Skip to main content Accessibility help
×
Hostname: page-component-cd9895bd7-gxg78 Total loading time: 0 Render date: 2024-12-25T12:45:00.656Z Has data issue: false hasContentIssue false

14 - Affine Epipolar Geometry

Published online by Cambridge University Press:  25 January 2011

Richard Hartley
Affiliation:
Australian National University, Canberra
Andrew Zisserman
Affiliation:
University of Oxford
Get access

Summary

This chapter recapitulates the developments and objectives of the previous chapters on two-view geometry, but here with affine cameras replacing projective cameras. The affine camera is an extremely usable and well conditioned approximation in many practical situations. Its great advantage is that, because of its linearity, many of the optimal algorithms can be implemented by linear algebra (matrix inverses, SVD etc.), whereas in the projective case solutions either involve high order polynomials (such as for triangulation) or are only possible by numerical minimization (such as in the Gold Standard estimation of F).

We first describe properties of the epipolar geometry of two affine cameras, and its optimal computation from point correspondences. This is followed by triangulation, and affine reconstruction. Finally the ambiguities in reconstruction that result from parallel projection are sketched, and the non-ambiguous motion parameters are computed from the epipolar geometry.

Affine epipolar geometry

In many respects the epipolar geometry of two affine cameras is identical to that of two perspective cameras, for example a point in one view defines an epipolar line in the other view, and the pencil of such epipolar lines intersect at the epipole. The difference is that because the cameras are affine their centres are at infinity, and there is parallel projection from scene to image. This leads to certain simplifications in the affine epipolar geometry:

Epipolar lines. Consider two points, x1, x2, in the first view. These points backproject to rays which are parallel in 3-space, since all projection rays are parallel.

Type
Chapter
Information
Publisher: Cambridge University Press
Print publication year: 2004

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

Save book to Kindle

To save this book to your Kindle, first ensure no-reply@cambridge.org is added to your Approved Personal Document E-mail List under your Personal Document Settings on the Manage Your Content and Devices page of your Amazon account. Then enter the ‘name’ part of your Kindle email address below. Find out more about saving to your Kindle.

Note you can select to save to either the @free.kindle.com or @kindle.com variations. ‘@free.kindle.com’ emails are free but can only be saved to your device when it is connected to wi-fi. ‘@kindle.com’ emails can be delivered even when you are not connected to wi-fi, but note that service fees apply.

Find out more about the Kindle Personal Document Service.

Available formats
×

Save book to Dropbox

To save content items to your account, please confirm that you agree to abide by our usage policies. If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. Find out more about saving content to Dropbox.

Available formats
×

Save book to Google Drive

To save content items to your account, please confirm that you agree to abide by our usage policies. If this is the first time you use this feature, you will be asked to authorise Cambridge Core to connect with your account. Find out more about saving content to Google Drive.

Available formats
×