Method for determining and reproducing noise inducing vibrations in a multi-component assembly

• US 6,101,882 A
• Filed: 07/08/1998
• Issued: 08/15/2000
• Est. Priority Date: 07/08/1998
• Status: Expired due to Term

• Current Assignee: Ford Global Technologies, LLC (Ford Motor Company)
• Original Assignee: Ford Global Technologies, LLC (Ford Motor Company)
• Inventors: Charette, Francois, Phillips, Andrew, Boes, Gary, Covitz, Bill, Hsueh, Keng D., Tran, Vy, Fuller, Christopher Robert
• Primary Examiner(s): MOLLER, RICHARD ALAN
• Application Number:
  US09/111,944
• Time in Patent Office: 769 Days
• Field of Search: 73/570, 73/662, 73/669
• US Class Current: 73/662
• CPC Class Codes: F16F 15/02 Suppression of vibrations of non-rotating, e.g. reciprocating systems; Suppression of vibrations of rotating systems by use of members not moving with the rotating systems F16F15/005 takes precedence ; layered products B32B; suppression of vibration in ships B63; relieving load on bearings, using magnetic means F16C39/06
• CPC Class Codes: G01M 7/00 Vibration-testing of structures; Shock-testing of structures G01M9/00 takes precedence

Abstract

The recreation of vibration levels at certain points in a stationary vehicle interior that are representative of realistic road conditions are achieved using road measurements in conjunction with a technique known as "reciprocal filtering." The reciprocal filtering technique consists of using an inverse transfer function, or impulse response in the time domain, between an excitation transducer and an accelerometer to calculate the excitation signal needed to recreate the vibrations measured on the road when squeak and rattle are present in a component of the vehicle. A set of excitation signals may be recorded for each component in the vehicle which is suspected of producing squeak and rattle noise. When a complaint is made that a vehicle is producing squeak and rattle, a service technician may reproduce noise by inducing vibrations through a kit having a CD player, an amplifier, a bass shaker and a CD with the set of excitation signals stored on separate tracks thereof. The bass shaker is attached, for example with two side tape, to the component suspected of producing noise, and noise inducing vibrations are played from the CD, through the CD player and amplifier, to the bass shaker. In this way, squeak and rattle may be quickly identified and repaired.

Claims

1. A method for reproducing noise inducing vibrations in a target component of a multi-component assembly, the method comprising the steps of:

collecting a set of vibration data at a predetermined vibration measurement location of the target component when the multi-component assembly is vibrated;

determining a reciprocal filter expression representing a transformation of an input signal to an output response in the target component;

calculating a set of calibration signals using the reciprocal filter expression and the set of vibration data; and

exciting the target component by inputting the calibration signals to a vibration generating system attached thereto at the vibration measurement location so as to reproduce noise therefrom.

2. The method according to claim 1 wherein the step of determining a reciprocal filter expression is accomplished by:

providing an input signal, x(t), to the vibration generating system attached at the predetermined measurement location;

measuring a vibration response, y(t), of the target component;

determining a transfer function, H(ƒ

), for the target component; and

using the transfer function to realize a reciprocal filter.

3. The method according to claim 2 wherein the transfer function is determined as ##EQU2## where, Pxy(ƒ

) and Pxx(ƒ

) respectively represent the cross-power spectrum of x(t) and y(t) and auto-power spectrum of x(t) at frequency,ƒ

.

4. The method according to claim 3 wherein the transfer function is used to realize a reciprocal filter as

5. The method according to claim 4 wherein a polynomial form of the reciprocal filter is realized using an Inverse Fourier Transform in the form of

6. The method according to claim 5 wherein the set of calibration signals is calculated by the time-domain difference equation:

space="preserve" listing-type="equation">x.sub.c (k)=b(1)*y.sub.d (k)+b(2)*y.sub.d (k-1)+. . . +b(n +1)*y.sub.d (k-n)

where x_c (t) is the s et of calibration signals, b(n) are the filter coefficients, y_d (t) are the desired response signals, such as the vibrations measured on road, and k is the sample operation.

7. The method according to claim 6 wherein the digital calibration signal, x_c (k), is converted into an analog signal, x_c (t), using a digital-to-analog converter to drive the vibration generation system.

8. A method for locally reproducing noise inducing vibrations in a multi-component assembly for diagnosing un expected noise therein, the method comprising the steps of:

identifying a vibration measurement location for a target component in the assembly;

collecting a set of vibration data at the vibration measurement location when the multi-component assembly is vibrated;

determining a reciprocal filter expression representing a transformation of an input signal to an output response in the target component;

calculating a set of calibration signals using the reciprocal filter expression and the set of vibration data; and

exciting the target component by inputting the calibration signals to a vibration generating system attached thereto at the vibration measurement location so to reproduce noise there at.

9. The method according to claim 8 wherein the step of identifying the vibration measurement location comprises conducting a modal analysis of the target component at a plurality of test measurement locations to determine vibration characteristics thereof.

10. The method according to claim 9 wherein the modal analysis is used to identify at least one active point on the target component characterized by a high vibration magnitude on a modal vibration graph.

11. The method according to claim 9 wherein the modal analysis is used to identify at least one nodal point on the target component characterized by a low vibration magnitude on a modal vibration graph.

12. The method according to claim 8 including the step of determining a target component transfer function, H(ƒ

), for the target component and using the transfer function to realize the reciprocal filter expression.

13. The method according to claim 12 wherein the target component transfer function is determined in the time domain by using an adaptive filter to calculate a set of coefficients for a FIR filter.

14. The method according to claim 12 wherein the target component transfer function is determined in the frequency domain as the ratio between a Fourier transform of a test excitation signal input to the target component and a measured response on the target component.

15. A method for calibrating a vibration generating system for reproducing noise inducing vibrations in a target component of a multi-component assembly, the method comprising the steps of:

(a) identifying a vibration measurement location for a target component in the assembly;

(b) collecting a set of vibration data at the vibration measurement location when the multi-component assembly is vibrated;

(c) determining a reciprocal filter expression by;

providing an input signal, x(t), to the vibration generating system attached at the predetermined measurement location;

measuring a vibration response, y(t),of the target component;

determining a transfer function, H(ƒ

),for the target component; and

using the transfer function to realize a reciprocal filter; and

(d) calculating a set of calibration signals using the reciprocal filter and the set of vibration data which when input to a vibration generating system attached to the target component at the vibration measurement location reproduces noise therefrom.

16. The method according to claim 15 wherein the transfer function is determined as ##EQU3## where, Pxy(ƒ

) and Pxx(ƒ

) respectively represent the cross-power spectrum of x(t) and y(t) and auto-power spectrum of x(t) at frequency,ƒ

.

17. The method according to claim 16 wherein the transfer function is used to realize a reciprocal filter as

18. The method according to claim 17 wherein a polynomial form of the reciprocal filter is realized using an Inverse Fourier Transform in the form of:

space="preserve" listing-type="equation">b(z)=b(1)+b(2)z.sup.-1 +. . . +b(n+1)z.sup.-n

where z is the z-transform, n-1 is the filter order, and b(z) are the filter coefficients.

19. The method according to claim 18 wherein the set of calibration signals is calculated by the time-domain difference equation:

space="preserve" listing-type="equation">x.sub.c (k)=b(1)* y.sub.d (k)+b(2)*y.sub.d (k-1)+. . . +b(n+1)*y.sub.d (k-n)

where x_c (t), is the set of calibration signals , b(n) are the filter coefficients, y_d (t) are the desired response signals, such as the vibrations measured on road, and k is the sample operation.