Method and apparatus for storing velocity data

• US 5,130,937 A
• Filed: 03/07/1990
• Issued: 07/14/1992
• Est. Priority Date: 03/07/1990
• Status: Expired due to Fees

• Current Assignee: Sundstrand Corporation (Rtx Corporation)
• Original Assignee: Sundstrand Corporation (Rtx Corporation)
• Inventors: Kumar, Lalit, Peters, Rex B.
• Primary Examiner(s): Swann, Tod
• Application Number:
  US07/490,157
• Time in Patent Office: 860 Days
• Field of Search: 73/517 AV, 73/510, 73/DIG. 1, 73/503, 73/511, 73/862.59, 364/565, 364/566
• US Class Current: 702/141
• CPC Class Codes: G01P 15/097 by vibratory elements
• CPC Class Codes: G01P 2015/0817 for pivoting movement of the mass, e.g. in-plane pendulum

Abstract

A method and apparatus for determining a change in velocity of a body following a power disruptive event. An accelerometer (10, 50) includes quartz crystals (16 and 18, 60 and 62), which produce output signals indicative of the acceleration to which a body connected to the accelerometer is subjected. The acceleration measured is directed along the sensitive axis of the accelerometer. The quartz crystals are selected to have different scale factors, K₁ and K₂, which define the change in frequency of the quartz crystal from its no-load resonant frequency as a force is applied to it. The quartz crystals are connected between a supporting case (14) and a proof mass (12) so that a given acceleration applied to the proof mass along its sensitive axis causes one of the crystals to experience a tension force and the other to experience a compression force. A processor (86) determines the change in velocity of the body as a function of the change in phase of the signals produced by the quartz crystals at a time, t₁, and a subsequent time, t.sub. 2, and further in response to the scale factors, K₁ and K₂. Since the quartz crystals continue to oscillate during a brief interruption of their driving signal, the change in velocity of the body during a time interval from t₁ to t₂ can be determined after recovery from a brief power disruptive event that has occurred during that interval.

Claims

1. A method for recovering velocity data for a body from an attached accelerometer following a power disruptive event that interrupts electrical power supplied to the accelerometer, said accelerometer including two acceleration sensors, one of the acceleration sensors being characterized by a periodic output having a frequency that increases and the other by a periodic output having a frequency that decreases in response to an acceleration acting on the body along a sensitive axis of the accelerometer, each acceleration sensor having a scale factor associated with an output signal from it, said method comprising the steps of:

(a) providing selected different scale factors K₁ and K₂ to define output signals produced by the two acceleration sensors, said output signals varying as a function of said acceleration;

(b) determining a first phase difference, Δ

Φ

(t₁), between a component of the output signals of the two acceleration sensors that changes due to the acceleration, prior to the power disruptive event, at a first time, t₁ ;

(c) determining a second phase difference, Δ

Φ

(t₂), between said components of the output signals of the two acceleration sensors, after the power disruptive event, at a second time, t₂ ; and

(d) following the power disruptive event, determining a change in velocity of the body between times t₁ and t₂ as a function of the scale factors and the first and second phase differences of the output signals.

2. The method of claim 1, wherein the change in velocity Δ

V is defined as follows;

space="preserve" listing-type="equation">Δ

V=[Δ

Φ

(t.sub.2)-Δ

Φ

(t.sub.1)]/(K.sub.1 -K.sub.2).

3. The method of claim 1, further comprising the steps of storing the first phase difference Δ

Φ

(t₁) and the time t₁ in an electronic memory that is unaffected by the power disruptive event.

4. The method of claim 1, further comprising the step of storing successive phase differences determined at predetermined time intervals in an electronic memory that is unaffected by the power disruptive event, so that after said power disruptive event a phase difference determined prior to a power disruptive event is available for use in determining the change in velocity of the body.

5. The method of claim 4, wherein a clock that is unaffected by the power disruptive event determines the times at which each successive phase difference is determined.

6. The method of claim 1, wherein the step of providing different scale factors comprises the steps of measuring the scale factors of a plurality of acceleration sensors and selecting acceleration sensors that have scale factors K₁ and K₂ that differ by a predetermined amount, for use in the accelerometer.

7. The method of claim 1, wherein the scale factors K₁ and K₂ differ by from about 0.1 to about 0.5 percent.

8. A method for determining a change in velocity of a body using a vibrating beam accelerometer that includes opposed piezoelectric crystals arranged such that an acceleration acting on the body and directed along a sensitive axis of the accelerometer subjects one of the piezoelectric crystals to compression and the other to tension, the method comprising the steps of:

(a) biasing at least one of the piezoelectric crystals so that they have different scale factors, K₁ and K₂, where the scale factors define the relationship between the acceleration and a component of a periodic output signal produced by each piezoelectric crystal;

(b) at successive intervals of time Δ

t, determining phase differences Δ

Φ

(t_n) between said components of the periodic output signals produced by the two piezoelectric crystals, where a frequency of the component varies in response to the acceleration acting on the body; and

(c) determining the change in velocity of the body, Δ

V, as a function of the change in the phase differences determined at two different points in time, t_n-1 and t_n, and as a function of the scale factors, K₁ and K₂.

9. The method of claim 8, wherein time t_n-1 occurs before an event that interrupts processing of the output signals from the accelerometer, and time t_n occurs after the event, said step of determining the change in velocity being unaffected by the event.

10. The method of claim 9, wherein the interval Δ

t is substantially longer in duration than the event.

11. The method of claim 8, further comprising the step of storing the phase differences Δ

Φ

(t_n) in an electronic memory that is unaffected by the event, so that the phase difference at time t_n is available to determine the change in velocity, Δ

V, after the event.

12. The method of claim 8, wherein the change in velocity is determined from the relationship:

space="preserve" listing-type="equation">Δ

V=[Δ

Φ

(t.sub.n)-Δ

Φ

(t.sub.n-1)]/(K.sub.1 -K.sub.2)

where;

Δ

Φ

(t_n-1)=the phase difference at t_n-1 ; and

Δ

Φ

(t_n)=the phase difference at t_n.

13. An accelerometer capable of determining the change in velocity, Δ

V, of a body to which the accelerometer is attached, from a time t_n-1, to a time t_n, comprising;

two opposed acceleration sensitive elements, each operative to produce a periodic output signal having a component that varies in frequency as a function of an acceleration directed along a sensitive axis of the accelerometer, as described by a scale factor associated with each acceleration sensitive element, said acceleration causing one of the acceleration sensitive elements to be subjected to a force of compression and the other to be subjected to a force of tension, said acceleration sensitive elements being provided with different scale factors K₁ and K₂, so that said components of their periodic output signals have a time varying phase relationship; and

processor means for determining a difference in phase Δ

Φ

(t_n-1) between said components of output signals from the acceleration sensitive elements at the time t_n-1, and a difference in phase Δ

Φ

(t_n) of the output signals at the time t_n, and for determining the change in velocity Δ

V of the body as a function of both the differences in phase and the scale factors.

14. The accelerometer of claim 13, wherein the accelerometer is energized by a power supply subject to a brief interruption due to a power disruptive event, and wherein the processor means are operative to determine the change in velocity Δ

V of the body between times t_n-1 and t_n, where time t_n-1 occurs before the power disruptive event and time t_n occurs after the power disruptive event.

15. The accelerometer of claim 13, wherein the processor means comprise memory means that are unaffected by the power disruptive event, for storing the difference in phase Δ

Φ

(t_n-1) at time t_n-1, and clock means that are unaffected by the power disruptive event, for determining the time t_n after the power disruptive event occurs.

16. The accelerometer of claim 13, wherein the processor means determine the change in velocity of the body from the relationship:

space="preserve" listing-type="equation">Δ

V=[Δ

Φ

(t.sub.n)-Δ

Φ

(t.sub.n-1)]/(K.sub.1 -K.sub.2)

where;

Δ

Φ

(t_n-1)=the difference in phase at time t_n-1 ; and

Δ

Φ

(t_n)=the difference in phase at time t_n.

17. The accelerometer of claim 13, wherein the acceleration sensitive elements are selected to have scale factors K₁ and K₂ that differ in a desired ratio.

18. The accelerometer of claim 13, wherein the scale factors K₁ and K₂ of the acceleration sensitive elements differ by from about 0.1 to about 0.5 percent.

19. The accelerometer of claim 13, further comprising a proof mass that is connected to deflect due to the acceleration acting on the body, wherein the acceleration sensitive elements comprise quartz crystals that are each connected to the proof mass so that deflection of the proof mass applies a tension force to one quartz crystal and a compression force to the other quartz crystal.

20. The accelerometer of claim 19, wherein the proof mass comprises two pendulous weights of substantially equal mass, each connected by a flexure to a support, and wherein each of the quartz crystals is connected to one of the pendulous weights at a point substantially displaced from the flexure connecting that pendulous weight to the support.