Photoelastic measuring transducer and accelerometer based thereon

• US 4,648,274 A
• Filed: 08/07/1985
• Issued: 03/10/1987
• Est. Priority Date: 08/07/1985
• Status: Expired due to Term

• Current Assignee: General Signal Corporation (SPX Corporation)
• Original Assignee: General Signal Corporation (SPX Corporation)
• Inventors: Trainer, Michael N.
• Primary Examiner(s): Levy, Stewart J.
• Assistant Examiner(s): Oldham, Scott M.
• Application Number:
  US06/763,152
• Time in Patent Office: 580 Days
• Field of Search: 73/517 R, 73/800, 73/862.38, 73/862.64, 73/653, 350/371, 350/372, 350/373, 350/400, 350/401, 350/403, 350/404, 356/33, 356/34, 356/365
• US Class Current: 73/514.26
• CPC Class Codes: G01H 9/00 Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves by using radiation-sensitive means, e.g. optical means
• CPC Class Codes: G02F 1/0131 based on photo-elastic effects, e.g. mechanically induced birefringence

Abstract

A photoelastic transducer is constructed with a photoelastic element receiving a 45° polarized light beam with a wave plate providing a 90° phase displacement in its orthogonal components. The element has reflective surface coatings to produce multiple internal reflections so as to lengthen the optical path, and increase the sensitivity of the unit. Analysis of the orthogonal outputs can be according to the difference divided by the sum with one of the outputs being multiplied by the ratio of the D.C. component of the other output to its D.C. component, for the purpose of compensating for changes in tramsmission of the two signals. Alternatively, the signal analysis can be in accordance with the difference between the rates of change of the two signals with each rate of change being multiplied by a factor which is proportional to the square root of the ratio of the other signal to the present signal, for the purpose of compensating for changes in the wave plate dimensions due to factors such as temperature change.

Claims

1. A photoelastic measuring transducer, comprising:

a photoelastic element which exhibits a degree of birefringence which varies in proportion to variations in the amount of stress applied along an axis of the element, said stress being proportional to the variable to be measured, said photoelastic element being constructed to provide multiple internal reflections of light beams solely in a plane of internal reflection substantially normal to the stress axis so as to lengthen the optical path in said element;

means for providing a single beam only of plane polarized light directed at said element at an angle for propagation through said element in said plane of internal reflection with its plane of polarization at an angle with the axis of said stress;

means for producing a phase difference between two perpendicular components of the polarized light beam one of which is along the stress axis;

polarizing analyzer means for passing a first quantity of luminous flux of the beam transmitted by said element and polarized in a plane perpendicular to the plane of polarization of said incident beam and a second quantity of luminous flux polarized in a plane parallel to the plane of polarization of said incident beam;

first and second photocells for converting said first and second quantities of luminous flux into corresponding first and second electrical signals proportional to said quantities; and

means for combining functions of said first and second electrical signals as required to calculate the magnitude of the variable to be measured.

2. A photoelastic measuring transducer, as set forth in claim 1, in which:

said means for providing a single beam only of plane polarized light and said polarizing analyzer means are both provided by a single polarizing beam splitter cube.

3. A photoelastic measuring transducer, as set forth in claim 1, in which:

said element is a rectangular parallelapiped constructed to provide multiple internal reflections by having its planar surfaces parallel to the stress axis provided with a reflective coating.

4. A photoelastic measuring transducer, as set forth in claim 1, in which:

said element has one reflective face at an angle other than 90°

to the other reflective faces to provide a reflection of the beam which causes the beam to propagate back on along its original path.

5. A photoelastic measuring transducer, as set forth in claim 1, in which:

at least one of the reflective faces of said element is curved in shape.

6. A photoelastic measuring transducer, as set forth in claim 1, in which:

all of the reflective faces of said element are curved in shape.

7. A photoelastic measuring transducer, as set forth in claim 1, in which

the first and second signals are combined by dividing the difference between them by their sum where one of the signal values in the numerator and the denominator are multiplied by the ratio of the D.C. component of the other signal to that of the present signal.

8. A photoelastic measuring transducer, as set forth in claim 1, in which

fiber optics means are provided to transmit said first and second quantities of luminous flux to said first and second photocells where said first and second electrical signals, S₁ and S₂, are generated;

and

said means for combining the first and second electrical signals to calculate the magnitude of the variable to be measured (R) combines those signals as a function of a quantity equal to the difference between the first and second electrical signals all divided by the sum of those signals, as follows;

space="preserve" listing-type="equation">R=(S.sub.1 -rS.sub.2)/(S.sub.1 +rS.sub.2)

where r is the ratio of the D.C. components of the signals S₁ and S₂.

9. A photoelastic measuring transducer as set forth in claim 1, in which

said means for combining said first and second electrical signals determines the difference between the rates of change of the two signals with those rates of change each being modified by a factor equal to one half of the square root of the ratio of the other signal to the present signal.

10. A photoelastic measuring transducer, as set forth in claim 1, in which:

fiber optics means are provided to transmit said first and second quantities of luminous flux to said first and second photocells where said first and second electrical signals are generated; and

said means for combining the first and second electrical signals (S₁ and S₂) to calculate the magnitude of the variable to be measured (R) combines those signals in accordance with the following equation;

space="preserve" listing-type="equation">R=[(S.sub.2 /S.sub.1).sup.1/2 dS.sub.1 /dt-(S.sub.1 /S.sub.2).sup.1/2 dS.sub.2 /dt]=2dS/dt.

11. An improved photoelastic measuring transducer, comprising:

a photoelastic element;

means for inducing stress into said element along an axis of the element so that the magnitude of the stress is a known function of a variable to be measured;

means for providing a single beam only of plane polarized light incident on said element and directed for propagation through said element in a plane substantially normal to said stress axis and with the plane of polarization at an angle of 45°

with the axis of said induced stress;

a coating on said element for providing multiple internal reflections of said beam solely in said plane before said beam exits from said element;

a wave plate inserted in said beam with its orthogonal components at 45°

to said plane of polarization;

polarizing analyzer means for passing a first quantity of luminous flux of the beam exiting from said element and polarized in a plane perpendicular to the plane of polarization of said incident beam and a second quantity of luminous flux polarized in a plane parallel to the plane of polarization of said incident beam;

fiber optic means for transmitting said first and second quantities of luminous flux to a location where indication of the magnitude of the quantity being measured is desired;

first and second photocells at said location for converting said first and second quantities of luminous flux transmitted by said fiber optic means into corresponding first and second electrical signals proportional to said quantities; and

means for calculating the magnitude of said variable to be measured as a function of the difference between the first and second electrical signals all divided by the sum of those signals, whereby the resulting measurement is free of the effects of vibration induced microbending noise in the fiber optics and amplitude noise in the incident light beam.

12. An accelerometer for vibration monitoring comprising:

a base for attachment to a unit whose vibration is to be monitored;

a photoelastic element attached to said base, said element having a reflective coating to produce multiple internal reflections of light beams incident on said element;

an inertial mass attached to said photoelastic element to produce stress along an axis of said element of magnitude related to the acceleration of said mass when vibration of said base occurs;

means for providing a single beam only of plane polarized light incident on said element in a direction to produce said multiple internal reflections solely in a plane of internal reflection substantially perpendicular to said stress axis, said beam being plane polarized at an angle of 45°

with said stress axis;

wave plate means for producing a phase shift of 90°

between two perpendicular components of said polarized light beam, one of which is along the stress axis;

polarizing analyzer means for passing both a first quantity of luminous flux of the beam exiting said element with a polarization angle perpendicular to the plane of polarization of said incident beam and a second quantity of luminous flux exiting said element with a polarization angle parallel to the plane of polarization of said incident beam;

fiber optic means for transmitting said first and second quantities of luminous flux to a location where indication of the magnitude of the acceleration being measured is desired;

first and second photocells at said location for converting said first and second quantities of luminous flux transmitted by said fiber optic means into corresponding first and second electrical signals proportional to said quantities; and

means for calculating the magnitude of said acceleration as a function of a quantity equal to the difference between the first and second electrical signals all divided by the sum of those signals, whereby the resulting measurement is free of the effects of vibration induced microbending noise in the fiber optics and amplitude noise in the incident light beam.

13. An improved photoelastic measuring transducer comprising:

a photoelastic element having a reflective coating to produce multiple internal reflections of light beams incident on said element for propagation through said element along a plane of internal reflection;

means for inducing stress into said element along an axis of the element substantially normal to said plane of internal relection so that the magnitude of the stress is a known function of a variable to be measured;

means for providing a single beam only of plane polarized light incident on said element in a direction to produce said multiple internal reflections solely in said plane of internal reflection, said beam being plane polarized at an angle of 45°

with said stress axis;

wave plate means for producing a phase shift of 90°

between two perpendicular components of said polarized light beam, one of which is along the stress axis;

polarizing analyzer means for passing the luminous flux of the beam exiting said element with a polarization angle either perpendicular or parallel to the plane of polarization of said incident beam; and

a photocell for converting said luminous flux into a corresponding electrical signal of magnitude related to said variable to be measured.

14. An improved photoelastic measuring transducer comprising:

a photoelastic element having a reflective coating to produce multiple internal reflections of light beams incident on said element for propagation along a plane in said element;

means for inducing stress into said element along an axis of the element normal to said plane so that the magnitude of the stress is a known function of a variable to be measured;

means for providing a single beam only of plane polarized light incident on said element in a direction to produce said multiple internal reflections solely in said plane, said beam being plane polarized at an angle of 45°

with said stress axis;

wave plate means for producing a phase shift of 90°

between two perpendicular components of said polarized light beam, one of which is along the stress axis;

polarizing analyzer means for passing both a first quantity of luminous flux of the beam exiting said element with a polarization angle perpendicular to the plane of polarization of said incident beam and a second quantity of luminous flux exiting said element with a polarization angle parallel to the plane of polarization of said incident beam;

first and second photocells for converting said first and second quantities of luminous flux into corresponding first and second electrical signals proportional to said quantities; and

means for calculating the magnitude of said measured quantity as a function of the first and second electrical signals.