CN105973459A - Estimation method for theoretical sound pressure level of free sound field in anechoic chamber calibration - Google Patents

Estimation method for theoretical sound pressure level of free sound field in anechoic chamber calibration Download PDF

Info

Publication number
CN105973459A
CN105973459A CN201610352880.8A CN201610352880A CN105973459A CN 105973459 A CN105973459 A CN 105973459A CN 201610352880 A CN201610352880 A CN 201610352880A CN 105973459 A CN105973459 A CN 105973459A
Authority
CN
China
Prior art keywords
pressure level
sound pressure
unit
dead room
theoretical
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN201610352880.8A
Other languages
Chinese (zh)
Other versions
CN105973459B (en
Inventor
颜伟
王钦
王恩荣
李林
吴云
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nanjing Normal University
Original Assignee
Nanjing Normal University
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Nanjing Normal University filed Critical Nanjing Normal University
Priority to CN201610352880.8A priority Critical patent/CN105973459B/en
Publication of CN105973459A publication Critical patent/CN105973459A/en
Application granted granted Critical
Publication of CN105973459B publication Critical patent/CN105973459B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01HMEASUREMENT OF MECHANICAL VIBRATIONS OR ULTRASONIC, SONIC OR INFRASONIC WAVES
    • G01H17/00Measuring mechanical vibrations or ultrasonic, sonic or infrasonic waves, not provided for in the preceding groups

Abstract

The invention discloses an estimation method for a theoretical sound pressure level of a free sound field in anechoic chamber calibration, wherein the method is used for calculating theoretical sound pressure level data in anechoic chamber calibration. A multi-channel acoustic analyzer is used for measuring testing sound pressure level data, generated by a testing sound source at a path under a frequency, of a measured anechoic chamber; according to a practical testing environment of the measured anechoic chamber, a sound pressure level attenuation coefficient alpha is calculated; two unknown parameters A and r0 in a new theoretical sound pressure level calculation model are calculated by using a non-linear curve fitting method; an air absorption attenuation part is added into the calculation model; and a theoretical sound pressure level is estimated by using a non-linear least square method fitting way. Therefore, precise estimation of the theoretical sound pressure level of the measured anechoic chamber can be realized; the deviation distribution becomes reasonable; and the calibration precision is improved effectively.

Description

The evaluation method of free found field theory sound pressure level in the calibration of a kind of dead room
Technical field
The present invention relates to the evaluation method of free found field theory sound pressure level in the calibration of a kind of dead room, be used for calculating dead room Theoretical sound pressure level data in calibration.Belong to field of acoustics.
Background technology
Along with the development of acoustic-electric technology, the dead room application in the field of manufacture is increasingly wider, real as a kind of acoustics Testing room, its Main Function is to provide the low noise test environment in a free found field space.Good dead room calibration system can Effectively to evaluate the performance indications of dead room, promote the innovation of dead room, improve the quality of dead room.In order to judge dead room Acoustical behavior, need dead room is carried out place calibration, the development to dead room has indispensable meaning.
At present, the domestic calibration operation Main Basis for dead room and semianechoic room GB 6882, ISO 3745 annex The calibration procedure of regulation in A and JJF 1147 dead room calibrating standard, the main collimation technique index of dead room has two, bag The qualification of the frequency range of free found field and spatial dimension and background noise, wherein, the maximum free sound of tested dead room are included Field radius need to meet measurement sound pressure level and inverse square rate sound pressure level maximum allowable offset scope.At free found field frequency and space model In the qualification enclosed, the free found field theory sound pressure level model of above-mentioned national regulations disclosure satisfy that acoustic pressure is put down with the anti-of range attenuation Square gauge is restrained, but the measured value obtained by GB theory sound pressure level computational methods and theoretical value aberration curve exist near-end deviation The un-reasonable phenomenon relatively big, far-end deviation is less, i.e. free found field deviation " near big and far smaller " problem, the most existing theoretical sound pressure level Computation model in not yet consider air attenuation by absorption amount, have impact on precision and the accuracy of calibration result.
For the problems referred to above, the present invention is after the problem that analytic set code computational methods exist, it is proposed that Yi Zhonggai The dead room theory sound pressure level computational methods entered.Air attenuation by absorption part is added computation model by new method, uses non-linear Theoretical sound pressure level is estimated by the mode of least square fitting, makes deviation profile tend to reasonable, is effectively improved calibration accuracy.
The present invention can be applied to the calibration of dead room and the qualification of free found field, it is possible to effectively estimates that tested dead room is certainly By the theoretical sound pressure level of sound field, the optimization for dead room calibration steps provides theoretical foundation and Engineering Guidance with improving.
Summary of the invention
The present invention is directed to free found field deviation " near big and far smaller " that existing GB theory sound pressure level computational methods cause and not The problem considering air attenuation by absorption factor, it is proposed that a kind of for estimating free found field theory sound pressure level in dead room calibration Method, the final theoretical sound pressure level obtaining dead room free found field.
The inventive method, it specifically comprises the following steps that
The first step: utilize microphone, multiple channel acousto analyser, PULSE test n point of systematic survey tested dead room (n >= 10) sound pressure level, measurement result is designated as LPi, unit be dB, i be 1 to n, i-th is designated as r with the distance at measuring sound source centeri
Second step: allow dead room be in standard atmosphere pressure, measure the Celsius temperature T of dead room, relative humidity hr, sound source Frequency f, calculates sound pressure level attenuation quotient α according to following formula.
α = 8.686 f 2 [ 1.84 × 10 - 11 ( T K T 0 ) - 1 2 + ( T K T 0 ) - 5 2 × ( 0.01275 f r O f r O 2 + f 2 e - 2239.1 T K + 0.1068 f r N f r N 2 + f 2 e - 3352.0 T K ) ] - - - ( 4 )
In formula, TkFor the absolute temperature of dead room, unit is K, Tk=T+273.15;T0For reference temperature, size is 293.15K;F is the frequency of sound source, and unit is Hz;frOFor oxygen relaxation frequency, unit is Hz;frNFor nitrogen relaxation frequency, unit is Hz, wherein
f r O = 24 + 4.04 × 10 4 h 0.02 + h 0.319 + h - - - ( 5 )
f r N = 9 T 0 T K + 280 e - 4.170 ( T 0 T K 3 - 1 ) · T 0 T K h - - - ( 6 )
In formula, h and TkFor,
h = h r 10 - 6.8346 ( T 01 T K ) 1.261 + 4.6151 - - - ( 7 )
TK=T+273.15 (8)
In formula, h is the molar concentration of water vapour, and unit is %;T is the Celsius temperature of dead room, and unit is DEG C;hrFor phase To humidity, unit is %;T01For triple point, size is-273.16K.
3rd step: 1. by A and r0Initial value be respectively set to 0 and-0.5;
2. by LPi, ri, A brings following formula into
Q = Σ i = 1 n [ L P i - 20 lg A ( r i - r 0 ) - α ( r 0 - r i ) ] 2 - - - ( 3 )
If 3. Q > 0.5 and r0≤ 0.5, then r0=r0+ 0.0001, return 2.;
If 4. Q > 0.5 and r0> 0.5, then A=A+1, r02.=-0.5, return;
If 5. Q≤0.5, then record A and r now0, terminate Q and calculate.
4th step: according to following formula and ri, α, A and r0Determine free found field theory sound pressure level curve.
L P T i = 20 lg A ( r i - r 0 ) + α ( r 0 - r i ) - - - ( 1 )
In formula, LPTiFor distance Sound Source Center riThe theoretical sound pressure level at place, unit is dB.
The inventive method, utilizes multiple channel acousto analyser to measure tested dead room and is produced by measuring sound source under path and frequency Raw test sound pressure level data, the actual test environment further according to tested dead room calculates sound pressure level attenuation quotient α, then utilizes Linear curve fitting method determines two unknown parameter A and r in theoretical sound pressure level novel model of calculating0, air is absorbed and declines Subtract part and add computation model, use the mode of Non-linear least-square curve fitting that theoretical sound pressure level is estimated, thus real The accurate estimation of existing tested dead room theory sound pressure level, makes deviation profile tend to reasonable, is effectively improved calibration accuracy.
Accompanying drawing explanation
Fig. 1 be frequency of source be 10kHz, temperature be 20 DEG C, relative humidity is when being 50%, calculated sound pressure level decays Curve.
Detailed description of the invention
Below in conjunction with the accompanying drawings and specific embodiment, the present invention is described in further details.
The first step: utilize microphone, multiple channel acousto analyser, PULSE to test systematic survey dead room n point (n= 16) sound pressure level, measurement result is designated as LPi, unit be dB, i be 1 to n, i-th is designated as r with the distance at measuring sound source centeri
Second step: allow dead room be in standard atmosphere pressure, measure Celsius temperature T=20 DEG C of dead room, relative humidity hr=50%, frequency of source f=10kHz, calculates sound pressure level attenuation quotient α according to following formula.
α = 8.686 f 2 [ 1.84 × 10 - 11 ( T K T 0 ) - 1 2 + ( T K T 0 ) - 5 2 × ( 0.01275 f r O f r O 2 + f 2 e - 2239.1 T K + 0.1068 f r N f r N 2 + f 2 e - 3352.0 T κ ) ] - - - ( 4 )
In formula, TkFor the absolute temperature of dead room, unit is K, Tk=T+273.15;T0For reference temperature, size is 293.15K;F is the frequency of sound source, and unit is Hz;frOFor oxygen relaxation frequency, unit is Hz;frNFor nitrogen relaxation frequency, unit is Hz, wherein
f r O = 24 + 4.04 × 10 4 h 0.02 + h 0.319 + h - - - ( 5 )
f r N = 9 T 0 T K + 280 e - 4.170 ( T 0 T K 3 - 1 ) T 0 T K h - - - ( 6 )
In formula, h and TkFor,
h = h r 10 - 6.8346 ( T 01 T K ) 1.261 + 4.6151 - - - ( 7 )
TK=T+273.15 (8)
In formula, h is the molar concentration of water vapour, and unit is %;T is the Celsius temperature of dead room, and unit is DEG C;hrFor phase To humidity, unit is %;T01For triple point, size is-273.16K.
Result of calculation obtains sound pressure level attenuation quotient α=0.159.
3rd step: 1. by A and r0Initial value be respectively set to 0 and-0.5;
2. by LPi, ri, A brings following formula into
Q = Σ i = 1 n [ L P i - 20 lg A ( r i - r 0 ) - α ( r 0 - r i ) ] 2 - - - ( 3 )
If 3. Q > 0.5 and r0≤ 0.5, then r0=r0+ 0.00001, return 2.;
If 4. Q > 0.5 and r0> 0.5, then A=A+1, r02.=-0.5, return;
If 5. Q≤0.5, then record A and r now0, terminate to calculate.
Result of calculation obtains A and r0It is respectively 1890 and 0.04904.
4th step: according to following formula and ri, α, A and r0Determine free found field theory sound pressure level curve, as shown in drawings.
L P T i = 20 lg A ( r i - r 0 ) - α ( r 0 - r i ) - - - ( 1 )
In formula, LPTiFor distance Sound Source Center riThe theoretical sound pressure level at place, unit is dB.

Claims (1)

1. an evaluation method for free found field theory sound pressure level in dead room calibration, it specifically comprises the following steps that
The first step: utilize the acoustic pressure of microphone, multiple channel acousto analyser, PULSE test systematic survey tested dead room n point Level, n >=10, measurement result is designated as LPi, unit is dB, i=1,2 ..., n, i-th is designated as with the distance at measuring sound source center ri
Second step: dead room is in standard atmosphere pressure, measures the Celsius temperature T of dead room, relative humidity hr, frequency of source f, According to following formula calculating sound pressure level attenuation quotient α:
α = 8.686 f 2 [ 1.84 × 10 - 11 ( T K T 0 ) - 1 2 + ( T K T 0 ) - 5 2 × ( 0.01275 f r O f r O 2 + f 2 e - 2239.1 T K + 0.1068 f r N f r N 2 + f 2 e - 3352.0 T K ) ]
In formula, TkFor the absolute temperature of dead room, unit is K, Tk=T+273.15;T0For reference temperature, size is 293.15K; F is the frequency of sound source, and unit is Hz;frOFor oxygen relaxation frequency, unit is Hz;frNFor nitrogen relaxation frequency, unit is Hz, wherein
f r O = 24 + 4.04 × 10 4 h 0.02 + h 0.319 + h
f r N = 9 T 0 T K + 280 e - 4.170 ( T 0 T K 3 - 1 ) T 0 T K h
h = h r 10 - 6.8346 ( T 01 T K ) 1.261 + 4.6151
TK=T+273.15
In formula, h is the molar concentration of water vapour, and unit is %;T is the Celsius temperature of dead room, and unit is DEG C;hrFor the wettest Degree, unit is %;T01For triple point, size is-273.16K;
3rd step: 1. by A and r0Initial value be respectively set to 0 and-0.5;
2. by LPi, ri, A brings following formula into
Q = Σ i = 1 n [ L P i - 20 lg A ( r i - r 0 ) - α ( r 0 - r i ) ] 2
If 3. Q > 0.5 and r0≤ 0.5, then r0=r0+ 0.0001, return 2.;
If 4. Q > 0.5 and r0> 0.5, then A=A+1, r02.=-0.5, return;
If 5. Q≤0.5, then record A and r now0, terminate Q and calculate;
4th step: according to following formula and ri, α, A and r0Determine free found field theory sound pressure level curve
L P T i = 20 lg A ( r i - r 0 ) + α ( r 0 - r i )
In formula, LPTiFor distance Sound Source Center riThe theoretical sound pressure level at place, unit is dB.
CN201610352880.8A 2016-05-25 2016-05-25 The evaluation method of free found field theory sound pressure level in a kind of calibration of anechoic room Active CN105973459B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201610352880.8A CN105973459B (en) 2016-05-25 2016-05-25 The evaluation method of free found field theory sound pressure level in a kind of calibration of anechoic room

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201610352880.8A CN105973459B (en) 2016-05-25 2016-05-25 The evaluation method of free found field theory sound pressure level in a kind of calibration of anechoic room

Publications (2)

Publication Number Publication Date
CN105973459A true CN105973459A (en) 2016-09-28
CN105973459B CN105973459B (en) 2018-10-23

Family

ID=56957051

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201610352880.8A Active CN105973459B (en) 2016-05-25 2016-05-25 The evaluation method of free found field theory sound pressure level in a kind of calibration of anechoic room

Country Status (1)

Country Link
CN (1) CN105973459B (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107063445A (en) * 2017-05-04 2017-08-18 中国航发沈阳发动机研究所 A kind of high-frequency acoustic performance detecting system and method
CN110312195A (en) * 2019-07-05 2019-10-08 佛山朗谷创客科技有限公司 A kind of autobalance sound field calibration method

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002365127A (en) * 2001-06-06 2002-12-18 Mitsubishi Heavy Ind Ltd Method and device for estimating acoustic power level of sound source
CN103438988A (en) * 2013-09-02 2013-12-11 浙江省计量科学研究院 Method for automatically measuring and testing sound field of complete anechoic chamber and standard device
CN103438989A (en) * 2013-09-02 2013-12-11 浙江省计量科学研究院 Semi-anechoic room sound field automatic measurement and detection method and standard device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002365127A (en) * 2001-06-06 2002-12-18 Mitsubishi Heavy Ind Ltd Method and device for estimating acoustic power level of sound source
CN103438988A (en) * 2013-09-02 2013-12-11 浙江省计量科学研究院 Method for automatically measuring and testing sound field of complete anechoic chamber and standard device
CN103438989A (en) * 2013-09-02 2013-12-11 浙江省计量科学研究院 Semi-anechoic room sound field automatic measurement and detection method and standard device

Non-Patent Citations (2)

* Cited by examiner, † Cited by third party
Title
蒲志强等: "一种用于消声室校准计算反平方律声压级的新方法", 《计量学报》 *
钟静等: "一种新的消声室声压级的计算方法", 《中国计量学院学报》 *

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN107063445A (en) * 2017-05-04 2017-08-18 中国航发沈阳发动机研究所 A kind of high-frequency acoustic performance detecting system and method
CN110312195A (en) * 2019-07-05 2019-10-08 佛山朗谷创客科技有限公司 A kind of autobalance sound field calibration method

Also Published As

Publication number Publication date
CN105973459B (en) 2018-10-23

Similar Documents

Publication Publication Date Title
US9810598B2 (en) Systems and methods for determining a leak rate through an opening using acoustical sensors
JP6130825B2 (en) Upstream volume mass flow verification system and method
Sherman et al. Uncertainties in fan pressurization measurements
CN104897780B (en) A kind of method positioned using Acoustic Emission Signal Energy to acoustic emission source
CN101473196A (en) Measuring apparatus and methods of using them
CN102865952A (en) Nondestructive testing method for working stress of concrete
CN104729974B (en) A kind of gas gaging hole porosity measuring method for considering temperature effect
CN105973459A (en) Estimation method for theoretical sound pressure level of free sound field in anechoic chamber calibration
CN102928171A (en) Uncertainty determination method of spacecraft total leak rate test result
CN101650220A (en) Method for correcting finite difference error of cross-spectrum sound intensity
RU135795U1 (en) INSTALLATION FOR VERIFICATION AND CALIBRATION OF METERS, FLOW METERS AND FLOW METERS-GAS METERS
CN205808546U (en) A kind of dead room free found field automated calibration system
CN113358290B (en) Stainless steel sealing detection method based on helium mass spectrometer leak detector
Kölsch et al. Quantification of air leakage paths: a comparison of airflow and acoustic measurements
JP2004347389A (en) Wind pressure measuring method
Carrié Temperature and pressure corrections for power-law coefficients of airflow through ventilation system components and leaks
JP2013083515A (en) Inverse square characteristic analyzer and inverse square characteristic evaluation method
CN111854929B (en) Method and system for evaluating uncertainty of sound power level of extra-high voltage main equipment
Dwisetyo et al. Evaluation and Analysis of Uncertainty Measurement of The Sound Level Meter Calibration by Coupler Method
Garai et al. On the uncertainty of sound reduction index measurements from inter-laboratory tests
WO2018196150A1 (en) Sound box air leakage detection device and method, and computer-readable storage medium
RU2533329C1 (en) Verification and calibration unit of gas meters, flow meters and volumeters
Robinson et al. Evaluation of uncertainty in the free-field calibration of hydrophones by the three-transducer spherical wave reciprocity method
Mohamady et al. Statistical uncertainty analysis of an acoustic system
Zhang et al. The investigation of the method for measuring the low-frequency radiated sound power in a reverberation tank

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant