a method of measuring low-noise acoustical impulse

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A Method of Measuring Low-Noise Acoustical Impulse Responses at High Sampling Rates 137th AES Convention October 11th, 2014 Joseph G. Tylka Rahulram Sridhar Braxton B. Boren Edgar Y. Choueiri 3D Audio and Applied Acoustics (3D3A) Laboratory Princeton University www.princeton.edu/3D3A 1

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Page 1: A Method of Measuring Low-Noise Acoustical Impulse

A Method of Measuring Low-Noise Acoustical Impulse Responses at

High Sampling Rates137th AES Convention

October 11th, 2014 !

Joseph G. Tylka Rahulram Sridhar Braxton B. Boren Edgar Y. Choueiri

!3D Audio and Applied Acoustics (3D3A) Laboratory

Princeton University www.princeton.edu/3D3A

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Page 2: A Method of Measuring Low-Noise Acoustical Impulse

Applications

2

HRTF Measurements 3D3A Lab, Princeton University

Page 3: A Method of Measuring Low-Noise Acoustical Impulse

Objectives

• Measurements at high sampling rates (>48 kHz)

• Efficient, low-noise, and artifact-free measurements

3

Page 4: A Method of Measuring Low-Noise Acoustical Impulse

ApproachInitial Measurement

Refined Measurement

4

Processing

Page 5: A Method of Measuring Low-Noise Acoustical Impulse

Outline

• Review: impulse response (IR) measurements

• Measurements at high sampling rates

• Proposed measurement procedure

• Experimental results

5

Page 6: A Method of Measuring Low-Noise Acoustical Impulse

IR Measurements

• Exponential sine sweep (ESS) [1, 2]

• Deconvolution

6

x(t) h(t)w(t)

n(t)

y(t)+

[1] A. Farina (2007) Advancements in Impulse Response Measurements by Sine Sweeps[2] S. Müller and P. Massarani (2001) Transfer-Function Measurements with Sweeps

Page 7: A Method of Measuring Low-Noise Acoustical Impulse

Exact Deconvolution

7

Frequency (Hz)

Mag

nitu

de (d

B)

Frequency (Hz)

Mag

nitu

de (d

B)

Frequency (Hz)

Mag

nitu

de (d

B)+

=

Input spectrum Exact inverse

-3 dB/oct+3 dB/oct

Signal

Noise

Signal

Noise

Page 8: A Method of Measuring Low-Noise Acoustical Impulse

8

Frequency (Hz)

Mag

nitu

de (d

B)

Frequency (Hz)

Mag

nitu

de (d

B)

Frequency (Hz)

Mag

nitu

de (d

B)

=

Input spectrum Time-reversed inverse [1]

-3 dB/oct+3 dB/oct

Signal

Noise

Signal

Noise

+Time-Reversed Deconvolution

Page 9: A Method of Measuring Low-Noise Acoustical Impulse

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NoisyPre-response (16%)

SNR = 25 dB SNR = 32 dB

Settings: 96 kHz sampling rate, 5 second sweep from 20 Hz to 24 kHz

Exact deconvolution Time-reversed deconvolution

An improvement of 7 dB due to BPF

Page 10: A Method of Measuring Low-Noise Acoustical Impulse

Why high sampling rates?

• Ultrasonic transducers

• “Time-smear” [3]

• Minimum interaural time difference ~ 10 μs [4]

• Facilitate subjective tests

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[3] P. G. Craven (2004) Antialias Filters and System Transient Response at High Sample Rates[4] A. W. Mills (1958) On the Minimum Audible Angle

Page 11: A Method of Measuring Low-Noise Acoustical Impulse

Challenges

• Signal-to-noise ratio (SNR)

• Deconvolution issues

• Transducer heating/damage

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Page 12: A Method of Measuring Low-Noise Acoustical Impulse

Measurement ProcedureInitial Measurement

Determine Pass-Band

Refined Measurement

12

Band-Pass Filter

Page 13: A Method of Measuring Low-Noise Acoustical Impulse

Defining the Pass-Band

• Improved signal-to-noise ratio

• Minimal filtering artifacts (PDA)

• User preferences

• Cost function?

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Page 14: A Method of Measuring Low-Noise Acoustical Impulse

Optimal SNR

14

Frequency (Hz)

Mag

nitu

de (d

B)Signal

Noise

Signal and Noise

Pass-Band

Page 15: A Method of Measuring Low-Noise Acoustical Impulse

Optimal SNR

14

Frequency (Hz)

Mag

nitu

de (d

B)Signal

Signal and Noise

Pass-Band

Noise + 2.1 dB

Page 16: A Method of Measuring Low-Noise Acoustical Impulse

STOP

Phase III

Phase II

no

yes

Input preference: keep/reject PDA

Is preference to reject PDA?

Input max. PDA

Determine constrained-PDA pass-band

Determine optimal-SNR pass-band and estimate

corresponding PDA

Design and execute refined ESS with fade-out

Band-pass filter mic. signal

Deconvolve mic. signal by input sweep to get IR

Design and execute phase-controlled ESS

Phase I

START

[5]

Example Implementation

15

STOP

Phase III

Phase II

no

yes

Input preference: keep/reject PDA

Is preference to reject PDA?

Input max. PDA

Determine constrained-PDA pass-band

Determine optimal-SNR pass-band and estimate

corresponding PDA

Design and execute refined ESS with fade-out

Band-pass filter mic. signal

Deconvolve mic. signal by input sweep to get IR

Design and execute phase-controlled ESS

Phase I

START

STOP

Phase III

Phase II

no

yes

Input preference: keep/reject PDA

Is preference to reject PDA?

Input max. PDA

Determine constrained-PDA pass-band

Determine optimal-SNR pass-band and estimate

corresponding PDA

Design and execute refined ESS with fade-out

Band-pass filter mic. signal

Deconvolve mic. signal by input sweep to get IR

Design and execute phase-controlled ESS

Phase I

START

[5] K. Vetter and S. di Rosario (2011) ExpoChirpToolbox: a Pure Data implementation of ESS impulse response measurement

Page 17: A Method of Measuring Low-Noise Acoustical Impulse

Optimal SNR

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Page 18: A Method of Measuring Low-Noise Acoustical Impulse

Results

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Sweep Length (s) Frequency Range Raw SNR

(dB)BPF SNR

(dB)Pre-response

Peak (%)Initial

Measurement ~1 23 Hz — 48 kHz 21 — —

Optimal SNR 5 26 Hz — 40.6 kHz 24 37 <0.2

Conventional ESS 5 20 Hz — 24 kHz 25 32 16

Note: all measurements were performed with an output level of 75 dB SPL (1 kHz, 1 m)

Exact deconv. Time-reversed deconv.

Page 19: A Method of Measuring Low-Noise Acoustical Impulse

Summary

• IR measurements at high sampling rates (>48 kHz)

• Customizable measurement procedure

• SNR improvement with minimal filtering artifacts

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Page 20: A Method of Measuring Low-Noise Acoustical Impulse

Acknowledgements

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This work was conducted under a contract from the Sony Corporation of America.

Page 22: A Method of Measuring Low-Noise Acoustical Impulse

References1. A. Farina, “Advancements in Impulse Response Measurements by

Sine Sweeps,” presented at the AES 122nd Convention, May 2007.

2. S. Müller and P. Massarani, “Transfer-Function Measurements with Sweeps,” J. Audio Eng. Soc., 49(6):443-471, 2001.

3. P. G. Craven, “Antialias Filters and System Transient Response at High Sample Rates,” J. Audio Eng. Soc., 52(3):216-242, 2004.

4. A. W. Mills, “On the Minimum Audible Angle,” J. Acoust. Soc. Am., 30(4):237-246, 1958.

5. K. Vetter and S. di Rosario, “ExpoChirpToolbox: a Pure Data implementation of ESS impulse response measurement,” presented at the 4th Pure Data Convention, 2011.

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