METHOD FOR RECORDING AND REPRODUCING PRESSURE WAVES COMPRISING DIRECT QUANTIFICATION

• US 20120167691A1
• Filed: 05/11/2010
• Published: 07/05/2012
• Est. Priority Date: 07/07/2009
• Status: Abandoned Application

• Current Assignee: Siemens AG
• Original Assignee: Siemens AG
• Inventors: Gilg, Albert, Wever, Utz
• Application Number:
  US13/383,162
• Publication Number:
  US 20120167691A1
• Time in Patent Office: Days
• US Class Current: 73/645
• CPC Class Codes: H04R 1/005 using digitally weighted transducing elements
• CPC Class Codes: H04R 1/38 in which sound waves act upon both sides of a diaphragm and incorporating acoustic phase-shifting means, e.g. pressure-gradient microphone
• CPC Class Codes: H04R 1/406 microphones

Abstract

In a method for recording and reproducing pressure wave signals, a wave pressure recording and an analog digital converter are to be linked. Higher dynamics are to be effected at identical bit depths and lower bit depths are to be required for identical dynamics. All information provided by the pressure wave signal is calculated and stored on the basis of detected and directly quantified wave pressure differences of the pressure wave signal. In addition, coefficients can be stored and, if necessary, retransformed into absolute wave pressures. In this way, the pressure wave signal can be reproduced.

Claims

1. A method for recording a pressure wave signal, comprising detecting and storing directly quantified wave pressure differences of the pressure wave signal.

2. The method according to claim 1, wherein coefficients of a basis function containing information of the pressure wave signal are calculated on the basis of the detected and directly quantified wave pressure differences of the pressure wave signal and stored.

3. The method according to claim 2, wherein the basis function is a wavelet basis function.

4. The method according to claim 1, wherein respective different wave pressure differences from different measurement time intervals are detected in repeating overall time intervals by a variety of pressure-gradient microphones.

5. The method according to claim 4, wherein an overall interval is equally subdivided into a number of equal-length basic time intervals and the length of a basic time interval is determined by means of a highest and a lowest frequency to be resolved.

6. The method according to claim 5, wherein the highest frequency to be resolved is divided by the lowest frequency to be resolved and the quotient determines the number and length of the basic time intervals in an overall time interval.

7. The method according to claim 6, wherein the number of basic time intervals is expressed as a power of 2, that is 2^m, with the exponent m, which determines the number of pressure-gradient microphones used.

8. The method according to claim 4, wherein by means of a sound pressure microphone, absolute wave levels at all measurement time points of an overall time interval are added to form a sum S.

9. The method according to claim 8, wherein all the coefficients are calculated by means of the wave pressure differences detected and the sum S per overall time interval is calculated.

10. The method according to claim 3, wherein the wavelet basis function is

a Haar wavelet function,

a Coiflet wavelet function,

a Gabor wavelet function,

a Daubechies wavelet function,

a Johnston-Barnard wavelet function or

a bioorthogonal spline wavelet function.

11. The method according to claim 7, wherein the wavelet basis function is selected from the group consisting of a Haar wavelet function, a Coiflet wavelet function, a Gabor wavelet function, a Daubechies wavelet function, a Johnston-Barnard wavelet function and a bioorthogonal spline wavelet function, and

the wavelet basis function being a Haar wavelet basis function, characterized in that in each instance, one of m pressure-gradient microphones detects pressure differences from 2ⁿ basic time intervals as the measurement time interval, the measurement time intervals each being separated from one another by 2ⁿ basic time intervals, wherein n is the element N₀ and n≦

m−

1.

12. The method according to claim 2, wherein compression is carried out in that coefficients below a threshold value are ignored.

13. The method according to claim 4, wherein a plurality of different pressure-gradient microphones is used for different frequency ranges.

14. The method according to claim 13, wherein the areas of detection diaphragms of the pressure-gradient microphones are tuned to the respective frequency range.

15. The method according to claim 13, wherein the detection diaphragms of the pressure-gradient microphones are arranged adjacent to one another in one housing.

16. The method according to claim 15, wherein the detection diaphragms are arranged concentrically with one another.

17. The method according to claim 16, wherein detection diaphragms for higher frequency wave pressure differences are arranged inwardly and detection diaphragms for lower frequency wave pressure differences are arranged outwardly.

18. A method for reproducing a pressure wave signal recorded with a method according to claim 1, wherein, by means of an upper Hessenberg matrix, the absolute wave pressures are calculated back from the stored pressure differences at all the measurement time points per overall time interval, and are output.

19. The method for reproducing a pressure wave signal recorded with a method according to claim 2, wherein, by means of an inverse transformation from the coefficients, optionally together with the sum S, the absolute wave pressures are calculated in reverse and reproduced for all the measurement time points per overall time interval.

20. Pressure-gradient microphones for recording a pressure wave signal with detecting and storing directly quantified wave pressure differences of the pressure wave signal, wherein areas of detection diaphragms of the pressure-gradient microphones are tuned to the respective frequency range.

21. The pressure-gradient microphones according to claim 20, wherein the detection diaphragms of the pressure-gradient microphones are arranged adjacent to one another in one housing.

22. The pressure-gradient microphones according to claim 21, wherein the detection diaphragms are arranged concentrically with one another.

23. The pressure-gradient microphones according to claim 22, wherein detection diaphragms for higher frequency wave pressure differences are arranged inwardly and detection diaphragms for lower frequency wave pressure differences are arranged outwardly.

24. A method comprising using of a microphone according to claim 20 for sound pressure waves in the audio range or the ultrasonic range in medicine or materials science or for seismic waves in geophysics or materials science.