersectable shapes don’t need to implement them; instead, a default implementation which prints error is provided.

in world space

Differential geometry

• DifferentialGeometry: a self-contained representation for a particular point on a surface so that all the other operations in pbrt can be executed without referring to the original shape. It contains

• Position• Parameterization (u,v)• Parametric derivatives (dp/du, dp/dv)• Surface normal (derived from (dp/du)x(dp/dv))• Derivatives of normals• Pointer to shape

Shape interface• float Area() useful when using as a area light• void GetShadingGeometry( const Transform &obj2world, const DifferentialGeometry &dg, DifferentialGeometry *dgShading)

• No back culling for that it doesn’t save much for ray tracing and it is not physically correct

for object instancing

Surfaces

• Implicit: F(x,y,z)=0 you can check• Explicit: (x(u,v),y(u,v),z(u,v)) you can enumerate also called parametric • Quadrics

0

1

1

z

y

x

JIGD

IHFC

GFEB

DCBA

zyx

Sphere

• A sphere of radius r at the origin• Implicit: x2+y2+z2-r2=0

• Parametric: f(θ,ψ)

x=rsinθcosψ

y=rsinθsinψ

z=rcosθ

mapping f(u,v) over [0,1]2

ψ=uψmax

θ=θmin+v(θmax-θmin)

useful for texture mapping

θ

Sphere

Sphere (construction)

class Sphere: public Shape {

……

private:

float radius;

float phiMax;

float zmin, zmax;

float thetaMin, thetaMax;

}

Sphere(const Transform &o2w, bool ro, float rad, float zmin, float zmax,

float phiMax);

• Bounding box for sphere, only z clipping

thetas are derived from z

Intersection (algebraic solution)

• Perform in object space, WorldToObject(r, &ray)• Assume that ray is normalized for a while

2222 rzyx

2222 rtdotdotdo zzyyxx

02 CBtAt

222zyx dddA

)(2 zzyyxx odododB 2222 roooC zyx

Step 1

Algebraic solution

A

ACBBt

2

42

0

A

ACBBt

2

42

1

If (B2-4AC<0) then the ray misses the sphereStep 2

Step 3

Calculate t0 and test if t0<0 (actually mint, maxt)Step 4

Calculate t1 and test if t1<0

check the real source code in sphere.cpp

Quadric (in pbrt.h)inline bool Quadratic(float A, float B, float C, float *t0, float *t1) { // Find quadratic discriminant float discrim = B * B - 4.f * A * C; if (discrim < 0.) return false; float rootDiscrim = sqrtf(discrim); // Compute quadratic _t_ values float q; if (B < 0) q = -.5f * (B - rootDiscrim); else q = -.5f * (B + rootDiscrim); *t0 = q / A; *t1 = C / q; if (*t0 > *t1) swap(*t0, *t1); return true;}

Why?

• Cancellation error: devastating loss of precision when small numbers are computed from large numbers by addition or subtraction.

double x1 = 10.000000000000004; double x2 = 10.000000000000000;

double y1 = 10.00000000000004;

double y2 = 10.00000000000000;

double z = (y1 - y2) / (x1 - x2); // 11.5

A

qt 0

q

Ct 1

otherwise 42

1

0 if 42

1

2

2

ACBB

BACBBq

Range checking

if (t0 > ray.maxt || t1 < ray.mint) return false;float thit = t0;if (t0 < ray.mint) {

thit = t1;if (thit > ray.maxt) return false;

} ...

phit = ray(thit);phi = atan2f(phit.y, phit.x);if (phi < 0.) phi += 2.f*M_PI;// Test sphere intersection against clipping parametersif (phit.z < zmin || phit.z > zmax || phi > phiMax) { ... // see if we should check another hit point}

Geometric solution

1. Origin inside? 2222 rooo zyx

Geometric solution

2. find the closest point, t=-O‧D if t<0 and O outside return false

t

t

D is normalized

Geometric solution

3. find the distance to the origin, d2=O2-t2

if s2=r2-d2<0 return false;

t

rrd

O

s

Geometric solution

4. calculate intersection distance, if (origin outside) then t-s else t+s

t

rd

O

s

t

r

d

O

s

Sphere

• Have to test sphere intersection against clipping parameters

• Fill in information for DifferentialGeometry– Position– Parameterization (u,v)– Parametric derivatives– Surface normal– Derivatives of normals– Pointer to shape

Partial sphere

u=ψ/ψmax

v=(θ-θmin)/ (θmax-θmin)

• Partial derivatives (pp103 of textbook)

• Area (pp107)

)0,,( maxmax xyu

p

)sin,sin,cos)(( minmax rzzv

p

)( minmaxmax zzrA

Cylinder

max ucosrx sinry

)( minmaxmin zzvzz

Cylinder

Cylinder (intersection)

222 ryx

222 rtdotdo yyxx

02 CBtAt

22yx ddA

)(2 yyxx ododB 222 rooC yx

Disk

max ucos))1(( vrrvx i

hz

sin))1(( vrrvy i

Disk

Disk (intersection)

h-Oz

h

t

Dz Dzz Oh

t

D

D

)( zz

OhD

Dt

z

z

D

Oh

D

tt

'

Other quadrics

0)( 222

hzr

hy

r

hx

conehyperboloidparaboloid

1222 zyx02

2

2

2

zr

hy

r

hx

Triangle mesh

The most commonly used shape. In pbrt, it can be supplied by users or tessellated from other shapes. Some ray tracers only support triangle meshes.

Triangle mesh

class TriangleMesh : public Shape {… int ntris, nverts; int *vertexIndex; Point *p; Normal *n; per vertex Vector *s; tangent float *uvs; parameters}

x,y,z x,y,z x,y,z x,y,z x,y,z…

vi[3*i]

vi[3*i+1]

vi[3*i+2]

p

Note that p is stored in world space to save transformations. n and s are in object space.

Triangle mesh

Pbrt calls Refine() when it encounters a shape that is not intersectable. (usually, refine is done in acceleration structure creation)

Void TriangleMesh::Refine(vector<Reference<Shape>>

&refined)

{

for (int i = 0; i < ntris; ++i)

refined.push_back(new Triangle(ObjectToWorld,

reverseOrientation, (TriangleMesh *)this, i));

}Triangle only stores a pointer to mesh and an index.

1. Intersect ray with plane2. Check if point is inside triangle

Ray triangle intersection

Algebraic Method

0:

: 0

dNPPlane

tVPPRay

Substituting for P, we get:

00 dNtVP

Solution:

NV

dNPt

0

tVPP 0

Ray plane intersection

Algebraic Method

FALSEreturn

dNPif

NPd

NNormalize

VVN

PTV

PTV

011

101

1

211

022

011

For each side of triangle:

end

Ray triangle intersection I

Parametric Method

triangleinsideisPthen

and

andif

TTTTP

Compute

0.1

0.10.00.10.0

:,

1312

Ray triangle intersection II

Ray triangle intersection III

Fast minimum storage intersection

210)1( vVuVVvutDO 1 and 0, vuvu

00201 VO

v

u

t

VVVVD

a point on the ray

a point inside the triangle

Fast minimum storage intersection

00201 VO

v

u

t

VVVVD

O

D

V0

V1

V2O

D

V0

V1

V2 1

1

Fast minimum storage intersection

011 VVE 022 VVE 0VOT

00201 VO

v

u

t

VVVVD

T

v

u

t

EED

21

Fast minimum storage intersection• Cramer’s rule

TED

ETD

EET

EEDv

u

t

,,

,,

,,

,,

1

1

2

21

21

T

v

u

t

EED

21

ABCBCACBA )()(,,

Fast minimum storage intersection

2EDP 1ETQ

DQ

TP

EQ

EPv

u

t 2

1

1

TED

ETD

EET

EEDv

u

t

,,

,,

,,

,,

1

1

2

21

21

Triangle

P0

(u0, v0)P1

(u1, v1)

P2

(u2, v2)

v

pv

u

pupp iii

0

32

31

3232

3131

pp

pp

vp

up

vvuu

vvuu

32

31

1

3232

3131

pp

pp

vvuu

vvuu

vp

up

P(u,v)

Shading geometry

if (!mesh->n && !mesh->s) {

*dgShading = dg;

return;

}

// compute Barycentric coordinate

1210

221100

221100

bbb

vbvbvbv

ubububu

0

0

2

1

0201

0201

vv

uu

b

b

vvvv

uuuu

Shading geometry Normal ns; Vector ss, ts;if (mesh->n)

ns = Normalize(obj2world( b[0] * mesh->n[v[0]] + b[1] * mesh->n[v[1]] + b[2] * mesh->n[v[2]])); else ns = dg.nn; if (mesh->s) ss = Normalize(obj2world( b[0] * mesh->s[v[0]] + b[1] * mesh->s[v[1]] + b[2] * mesh->s[v[2]])); else ss = Normalize(dg.dpdu);

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