Doppler rotational velocity sensor

• US 20020075475A1
• Filed: 09/20/2001
• Published: 06/20/2002
• Est. Priority Date: 09/22/2000
• Status: Active Grant

• Current Assignee: Virginia Tech Intellectual Properties, Inc.
• Original Assignee: Virginia Tech Intellectual Properties, Inc.
• Inventors: Holton, Carvel E.
• Granted Patent: US 6,621,561 B2
• Time in Patent Office: Days
• US Class Current: 356/28.5
• CPC Class Codes: G01P 3/366 by using diffraction of light for measuring speed of fluids G01P5/26
• CPC Class Codes: G01P 3/44 for measuring angular speed G01P3/56 takes precedence
• CPC Class Codes: G01S 17/58 Velocity or trajectory determination systems; Sense-of-movement determination systems
• CPC Class Codes: G01S 17/88 Lidar systems specially adapted for specific applications
• CPC Class Codes: G01S 7/4818 using optical fibres

Abstract

The disclosed invention concept utilizes a homodyne/heterodyne interferometer technique in a modified lidar in such a manner as to sense the rotational velocity magnitude and sense of a rotating (or “spinning”) object. Sensing is accomplished in assessing either the Doppler bandwidth of a single axis system or in sensing the frequency separation of Doppler spectrums in a “two” axis system. The technique is unique in that the Doppler bandwidth is linearly proportional to rotational velocity and independent of intercept position in the rotation plane. The technique as disclosed is based on optical fiber lidar techniques, but can be implemented in free-space optics as well. The disclosed invention therefore comprises both a technique for utilization of an optical fiber lidar and a new arrangement of lidar elements. Compact and cost effective, standoff rotation velocity sensors and systems can be fabricated with this technique.

Claims

1. A method of determining the rotational velocity of an object, the method comprising:

directing at least one beam of light at the object;

sensing at least one beam of light reflected or backscattered from the object;

determining the Doppler spectral bandwidth of the sensed beam of light reflected or backscattered from the object;

determining the width of the area subtended by the intersection of the at least one beam of light and the surface of the rotating object; and

determining the angle at which the at least one beam of light intercepts the rotating object.

2. The method as set forth in claim 1 further comprising calculating the rotational velocity of the object based upon the equation:

δ

f=−

2ω

δ

X cos (α

)

where δ

f is the Doppler spectral bandwidth contribution due to the rotational velocity, ω

is the rotational rate in radians per second, α

is the beam intercept angle and δ

X is the width of the beam and the major axis of the illumination ellipse.

3. The method as set forth in claim 1 wherein the Doppler bandwidth or separation frequencies are rotationally and positionally invariant after the angle of intercept to the rotating surface is fixed.