Light-operated accelerometer-type techniques

• US 5,159,406 A
• Filed: 09/28/1964
• Issued: 10/27/1992
• Est. Priority Date: 09/28/1964
• Status: Expired due to Term

• Current Assignee: Zenith Electronics Corporation (LG Corporation)
• Original Assignee: Zenith Electronics Corporation (LG Corporation)
• Inventors: Foster, L. Curtis, Adler, Robert
• Primary Examiner(s): Boczinski, Stephen C.
• Application Number:
  US06/399,730
• Time in Patent Office: 10,256 Days
• Field of Search: 331/94.5, 250/199, 343/117.1, 343/7.3, 343/8, 88/14 PL, 88/10, 330/4.3, 356/5, 356/28.5, 356/345, 356/349, 372/13, 372/23, 372/28, 559/285, 559/305, 73/601, 73/627
• US Class Current: 356/486
• CPC Class Codes: G01P 15/093 by photoelectric pick-up
• CPC Class Codes: G01S 17/04 Systems determining the presence of a target
• CPC Class Codes: G01S 17/50 Systems of measurement based on relative movement of target

Abstract

A laser based accelerometer system uses small motion induced shifts in frequency to measure the motion of an object without contact thereof. This technique is particularly useful for determining the vibratory and velocity characteristics of objects that are otherwise inaccessible for direct motion measurement by contact sensors.

Claims

1. Apparatus, comprising:

means for developing coherent light;

means for directing said light onto a surface of an element and effective to return a portion of said light having a parameter shifted by an amount representative of a characteristic attendant to said surface;

a pair of frequency shifting means, one of which shifts the frequency of light higher and the other of which shifts the frequency of light lower with the amounts of said two shifts being unequal, for shifting the frequency of light a predetermined amount;

means of combining light, which has been shifted in frequency by said shifting means and which also has experienced a shift in said parameter at said surface, with another quantity of light from said developing means; and

means for developing from the combination of said returned light and said other quantity a signal representative of the product of said portion and said quantity and for processing said signal to yield another signal representative of said characteristic;

in which said developing means is a laser having a resonant passband, in which said predetermined amount is of a value causing the returning light to have a frequency within said resonant passband to excite the laser into regeneration, and in which said combining means directs the returning light into said laser.

2. Apparatus, comprising:

means for developing coherent light;

means for directing said light onto a surface of an element and effective to return light having a parameter shifted by an amount representative of a characteristic attendant to said surface;

means for combining light, which has experienced a shift in said parameter at said surface, with another quantity of light from said developing means;

means disposed in the light path between said developing means and said surface and also disposed in the light path between said surface and said combining means for shifting the frequency of the light a predetermined amount during each passage of the light therethrough; and

means for deriving from the combination of said returned light and said other quantity a signal representative of the product of this portion and said quantity and for processing said signal to yield another signal representative of said characteristic.

3. In an apparatus including a laser productive of a beam of light and capable of laser action in a plurality of longitudinal modes with light developed in each mode being of a frequency differing from the frequency of the light developed in the next adjacent mode, in terms of frequency, by a predetermined amount, the improvement comprising:

means for shifting the frequency of a portion of the light in said beam by said predetermined amount and returning said frequency-shifted light into the active region of said laser.

4. Apparatus as defined in claim 3 in which said shifting means includes an element which shifts the frequency of light emerging form said laser by one-half said predetermined amount and subsequently shifts said light returning to said laser again by one-half said predetermined amount.

5. Apparatus as defined in claim 3 in which said predetermined amount equals C/2L, where C is the velocity of light and L is the resonant optical cavity length of said laser.

6. Optical heterodyning apparatus for analyzing motion of an element, comprising:

a source of coherent light;

photodetecting means;

means for directing a first portion of said coherent light onto said element, for collecting light returned from said element and for directing said returned light to said photodetecting means;

means for directing a second portion of said coherent light to said photodetecting means for combination in a condition of wavefront alignment with said returned first portion of said coherent light;

means coupled to said photodetecting means for developing a signal corresponding to the motion of said element; and

Bragg cell means located in the path of said coherent light for effecting a relative shift in frequency between said first and second portions of said coherent light

7. Optical heterodyning apparatus for analyzing motion of an element, comprising

a source of coherent light;

photodetecting means;

means for directing a first portion of said coherent light onto said element, for collecting light returned from said element and for directing said returned light to said photodetecting means;

means for directing a second portion of said coherent light to said photodetecting means for combination in a condition of wavefront alignment with said returned first portion of said coherent light;

frequency discriminating means coupled to said photodetecting means for developing a signal corresponding to the motion of said element; and

Bragg cell means located in the path of said coherent light for effecting a relative shift in frequency between said first and second portions of said coherent light, whereby the electrical output from said photodetecting means has an instantaneous frequency which equals the algebraic sum of the frequency applied to said Bragg cell means and the instantaneous velocity of the motion of said element multiplied by a constant.

8. Optical heterodyning apparatus for analyzing motion of an element, comprising:

a source of coherent light;

photodetecting means;

first means for focusing a first portion of said coherent light onto said element and for collecting light returned from said element, and second means for directing said returned light to said photodetecting means;

mirror means for directing a second portion of said coherent light to said photodetecting means for combination in a condition of wavefront alignment with said returned first portion of said coherent light;

frequency discriminating means coupled to said photodetecting means for developing a signal corresponding to the motion of said element; and

Bragg cell means located in the path of said coherent light for effecting a relative shift in frequency between said first and second portions of said coherent light, whereby the electrical output from said photodetecting means has an instantaneous frequency which equals the algebraic sum of the frequency applied to said Bragg cell means and the instantaneous velocity of the motion of said element multiplied by a constant.

9. Optical heterodyning apparatus for analyzing motion of an element, comprising:

a source of coherent light;

photodetecting means;

lens means for focusing a first portion of said coherent light onto said element and for collecting light returned from said element;

means for directing said returned light to said photodetecting means and for directing a second portion of said coherent light to said photodetecting means for combination in a condition of wavefront alignment with said returned first portion of said coherent light;

means coupled to said photodetecting means for developing a signal corresponding to the motion of said element; and

Bragg cell means in the path of said coherent light driven by a signal source and constructed and arranged to receive and act upon light arriving from opposite directions such that said signal developed by said photodetecting means has a frequency equal to twice that developed by said signal source.

10. Optical heterodyning apparatus for analyzing motion of an element, comprising:

a source of coherent light;

photodetecting means;

lens means for focusing a first portion of said coherent light onto said element and for collecting light returned from said element;

means for directing said returned light to said photodetecting means and for directing a second portion of said coherent light to said photodetecting means for combination in a condition of wavefront alignment with said returned first portion of said coherent light;

means coupled to said photodetecting means for developing a signal corresponding to the motion of said element; and

Bragg cell means driven by a signal source and constructed and arranged to receive and act upon light arriving from opposite directions such that said signal developed by said photodetecting means has a frequency equal to twice that developed by said signal source, said Bragg cell being located in said first light portion.

11. A method of analyzing motion of an element, comprising:

generating a beam of coherent light;

directing a first portion of said coherent light beam onto said element, collecting light returned from said element and directing said returned light to a detecting location;

directing a second portion of said light beam to said detecting location for combination in a condition of wavefront alignment with said returned first portion of said light beam;

acousto-optically effecting a relative shift in frequency between said first and second portions of said coherent light; and

at said detecting location, photodetecting said combined first and second portions of said light beam.

12. A method of analyzing motion of an element, comprising:

generating a beam of coherent light;

directing a first portion of said light beam onto said element, collecting light returned from said element and directing said returned light to a detecting location;

directing a second portion of said light beam to said detecting location for combination in a condition of wavefront alignment with said returned first portion of said light beam;

with a Bragg cell located in the path of said light beam, effecting a relative shift in frequency between said first and second portions of said light beam; and

at said detecting location, photodetecting said combined first and second portions of said light beam and developing a signal whose instantaneous frequency corresponds to the motion of said element, said instantaneous frequency being equal to the algebraic sum of the frequency applied to the Bragg cell and the instantaneous velocity of the motion of the element multiplied by a constant.

13. A method of analyzing motion of an element, comprising:

generating a beam of coherent light;

focusing a first portion of said light beam onto said element and collecting light returned from said element;

directing said returned first portion light and a second portion of said light beam to said detecting location for combination in a condition of wavefront alignment;

with a Bragg cell driven by a signal source and arranged in the path of said light beam to receive and act upon light arriving from opposite directions, effecting a relative shift in frequency between said first and second portions of said light beam which equals twice the frequency developed by the signal source; and

at said detecting location, photodetecting said combined first and second portions of said coherent light beam and developing a signal corresponding to the motion of said element.

14. A method of analyzing motion of an element, comprising:

generating a beam of coherent light;

focusing a first portion of said light beam onto said element and collecting light returned from said element;

directing said returned first portion light and a second portion of said light beam to said detecting location for combination in a condition of wavefront alignment;

with a Bragg cell driven by a signal source and located in the path of said first portion of said light beam to receive and act upon light arriving from opposite directions, effecting a relative shift in frequency between said first and second portions of said light beam which is twice the frequency developed by the signal source; and

at said detecting location, photodetecting said combined first and second portions of said light beam and developing a signal corresponding to the motion of said element.