Precision optical systems with performance characterization and uses thereof

• US 20090225165A1
• Filed: 12/05/2008
• Published: 09/10/2009
• Est. Priority Date: 09/08/2005
• Status: Active Grant

• Current Assignee: Goodrich Corporation (Rtx Corporation)
• Original Assignee: Goodrich Corporation (Rtx Corporation)
• Inventors: Cotton, Christopher, Reneker, Douglas Alan, Diehl, Damon W.
• Granted Patent: US 7,751,645 B2
• Time in Patent Office: Days
• US Class Current: 348/144
• CPC Class Codes: G01C 11/02 Picture taking arrangements specially adapted for photogrammetry or photographic surveying, e.g. controlling overlapping of pictures
• CPC Class Codes: G02B 27/0068 having means for controlling the degree of correction, e.g. using phase modulators, movable elements controlling the phase of light using moving or deformable elements G02B26/06
• CPC Class Codes: G02B 27/648 for automatically maintaining a reference alignment, e.g. in self-levelling surveying instruments surveying instruments per se G01C

Abstract

A camera for aerial photography includes a reference projector that projects collimated beams of light into the optical system entrance aperture which are imaged by an image recording device. The beams produce fiducial images present in every image captured by the imaging recording device. The fiducial images can be used to characterize the performance of the optical system and derive distortion correction coefficients. The distortion correction coefficients can be applied to a portion of an image, such as a group of pixels, or to the entire image, to thereby compensate for distortions in the optical system. In some embodiments, e.g., airborne cameras, the projector is rigidly coupled to an inertial measurement unit. The ability of the airborne camera to perform object geolocation from imagery is improved. The fiducial images enable optical system performance to be characterized and distortion correction coefficients to be obtained and thereby improve the accuracy of a ray angle calculation to the object of interest. Furthermore, the ray angle can be related to an inertial measurement system coordinate system using a direction cosine matrix.

Claims

1. A camera for use in aerial photography, comprising:

an optical system directing radiation from a scene onto a focal plane,

an image recording device located at the focal plane; and

a projector projecting a set of collimated beams of light, the optical system directing the set of collimated beams onto the image recording device.

2. The camera of claim 1, further comprising an inertial measurement unit rigidly coupled to the projector.

3. The camera of claim 1, wherein the projector comprises a source of an array of individual collimated light beams, wherein the projector is designed to project the collimated light beams onto the periphery of the image recording device.

4. The camera of claim 1, wherein the projector includes a laser light source.

5. The method of claim 1, wherein the laser light source projects light at a wavelength which is selected such that it is outside of the band where useful scene information is normally imaged by the image recording device.

6. The camera of claim 1, wherein the projector projects fan-shaped sets of beams that are imaged in at least the peripheral portion of the image recording device.

7. The camera of claim 1, wherein the image recording device comprises an electronic imaging array arranged in a plurality of row and columns of pixel elements.

8. The camera of claim 2, further comprising software and hardware for performing distortion correction on at least a portion of an image of the scene captured by the image recording device based on the images from the reference projector, and

a module for performing geolocation of an object of interest;

wherein distortion corrected scene image data is supplied to said module for performing geolocation of an object of interest represented by the portion of the scene image subject to the distortion correction.

9. The camera of claim 1, wherein the projector comprises a single mode fiber optic reticle constructed and arranged to produce a Gaussian radiation pattern of collimated beams, without the use of a physical stop for controlling the diameter of the collimated beams.