3D Sensing and ReconstructionReadings Ch 12 125-6 Ch 13 131-3 1394

bull Perspective Geometry

bull Camera Model

bull Stereo Triangulation

bull 3D Reconstruction by Space Carving

3D Shape from Xmeans getting 3D coordinates

from different methods

bull shadingbull silhouettebull texture

bull stereo bull light stripingbull motion

mainly research

used in practice

Perspective Imaging Model 1D

xi

xf

f

This is the axis of the real image plane

O O is the center of projection

This is the axis of the frontimage plane which we usezc

xc

xi xc

f zc

=

camera lens

3D objectpoint

B

D

E

image of pointB in front image

real imagepoint

Perspective in 2D(Simplified)

P=(xcyczc) =(xwywzw)

3D object point

xc

yc

zw=zc

yi

Yc

Xc

Zc

xi

F f

cameraPacute=(xiyif)

xi xc

f zc

yi yc

f zc

=

=

xi = (fzc)xc

yi = (fzc)ycHere camera coordinatesequal world coordinates

opticalaxis

ray

3D from Stereo

left image right image

3D point

disparity the difference in image location of the same 3Dpoint when projected under perspective to two different cameras

d = xleft - xright

Depth Perception from StereoSimple Model Parallel Optic Axes

f

f

L

R

camera

baselinecamera

b

P=(xz)

Z

X

image plane

xl

xr

z

z xf xl

=

x-b

z x-bf xr

= z y yf yl yr

= =y-axis is

perpendicularto the page

Resultant Depth Calculation

For stereo cameras with parallel optical axes focal length fbaseline b corresponding image points (xlyl) and (xryr)with disparity d

z = fb (xl - xr) = fbd

x = xlzf or b + xrzf

y = ylzf or yrzf

This method ofdetermining depthfrom disparity is called triangulation

Finding Correspondences

bull If the correspondence is correct triangulation works VERY well

bull But correspondence finding is not perfectly solved (What methods have we studied)

bull For some very specific applications it can be solved for those specific kind of images eg windshield of a car

deg deg

3 Main Matching Methods

1 Cross correlation using small windows

2 Symbolic feature matching usually using segmentscorners

3 Use the newer interest operators ie SIFT

dense

sparse

sparse

Epipolar Geometry Constraint1 Normal Pair of Images

x

y1

y2

z1 z2

C1 C2b

P

P1 P2

epipolarplane

The epipolar plane cuts through the image plane(s)forming 2 epipolar lines

The match for P1 (or P2) in the other image must lie on the same epipolar line

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

3D Shape from Xmeans getting 3D coordinates

from different methods

bull shadingbull silhouettebull texture

bull stereo bull light stripingbull motion

mainly research

used in practice

Perspective Imaging Model 1D

xi

xf

f

This is the axis of the real image plane

O O is the center of projection

This is the axis of the frontimage plane which we usezc

xc

xi xc

f zc

=

camera lens

3D objectpoint

B

D

E

image of pointB in front image

real imagepoint

Perspective in 2D(Simplified)

P=(xcyczc) =(xwywzw)

3D object point

xc

yc

zw=zc

yi

Yc

Xc

Zc

xi

F f

cameraPacute=(xiyif)

xi xc

f zc

yi yc

f zc

=

=

xi = (fzc)xc

yi = (fzc)ycHere camera coordinatesequal world coordinates

opticalaxis

ray

3D from Stereo

left image right image

3D point

disparity the difference in image location of the same 3Dpoint when projected under perspective to two different cameras

d = xleft - xright

Depth Perception from StereoSimple Model Parallel Optic Axes

f

f

L

R

camera

baselinecamera

b

P=(xz)

Z

X

image plane

xl

xr

z

z xf xl

=

x-b

z x-bf xr

= z y yf yl yr

= =y-axis is

perpendicularto the page

Resultant Depth Calculation

For stereo cameras with parallel optical axes focal length fbaseline b corresponding image points (xlyl) and (xryr)with disparity d

z = fb (xl - xr) = fbd

x = xlzf or b + xrzf

y = ylzf or yrzf

This method ofdetermining depthfrom disparity is called triangulation

Finding Correspondences

bull If the correspondence is correct triangulation works VERY well

bull But correspondence finding is not perfectly solved (What methods have we studied)

bull For some very specific applications it can be solved for those specific kind of images eg windshield of a car

deg deg

3 Main Matching Methods

1 Cross correlation using small windows

2 Symbolic feature matching usually using segmentscorners

3 Use the newer interest operators ie SIFT

dense

sparse

sparse

Epipolar Geometry Constraint1 Normal Pair of Images

x

y1

y2

z1 z2

C1 C2b

P

P1 P2

epipolarplane

The epipolar plane cuts through the image plane(s)forming 2 epipolar lines

The match for P1 (or P2) in the other image must lie on the same epipolar line

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Perspective Imaging Model 1D

xi

xf

f

This is the axis of the real image plane

O O is the center of projection

This is the axis of the frontimage plane which we usezc

xc

xi xc

f zc

=

camera lens

3D objectpoint

B

D

E

image of pointB in front image

real imagepoint

Perspective in 2D(Simplified)

P=(xcyczc) =(xwywzw)

3D object point

xc

yc

zw=zc

yi

Yc

Xc

Zc

xi

F f

cameraPacute=(xiyif)

xi xc

f zc

yi yc

f zc

=

=

xi = (fzc)xc

yi = (fzc)ycHere camera coordinatesequal world coordinates

opticalaxis

ray

3D from Stereo

left image right image

3D point

disparity the difference in image location of the same 3Dpoint when projected under perspective to two different cameras

d = xleft - xright

Depth Perception from StereoSimple Model Parallel Optic Axes

f

f

L

R

camera

baselinecamera

b

P=(xz)

Z

X

image plane

xl

xr

z

z xf xl

=

x-b

z x-bf xr

= z y yf yl yr

= =y-axis is

perpendicularto the page

Resultant Depth Calculation

For stereo cameras with parallel optical axes focal length fbaseline b corresponding image points (xlyl) and (xryr)with disparity d

z = fb (xl - xr) = fbd

x = xlzf or b + xrzf

y = ylzf or yrzf

This method ofdetermining depthfrom disparity is called triangulation

Finding Correspondences

bull If the correspondence is correct triangulation works VERY well

bull But correspondence finding is not perfectly solved (What methods have we studied)

bull For some very specific applications it can be solved for those specific kind of images eg windshield of a car

deg deg

3 Main Matching Methods

1 Cross correlation using small windows

2 Symbolic feature matching usually using segmentscorners

3 Use the newer interest operators ie SIFT

dense

sparse

sparse

Epipolar Geometry Constraint1 Normal Pair of Images

x

y1

y2

z1 z2

C1 C2b

P

P1 P2

epipolarplane

The epipolar plane cuts through the image plane(s)forming 2 epipolar lines

The match for P1 (or P2) in the other image must lie on the same epipolar line

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Perspective in 2D(Simplified)

P=(xcyczc) =(xwywzw)

3D object point

xc

yc

zw=zc

yi

Yc

Xc

Zc

xi

F f

cameraPacute=(xiyif)

xi xc

f zc

yi yc

f zc

=

=

xi = (fzc)xc

yi = (fzc)ycHere camera coordinatesequal world coordinates

opticalaxis

ray

3D from Stereo

left image right image

3D point

disparity the difference in image location of the same 3Dpoint when projected under perspective to two different cameras

d = xleft - xright

Depth Perception from StereoSimple Model Parallel Optic Axes

f

f

L

R

camera

baselinecamera

b

P=(xz)

Z

X

image plane

xl

xr

z

z xf xl

=

x-b

z x-bf xr

= z y yf yl yr

= =y-axis is

perpendicularto the page

Resultant Depth Calculation

For stereo cameras with parallel optical axes focal length fbaseline b corresponding image points (xlyl) and (xryr)with disparity d

z = fb (xl - xr) = fbd

x = xlzf or b + xrzf

y = ylzf or yrzf

This method ofdetermining depthfrom disparity is called triangulation

Finding Correspondences

bull If the correspondence is correct triangulation works VERY well

bull But correspondence finding is not perfectly solved (What methods have we studied)

bull For some very specific applications it can be solved for those specific kind of images eg windshield of a car

deg deg

3 Main Matching Methods

1 Cross correlation using small windows

2 Symbolic feature matching usually using segmentscorners

3 Use the newer interest operators ie SIFT

dense

sparse

sparse

Epipolar Geometry Constraint1 Normal Pair of Images

x

y1

y2

z1 z2

C1 C2b

P

P1 P2

epipolarplane

The epipolar plane cuts through the image plane(s)forming 2 epipolar lines

The match for P1 (or P2) in the other image must lie on the same epipolar line

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

3D from Stereo

left image right image

3D point

disparity the difference in image location of the same 3Dpoint when projected under perspective to two different cameras

d = xleft - xright

Depth Perception from StereoSimple Model Parallel Optic Axes

f

f

L

R

camera

baselinecamera

b

P=(xz)

Z

X

image plane

xl

xr

z

z xf xl

=

x-b

z x-bf xr

= z y yf yl yr

= =y-axis is

perpendicularto the page

Resultant Depth Calculation

For stereo cameras with parallel optical axes focal length fbaseline b corresponding image points (xlyl) and (xryr)with disparity d

z = fb (xl - xr) = fbd

x = xlzf or b + xrzf

y = ylzf or yrzf

This method ofdetermining depthfrom disparity is called triangulation

Finding Correspondences

bull If the correspondence is correct triangulation works VERY well

bull But correspondence finding is not perfectly solved (What methods have we studied)

bull For some very specific applications it can be solved for those specific kind of images eg windshield of a car

deg deg

3 Main Matching Methods

1 Cross correlation using small windows

2 Symbolic feature matching usually using segmentscorners

3 Use the newer interest operators ie SIFT

dense

sparse

sparse

Epipolar Geometry Constraint1 Normal Pair of Images

x

y1

y2

z1 z2

C1 C2b

P

P1 P2

epipolarplane

The epipolar plane cuts through the image plane(s)forming 2 epipolar lines

The match for P1 (or P2) in the other image must lie on the same epipolar line

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Depth Perception from StereoSimple Model Parallel Optic Axes

f

f

L

R

camera

baselinecamera

b

P=(xz)

Z

X

image plane

xl

xr

z

z xf xl

=

x-b

z x-bf xr

= z y yf yl yr

= =y-axis is

perpendicularto the page

Resultant Depth Calculation

For stereo cameras with parallel optical axes focal length fbaseline b corresponding image points (xlyl) and (xryr)with disparity d

z = fb (xl - xr) = fbd

x = xlzf or b + xrzf

y = ylzf or yrzf

This method ofdetermining depthfrom disparity is called triangulation

Finding Correspondences

bull If the correspondence is correct triangulation works VERY well

bull But correspondence finding is not perfectly solved (What methods have we studied)

bull For some very specific applications it can be solved for those specific kind of images eg windshield of a car

deg deg

3 Main Matching Methods

1 Cross correlation using small windows

2 Symbolic feature matching usually using segmentscorners

3 Use the newer interest operators ie SIFT

dense

sparse

sparse

Epipolar Geometry Constraint1 Normal Pair of Images

x

y1

y2

z1 z2

C1 C2b

P

P1 P2

epipolarplane

The epipolar plane cuts through the image plane(s)forming 2 epipolar lines

The match for P1 (or P2) in the other image must lie on the same epipolar line

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Resultant Depth Calculation

For stereo cameras with parallel optical axes focal length fbaseline b corresponding image points (xlyl) and (xryr)with disparity d

z = fb (xl - xr) = fbd

x = xlzf or b + xrzf

y = ylzf or yrzf

This method ofdetermining depthfrom disparity is called triangulation

Finding Correspondences

bull If the correspondence is correct triangulation works VERY well

bull But correspondence finding is not perfectly solved (What methods have we studied)

bull For some very specific applications it can be solved for those specific kind of images eg windshield of a car

deg deg

3 Main Matching Methods

1 Cross correlation using small windows

2 Symbolic feature matching usually using segmentscorners

3 Use the newer interest operators ie SIFT

dense

sparse

sparse

Epipolar Geometry Constraint1 Normal Pair of Images

x

y1

y2

z1 z2

C1 C2b

P

P1 P2

epipolarplane

The epipolar plane cuts through the image plane(s)forming 2 epipolar lines

The match for P1 (or P2) in the other image must lie on the same epipolar line

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Finding Correspondences

bull If the correspondence is correct triangulation works VERY well

bull But correspondence finding is not perfectly solved (What methods have we studied)

bull For some very specific applications it can be solved for those specific kind of images eg windshield of a car

deg deg

3 Main Matching Methods

1 Cross correlation using small windows

2 Symbolic feature matching usually using segmentscorners

3 Use the newer interest operators ie SIFT

dense

sparse

sparse

Epipolar Geometry Constraint1 Normal Pair of Images

x

y1

y2

z1 z2

C1 C2b

P

P1 P2

epipolarplane

The epipolar plane cuts through the image plane(s)forming 2 epipolar lines

The match for P1 (or P2) in the other image must lie on the same epipolar line

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

3 Main Matching Methods

1 Cross correlation using small windows

2 Symbolic feature matching usually using segmentscorners

3 Use the newer interest operators ie SIFT

dense

sparse

sparse

Epipolar Geometry Constraint1 Normal Pair of Images

x

y1

y2

z1 z2

C1 C2b

P

P1 P2

epipolarplane

The epipolar plane cuts through the image plane(s)forming 2 epipolar lines

The match for P1 (or P2) in the other image must lie on the same epipolar line

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Epipolar Geometry Constraint1 Normal Pair of Images

x

y1

y2

z1 z2

C1 C2b

P

P1 P2

epipolarplane

The epipolar plane cuts through the image plane(s)forming 2 epipolar lines

The match for P1 (or P2) in the other image must lie on the same epipolar line

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Epipolar GeometryGeneral Case

P

P1

P2

y1

y2

x1

x2

e1

e2

C1

C2

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Constraints

P

e1

e2

C1

C2

1 Epipolar Constraint Matching points lie on corresponding epipolar lines

2 Ordering Constraint Usually in the same order across the lines

Q

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Structured Light

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

camera

light stripe

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Structured Light3D Computation

3D data can also be derived using

bull a single camera

bull a light source that can produce stripe(s) on the 3D object

lightsource

x axisf

(xacuteyacutef)

3D point(x y z)

b

b[x y z] = --------------- [xacute yacute f] f cot - xacute

(000)

3D image

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Depth from Multiple Light Stripes

What are these objects

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Our (former) System4-camera light-striping stereo

projector

rotationtable

cameras

3Dobject

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Camera Model Recall there are 5 Different Frames of Reference

bull Object

bull World

bull Camera

bull Real Image

bull Pixel Image

yc

xc

zc

zwC

Wyw

xw

A

a

xf

yf

xp

yp

zppyramidobject

image

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

The Camera Model

How do we get an image point IP from a world point P

c11 c12 c13 c14

c21 c22 c23 c24

c31 c32 c33 1

s IPr

s IPc

s

Px

Py

Pz

1

=

imagepoint

camera matrix C worldpoint

Whatrsquos in C

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates

1 CP = T R WP2 FP = (f) CP

s FPx

s FPy

s FPz

s

1 0 0 00 1 0 00 0 1 00 0 1f 0

CPx

CPy

CPz

1

=

perspectivetransformation

imagepoint

3D point incamera

coordinates

Why is there not a scale factor here

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Camera Calibration

bull In order work in 3D we need to know the parameters of the particular camera setup

bull Solving for the camera parameters is called calibration

yw

xwzw

W

yc

xc

zc

C

bull intrinsic parameters are of the camera device

bull extrinsic parameters are where the camera sits in the world

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Intrinsic Parameters

bull principal point (u0v0)

bull scale factors (dxdy)

bull aspect ratio distortion factor

bull focal length f

bull lens distortion factor (models radial lens distortion)

C

(u0v0)

f

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Extrinsic Parameters

bull translation parameters t = [tx ty tz]

bull rotation matrix

r11 r12 r13 0r21 r22 r23 0r31 r32 r33 00 0 0 1

R = Are there reallynine parameters

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Calibration Object

The idea is to snapimages at differentdepths and get alot of 2D-3D pointcorrespondences

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

The Tsai Procedure

bull The Tsai procedure was developed by Roger Tsai at IBM Research and is most widely used

bull Several images are taken of the calibration object yielding point correspondences at different distances

bull Tsairsquos algorithm requires n gt 5 correspondences

(xi yi zi) (ui vi)) | i = 1hellipn

between (real) image points and 3D points

bull Lots of details in Chapter 13

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

We use the camera parameters of each camera for general

stereoP

P1=(r1c1)P2=(r2c2)

y1

y2

x1

x2

e1

e2

B

C

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

For a correspondence (r1c1) inimage 1 to (r2c2) in image 2

1 Both cameras were calibrated Both camera matrices are then known From the two camera equations B and C we get 4 linear equations in 3 unknowns

r1 = (b11 - b31r1)x + (b12 - b32r1)y + (b13-b33r1)zc1 = (b21 - b31c1)x + (b22 - b32c1)y + (b23-b33c1)z

r2 = (c11 - c31r2)x + (c12 - c32r2)y + (c13 - c33r2)zc2 = (c21 - c31c2)x + (c22 - c32c2)y + (c23 - c33c2)z

Direct solution uses 3 equations wonrsquot give reliable results

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

Solve by computing the closestapproach of the two skew rays

V

If the rays intersected perfectly in 3D the intersection would be PInstead we solve for the shortest line segment connecting the two rays and let P be its midpoint

P1

Q1

Psolve forshortest

V = (P1 + a1u1) ndash (Q1 + a2u2)

(P1 + a1u1) ndash (Q1 + a2u2) u1 = 0(P1 + a1u1) ndash (Q1 + a2u2) u2 = 0

u1

u2

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40

• 3D Sensing and Reconstruction Readings Ch 12 125-6 Ch 13 131-3 1394
• 3D Shape from X means getting 3D coordinates from different methods
• Perspective Imaging Model 1D
• Perspective in 2D (Simplified)
• 3D from Stereo
• Depth Perception from Stereo Simple Model Parallel Optic Axes
• Resultant Depth Calculation
• Finding Correspondences
• 3 Main Matching Methods
• Epipolar Geometry Constraint 1 Normal Pair of Images
• Epipolar Geometry General Case
• Constraints
• Structured Light
• Structured Light 3D Computation
• Depth from Multiple Light Stripes
• Our (former) System 4-camera light-striping stereo
• Camera Model Recall there are 5 Different Frames of Reference
• The Camera Model
• The camera model handles the rigid body transformation from world coordinates to camera coordinates plus the perspective transformation to image coordinates
• Camera Calibration
• Intrinsic Parameters
• Extrinsic Parameters
• Calibration Object
• The Tsai Procedure
• We use the camera parameters of each camera for general stereo
• For a correspondence (r1c1) in image 1 to (r2c2) in image 2
• Solve by computing the closest approach of the two skew rays
• Slide 28
• Slide 29
• Slide 30
• Slide 31
• Slide 32
• Slide 33
• Slide 34
• Slide 35
• Slide 36
• Slide 37
• Slide 38
• Slide 39
• Slide 40