CN101975634A - Engine excitation force measurement method employing window length varying phase difference correction method - Google Patents

Engine excitation force measurement method employing window length varying phase difference correction method Download PDF

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CN101975634A
CN101975634A CN 201010288084 CN201010288084A CN101975634A CN 101975634 A CN101975634 A CN 101975634A CN 201010288084 CN201010288084 CN 201010288084 CN 201010288084 A CN201010288084 A CN 201010288084A CN 101975634 A CN101975634 A CN 101975634A
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frequency
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CN101975634B (en
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杨志坚
丁康
王永胜
张绍辉
李魏华
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South China University of Technology SCUT
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Abstract

The invention discloses an engine excitation force measurement method employing a window length varying phase difference correction method. In the method, signal frequency error of an engine excitation frequency interval is solved by utilizing phase difference produced by adding Hanning with different time lengths during signal processing after a vibration acceleration signal on the surface or a suspension point of an engine cylinder is discretely sampled, and the signal frequency error is used for solving actual excitation frequency f, amplitude information and phase information of an engine in a vibration displacement frequency spectrum, so that the vibration displacement vector value in an excitation force measurement formula is accurately obtained and combined with other known engine parameters to calculate the excitation force F (f). The method of the invention can solve the problem that due to the lack of accurate phase information during the engine excitation force measurement, a complex non-linear equation needs to be solved.

Description

Use the engine exciting force measuring method that changes the correction method of window appearance potential difference
Technical field
This aspect relates to power machine and signal Processing field, specifically is a kind of frequency, amplitude, phase method for position of accurate identification of Engine vibration signal, is applied to the identification of engine exciting force.
Background technology
The exciting force of engine mainly is to obtain by the rigid dynamics Model Calculation at present, the excitation that the principal element of considering in calculating is a gas burst power in the cylinder, rotating inertia force and reciprocal inertia force produced.The major defect of this method is need to obtain precise parameters, and the accurate acquisition of some parameter is very difficult, the moment resulting from sidesway that causes as gas burst etc.On the other hand, in actual conditions, engine always links to each other with many annexes, and theoretical calculation formula is not considered the coupling of engine and these annexes usually, this will inevitably cause result of calculation and engineering is actual that certain deviation is arranged, and deviation can be very big in some cases.
In application of practical project, method is by experiment obtained the engine exciting force and is studied by numerous scholars, and this is the problem of typically inverting, and normally adopts the frequency response function matrix method of inverting.But in the vibration control problem of engine, what need is the equivalent force and the equivalent moment at Motor Mass Centre place, owing to can't directly apply excitation at the barycenter place, also the reciprocity method is used in the response that can't directly obtain the barycenter place, therefore can't record transport function, cause the frequency response function matrix method of inverting in the engine exciting force is measured, can't directly use.On the other hand, concerning the exciting force at Motor Mass Centre place was measured, the frequency response function matrix method of inverting was too complicated comparatively speaking.
External scholar J.S.TAO, G.R.LIU and K.Y.LAM etc. has proposed a kind of method (J.S.TAO that measures Motor Mass Centre place exciting force, G.R.LIU and K.Y.LAM is in 2001 articles of delivering on periodical " Journal of Sound and Vibration " " Excitation force identification of an engine with velocity data at mounting points "), point out the amplitude and the phase information of the three-way vibration velocity spectrum at each suspension point place of engine of measuring by extraction, can rebuild the exciting force of engine accurately, the exciting force measure equation
Figure BSA00000278397400011
But this method is when extracting phase information, usually can't obtain absolute phase information, therefore proposed only to utilize phase differential to obtain the method for exciting force, and this processing has been introduced and the measurement identical phase variant of counting that suspends, the non-linear overdetermined equation that makes finding the solution of problem become to find the solution a complexity has increased the complicacy of finding the solution.
Summary of the invention
The objective of the invention is defective at existing recognition methods, the engine exciting force measuring method that a kind of application changes the correction method of window appearance potential difference is proposed, solve for want of accurate phase information in the measurement of engine exciting force, and need find the solution the problem of complex nonlinear equation.
The object of the invention is achieved through the following technical solutions:
A kind of application changes the engine exciting force measuring method of window appearance potential difference correction method, comprises the steps:
(1) coordinate system is set up with correlation parameter and is collected: utilize the engine moment inertia experiment table, test out engine quality m, Motor Mass Centre O, with O is that initial point is set up coordinate system O-XYZ, the Y-axis forward points to crankshaft free-end, and Z axle forward is determined the X-axis forward by the right-hand rule straight up; Utilize the engine moment inertia experiment table to test out the moment of inertia J of engine again around the coordinate system X-axis x, Y-axis moment of inertia J y, the Z axle moment of inertia J z, engine is to the product of inertia J of X-axis and Y-axis Xy, to the inertia J of Y-axis and Z axle Yz, to the inertia J of Z axle and X-axis ZxForm the engine quality matrix M;
(2) obtain the multiple stiffness matrix that suspends: with engine by mount supports at threst stand; Determine engine mounting number h, h=3 or h=3; In the coordinate system O-XYZ of engine, give the label that suspends according to the descending order of directions X, be defined as first suspend, second suspend ... h suspends, and with the elastic body test macro the multiple stiffness characteristics that respectively suspends is tested, and obtains the first multiple rigidity that suspends
Figure BSA00000278397400021
The second multiple rigidity that suspends
Figure BSA00000278397400022
The multiple rigidity that h suspends
Figure BSA00000278397400023
Form the multiple stiffness matrix K that suspends *=[K * 1K * 2K * h];
(3) sensor installation: on the different test points of engine cylinder surface or suspension point, L three-dimensional acceleration transducer is installed, L 〉=3, each test point is installed a three-dimensional acceleration transducer; Sensor connects data acquisition unit, and data acquisition unit connects portable computer; In the coordinate system O-XYZ of engine, determine that according to the descending order of directions X the coordinate of three-dimensional acceleration transducer is respectively [x 1y 1z 1], [x 2y 2z 2] ..., [x Ly Lz L];
(4) on threst stand, setting engine moves with operate as normal rotating speed w, after treating that operating mode is stable, the acquisition time in 10s~30s, the vibration acceleration signal X of X-axis forward, Y-axis forward and Z axle forward by data acquisition unit collection and each test point of synchronous recording 1n, X 2nX LnY 1n, Y 2nY LnZ 1n, Z 2nZ LnX wherein 1nBe the vibration acceleration signal sequence with n point of the first test point X-axis forward collection, X LnBe n the vibration acceleration signal sequence of putting that L test point X-axis forward is gathered, Y 1nBe n the vibration acceleration signal sequence of putting that the first test point Y-axis forward is gathered, X LnThe vibration acceleration signal sequence of n the point that L test point Y-axis forward is gathered; Z 1nBe n the vibration acceleration signal sequence of putting that the first test point Z axle forward is gathered, Z LnThe vibration acceleration signal sequence of n the point that L test point Z axle forward is gathered; Sample frequency f s, sampling number N represents the data point number that discrete series comprises, wherein n=0,1 ..., N-1, require f s=N=2 p, P=9 or 10, frequency resolution Δ f=f s/ N=1;
(6) according to formula
Figure BSA00000278397400024
Measure the engine exciting force, wherein:
Figure BSA00000278397400025
Exciting force F (f) be mean engine under humorous excitation frequency f of rotating speed w η, the exciting force F of engine X-axis forward x(f), around the excitation torque M of X-axis x(f), the exciting force F of Y direction y(f), around the excitation torque M of Y-axis y(f), the exciting force F of Z-direction z(f), around the excitation torque M of Z axle z(f);
K *=[K * 1?K * 2…K * h]
M = m m m J x - J xy - J zx - J xy J y - J yz - J zx - J yz J z
E ‾ = 1 0 0 0 z 1 - y 1 0 1 0 - z 1 0 x 1 0 0 1 y 1 - x 1 0 1 0 0 0 z 2 - y 2 0 1 0 - z 2 0 x 2 0 0 1 y 2 - x 2 0 · · · · · · · · · · · · · · · · · · 1 0 0 0 z 3 - y 3 0 1 0 - z 3 0 x 3 0 0 1 y 3 - x 3 0
f = 1 3 L ( f 1 x + f 1 y + f 1 z + f 2 x + f 2 y + f 2 z + · · · + f Lx + f Ly + f Lz )
S ‾ ( f ) = dX 1 d Y 1 dZ 1 dX 2 dY 2 dZ 2 · · · dX L dY L dZ L T
Figure BSA00000278397400035
Representing matrix
Figure BSA00000278397400036
Transposition;
Humorous excitation frequency f of η and its corresponding transposed matrix
Figure BSA00000278397400037
Determine by the following method:
Humorous the η that selects the engine exciting force to analyze, η=0.5,1,1.5,2,2.5 or 3; Behind humorous time of the η of designated analysis engine speed w, carry out following computing:
Vibration acceleration signal sequence X to the first test point X-axis forward collection with n point 1n, add Hanning window (Hanning) w (t) 0≤t≤T of time length T=1, carry out N point quick Fourier conversion (FFT) according to formula (1-1), obtain amplitude spectrum X 1(f); To X 1nAdd time length
Figure BSA00000278397400038
Hanning window (Hanning) w (t) 0≤t≤T carries out N/2 point quick Fourier conversion (FFT) according to formula (1-2), obtains amplitude spectrum X 2(f);
X 1 ( f ) = Σ n = 0 N - 1 x n [ 0.5 - 0.5 cos ( 2 πn N ) ] e - j 2 π N fn = R 1 ( f ) + jI 1 ( f ) = y 1 ( f ) e j Φ 1 ( f ) f = 0,1 , · · · , N 2 - 1 - - - ( 1 - 1 )
X 2 ( f ) = Σ n = 0 N / 2 - 1 x n [ 0.5 - 0.5 cos ( 4 πn N ) ] e - j 4 π N fn = R 2 ( f ) + jI 2 ( f ) = y 2 ( f ) e j Φ 2 ( f ) f = 0,1 , 2 · · · , N 4 - 1 - - - ( 1 - 2 )
According to engine speed w, determine emending frequency interval [f 1, f 2], wherein
Figure BSA00000278397400045
Round numbers; Round numbers;
At emending frequency interval [f 1, f 2] in, X 1(f) peak-peak respective frequencies f i, f iReal part is R 1(f i), imaginary part is I 1(f i), phase place is Φ 1(f i), amplitude is y 1(f i); X 2(f) peak-peak frequency f j, phase place is Φ 2(f j); If emending frequency interval [f 1, f 2] interior peak-peak actual frequency is f 0, f 0Corresponding true phase place
Figure BSA00000278397400047
True amplitude A 0(f 0); If f iFrequency error be
Figure BSA00000278397400048
f iWith actual frequency f 0Difference
Figure BSA00000278397400049
For people's formula (1-3), obtain frequency error
Figure BSA000002783974000410
▿ f = - 2 [ Φ 1 ( f i ) - Φ 2 ( f j ) - π ( 2 f i - f j ) 2 ] / π - - - ( 1 - 3 )
Calculate actual frequency f 0
Figure BSA000002783974000412
Calculate true phase place
Figure BSA000002783974000413
The spectral function of Hanning window (Hanning)
Figure BSA000002783974000415
Calculate amplitude A after the correction according to formula (1-6) 0(f 0), form actual frequency f 0Acceleration with correspondence
To sequence X 2nX LnY 1n, Y 2nY LnZ 1n, Z 2nZ LnWith the vibration acceleration signal sequence X 1nCarry out same processing, obtain the humorous inferior excitation frequency f of engine speed w η respectively 2xF Lxf 1y, f 2yF Lyf 1z, f 2zF Lz
(1≤H≤L), the engine excitation frequency that records its directions X is f for any sensor H in L the sensor test point Hx, corresponding acceleration is The engine excitation frequency that records the Y direction is f Hy, corresponding acceleration is
Figure BSA000002783974000419
The engine excitation frequency that records the Z direction is f Hz, corresponding acceleration is
Figure BSA00000278397400051
The directions X displacement of sensor H is dX H, the displacement of Y direction is dY H, the displacement of Z direction is dZ H,
Obtain the transposed matrix of sensor H thus:
The excitation frequency of L sensor
Figure BSA00000278397400053
And corresponding transposed matrix
Figure BSA00000278397400054
For realizing that further the object of the invention, described crankshaft free-end are the end that bent axle connects belt pulley.
Described engine is defined as suspension point with the contact point that suspends that supports it.
Described operate as normal rotating speed w is preferably 750r/min to 5500r/min; Described operating mode is stable to be meant that the engine speed fluctuation is in 20r/min.
Described engine moment inertia experiment table preferably adopts three string pendulum method of testing experiment tablees.
The present invention only needs the value by conversion η, η=0.5,1,1.5,2,2.5,3 to the exciting force test of different humorous the η of engine; Calculate different frequency refinement interval [f 1, f 2], recalculate this excitation frequency f and corresponding transposed matrix of humorous time
Figure BSA00000278397400055
Solve humorous the exciting force F of η (f) of engine speed w.
With respect to prior art, the present invention has following advantage:
The present invention is by after sampling to the vibration displacement signal discrete on engine cylinder surface or the suspension point, the phase differential that adds the Hanning window (Hanning) of different time length and produce, utilize precise frequency, amplitude and the phase information of each response point vibration signal of this phase difference correction, thereby improve the measuring accuracy of exciting force.The present invention is in conjunction with J.S.TAO, the exciting force measure equation that G.R.LIU and K.Y.LAM proposes
Figure BSA00000278397400056
Middle K *, M,
Figure BSA00000278397400057
Method for solving proposes to use the correction method of change window appearance potential difference and accurately extracts transposed matrix
Figure BSA00000278397400058
In frequency, amplitude and phase information, improved and utilized the phase differential method to calculate Method, avoided finding the solution of problem having been become the non-linear overdetermined equation of finding the solution a complexity because of utilizing the phase differential method, improved and found the solution
Figure BSA000002783974000510
Precision and efficient, and improved the simplicity that F (f) finds the solution.
Embodiment:
The invention will be further described below in conjunction with embodiment, need to prove, embodiment does not constitute the qualification to the claimed scope of the present invention.
Embodiment 1
(1) utilize three-way pendulum engine rotary inertia experimental bench to test out: certain 1.8L in-line four cylinder engine quality m, Motor Mass Centre O is that initial point is set up coordinate system O-XYZ with barycenter O; And then test out the moment of inertia J of engine around the coordinate system X-axis x, Y-axis moment of inertia J y, the Z axle moment of inertia J z, engine is to the product of inertia J of X-axis and Y-axis Xy, to the inertia J of Y-axis and Z axle Yz, to the inertia J of Z axle and X-axis Zx, form the engine quality matrix M;
M = m m m J x - J xy - J zx - J xy J y - J yz - J zx - J yz J z = 80 kg 80 kg 80 kg 7.5 kgm 2 1.5 kgm 2 - 0.5 kg m 2 1.5 kgm 2 3.5 kgm 2 1 kg m 2 - 0.5 kg m 2 1 kgm 2 6 kgm 2
(2) determine engine mounting number h, h=3; In the coordinate system O-XYZ of engine, give the label that suspends according to the descending order of directions X, be defined as and suspend 1, suspend 2 ... the h that suspends adopts German MTS831 type elastic body test system and test to go out the multiple rigidity that respectively suspends, and forms the multiple stiffness matrix K that suspends *=[k * 1K * 2K * 3]=[be N/m (70000+7000j) N/m (80000+8000j) N/m (75000+7500j)];
(3) 1.8L in-line four cylinder engine is installed on the German FEV threst stand, adopts CPB three-dimensional acceleration transducer, number L=3 is arranged in the suspension point place.Measure the coordinate of 3 sensor test points by three-coordinates measuring machine, form the test point coordinate matrix
E ‾ = 1 0 0 0 z 1 - y 1 0 1 0 - z 1 0 x 1 0 0 1 y 1 - x 1 0 1 0 0 0 z 2 - y 2 0 1 0 - z 2 0 x 2 0 0 1 y 2 - x 2 0 1 0 0 0 z 3 - y 3 0 1 0 - z 3 0 x 3 0 0 1 y 3 - x 3 0 = 1 0 0 0 0.1 - 0.3 0 1 0 - 0.1 0 0 0 0 1 0.3 0 0 1 0 0 0 - 0.2 0.2 0 1 0 0.2 0 0.12 0 0 1 - 0.2 0.12 0 1 0 0 0 - 0.2 0.2 0 1 0 0.2 0 0.12 0 0 1 - 0.2 - 0.12 0
(4) input of CPB three-dimensional acceleration transducer is the data acquisition system (DAS) of German Miller shellfish nurse (BBM) testing apparatus, and data acquisition signal input portable computer is by the PAK test analysis software of installing on the portable computer, real-time monitored and tracer signal;
(5) on threst stand, set engine with certain operate as normal rotating speed w=1815rpm operation, treat the stable back of operating mode (being that the fluctuation of speed is in 20r/min), the beginning image data, the data acquisition system (DAS) of German Miller shellfish nurse (BBM) testing apparatus imported signal by CPB three-dimensional acceleration transducer, by PAK test analysis software, real-time monitored and the tracer signal of installing on the portable computer.Acquisition time length is 30s; Sample frequency f s=512, sampling number N=512, then frequency resolution Δ f=f s/ N=1, the vibration acceleration signal X of X-axis forward, Y-axis forward and Z axle forward by data acquisition unit collection and each test point of synchronous recording 1n, X 2n, X 3nY 1n, Y 2n, Y 3nZ 1n, Z 2n, Z 3nWherein n=0,1 ..., N-1; To vibration acceleration signal X 1n, X 2n, X 3nY 1n, Y 2n, Y 3nZ 1n, Z 2n, Z 3nCarry out the conversion of N=512 point fast Fourier.
According to engine speed w=1815rpm, determine frequency separation [f 1, f 2], the refinement interval of 0.5 humorous excitation frequency f of engine speed w is f 1=10HZ and f 2=20HZ; 1 humorous time refinement interval is f 1=25HZ and f 2=35HZ; 1.5 humorous time refinement interval is f 1=40HZ and f 2=50HZ; 2 humorous times refinement interval is f 1=55HZ and f 2=65HZ; 2.5 humorous time refinement interval is f 1=71HZ and f 2=81HZ; 3 humorous times refinement interval is f 1=86HZ and f 2=96HZ; To each frequency separation [f 1, f 2], to use to change window appearance potential difference method, concrete steps are carried out according to formula (1-1) to (1-7).
3), only list 1 humorous time and 2 humorous times the excitation frequency f of engine speed w here, the 1 humorous secondary frequencies interval [f of engine speed w owing to the length relation 1, f 2]=[25,35], use to change window appearance potential difference method, obtain 3 sensor correspondences the excitation frequency f and the acceleration of test point separately As shown in table 1; The 2 humorous secondary frequencies interval [f of engine speed w 1, f 2]=[55,65], use to change window appearance potential difference method, obtain 3 sensor correspondences the excitation frequency f and the acceleration of test point separately
Figure BSA00000278397400072
As shown in table 2;
1 humorous secondary frequencies and the acceleration of table 1 engine speed w
Figure BSA00000278397400081
2 humorous secondary frequencies and the accelerations of table 2 engine speed w
Figure BSA00000278397400082
Obtain thus: when
Figure BSA00000278397400083
The time,
Transposed matrix Wherein:
dX 1 d Y 1 dZ 1 = - 1 2 π * 30.25 0.174 e - 179.37 j - 1 2 π * 30 . 25 0.0491 e 179.42 j - 1 2 π * 30.25 0.4436 e 0.48 j
dX 2 d Y 2 dZ 2 = - 1 2 π * 30.25 0 . 0518 e 1.81 j - 1 2 π * 30 . 25 0 . 1887 e 1 . 08 j - 1 2 π * 30.25 0.0417 e - 176 . 19 j
dX 3 d Y 3 dZ 3 = - 1 2 π * 30.25 0 . 0518 e 1.81 j - 1 2 π * 30 . 25 0 . 4715 e 0 . 56 j - 1 2 π * 30.25 0 . 3353 e - 176 . 7 j
When
Figure BSA00000278397400088
The time,
Transposed matrix
Figure BSA00000278397400089
Wherein:
dX 1 d Y 1 dZ 1 = - 1 2 π * 60.5 0 . 2061 e 0.17 j - 1 2 π * 60 . 5 0 . 1592 e 0 . 25 j - 1 2 π * 60 . 5 1 . 1794 e 0 . 06 j
dX 2 d Y 2 dZ 2 = - 1 2 π * 60.5 1 . 7755 e - 179.79 j - 1 2 π * 60 . 5 0 . 3839 e - 179.93 j - 1 2 π * 60 . 5 2 . 877 1 e 0 . 12 j
dX 3 d Y 3 dZ 3 = - 1 2 π * 60.5 1 . 7755 e - 179.79 j - 1 2 π * 60 . 5 0 . 5075 e - 0 . 15 j - 1 2 π * 60 . 5 0 . 1938 e - 179.53 j
(7) fundamental formular of measuring according to the engine exciting force Wherein:
Figure BSA00000278397400095
For the mass matrix M among the people (1), the multiple stiffness matrix K that suspends in (2) *, the measuring point coordinates matrix in (3)
Figure BSA00000278397400096
When asking 1 humorous exciting force of engine speed w, for people f=30.25HZ and
Figure BSA00000278397400097
1 humorous exciting force obtaining engine start machine rotating speed w is as shown in table 3; When asking 2 humorous exciting forces of engine speed w, for people f=60.5HZ and
Figure BSA00000278397400098
2 humorous exciting forces obtaining engine start machine rotating speed w are as shown in table 4;
1 humorous exciting force of table 3 engine speed w
Figure BSA00000278397400099
2 humorous exciting forces of table 4 engine speed w
Figure BSA000002783974000910
Figure BSA00000278397400101
Embodiment 1 has illustrated that the present invention is by after sampling to the vibration displacement signal discrete on engine cylinder surface or the suspension point, the phase differential that adds the Hanning window (Hanning) of different time length and produce, utilize precise frequency, amplitude and the phase information of each response point vibration signal of this phase difference correction, thereby improve the measuring accuracy of exciting force.

Claims (5)

1. use the engine exciting force measuring method that changes the correction method of window appearance potential difference, it is characterized in that comprising the steps:
(1) coordinate system is set up with correlation parameter and is collected: utilize the engine moment inertia experiment table, test out engine quality m, Motor Mass Centre O, with O is that initial point is set up coordinate system O-XYZ, the Y-axis forward points to crankshaft free-end, and Z axle forward is determined the X-axis forward by the right-hand rule straight up; Utilize the engine moment inertia experiment table to test out the moment of inertia J of engine again around the coordinate system X-axis x, Y-axis moment of inertia J y, the Z axle moment of inertia J z, engine is to the product of inertia J of X-axis and Y-axis Xy, to the inertia J of Y-axis and Z axle Yz, to the inertia J of Z axle and X-axis Zx, form the engine quality matrix M;
(2) obtain the multiple stiffness matrix that suspends: with engine by mount supports at threst stand; Determine engine mounting number h, h=3 or h=3; In the coordinate system O-XYZ of engine, give the label that suspends according to the descending order of directions X, be defined as first suspend, second suspend ... h suspends, and with the elastic body test macro the multiple stiffness characteristics that respectively suspends is tested, and obtains the first multiple rigidity that suspends
Figure FSA00000278397300011
The second multiple rigidity that suspends
Figure FSA00000278397300012
The multiple rigidity that h suspends
Figure FSA00000278397300013
Form the multiple stiffness matrix K that suspends *=[K * 1K * 2K * h];
(3) sensor installation: on the different test points of engine cylinder surface or suspension point, L three-dimensional acceleration transducer is installed, L 〉=3, each test point is installed a three-dimensional acceleration transducer; Sensor connects data acquisition unit, and data acquisition unit connects portable computer; In the coordinate system O-XYZ of engine, determine that according to the descending order of directions X the coordinate of three-dimensional acceleration transducer is respectively [x 1y 1z 1], [x 2y 2z 2] ..., [x Ly Lz L];
(4) on threst stand, setting engine moves with operate as normal rotating speed w, after treating that operating mode is stable, the acquisition time in 10s~30s, the vibration acceleration signal X of X-axis forward, Y-axis forward and Z axle forward by data acquisition unit collection and each test point of synchronous recording 1n, X 2nX LnY 1n, Y 2nY LnZ 1n, Z 2nZ LnX wherein 1nBe the vibration acceleration signal sequence with n point of the first test point X-axis forward collection, X LnBe n the vibration acceleration signal sequence of putting that L test point X-axis forward is gathered, Y 1nBe n the vibration acceleration signal sequence of putting that the first test point Y-axis forward is gathered, X LnThe vibration acceleration signal sequence of n the point that L test point Y-axis forward is gathered; Z 1nBe n the vibration acceleration signal sequence of putting that the first test point Z axle forward is gathered, Z LnThe vibration acceleration signal sequence of n the point that L test point Z axle forward is gathered; Sample frequency f s, sampling number N represents the data point number that discrete series comprises, wherein n=0,1 ..., N-1, require f s=N=2 p, P=9 or 10, frequency resolution Δ f=f s/ N=1;
(5) according to formula
Figure FSA00000278397300014
Measure the engine exciting force, wherein: Exciting force F (f) be mean engine under humorous excitation frequency f of rotating speed w η, the exciting force F of engine X-axis forward x(f), around the excitation torque M of X-axis x(f), the exciting force F of Y direction y(f), around the excitation torque M of Y-axis y(f), the exciting force F of Z-direction z(f), around the excitation torque M of Z axle z(f);
K *=[K * 1?K * 2?…K * h]
M = m m m J x - J xy - J zx - J xy J y - J yz - J zx - J yz J z
E ‾ = 1 0 0 0 z 1 - y 1 0 1 0 - z 1 0 x 1 0 0 1 y 1 - x 1 0 1 0 0 0 z 2 - y 2 0 1 0 - z 2 0 x 2 0 0 1 y 2 - x 2 0 · · · · · · · · · · · · · · · · · · 1 0 0 0 z 3 - y 3 0 1 0 - z 3 0 x 3 0 0 1 y 3 - x 3 0
f = 1 3 L ( f 1 x + f 1 y + f 1 z + f 2 x + f 2 y + f 2 z + · · · + f Lx + f Ly + f Lz )
S ‾ ( f ) = dX 1 d Y 1 dZ 1 dX 2 dY 2 dZ 2 · · · dX L dY L dZ L T
Representing matrix
Figure FSA00000278397300026
Transposition;
Humorous excitation frequency f of η and its corresponding transposed matrix
Figure FSA00000278397300027
Determine by the following method:
Humorous the η that selects the engine exciting force to analyze, η=0.5,1,1.5,2,2.5 or 3; Behind humorous time of the η of designated analysis engine speed w, carry out following computing:
Vibration acceleration signal sequence X to the first test point X-axis forward collection with n point 1n, add Hanning window w (t) 0≤t≤T of time length T=1, carry out the conversion of N point quick Fourier according to formula (1-1), obtain amplitude spectrum X 1(f); To X 1nAdd time length
Figure FSA00000278397300028
Hanning window w (t) 0≤t≤T carries out N/2 point quick Fourier conversion (FFT) according to formula (1-2), obtains amplitude spectrum X 2(f);
X 1 ( f ) = Σ n = 0 N - 1 x n [ 0.5 - 0.5 cos ( 2 πn N ) ] e - j 2 π N fn = R 1 ( f ) + jI 1 ( f ) = y 1 ( f ) e j Φ 1 ( f ) f = 0,1 , · · · , N 2 - 1 - - - ( 1 - 1 )
X 2 ( f ) = Σ n = 0 N / 2 - 1 x n [ 0.5 - 0.5 cos ( 4 πn N ) ] e - j 4 π N fn = R 2 ( f ) + jI 2 ( f ) = y 2 ( f ) e j Φ 2 ( f ) f = 0,1 , 2 · · · , N 4 - 1 - - - ( 1 - 2 )
According to engine speed w, determine emending frequency interval [f 1, f 2], wherein
Figure FSA00000278397300033
Round numbers;
Figure FSA00000278397300034
Round numbers;
At emending frequency interval [f 1, f 2] in, X 1(f) peak-peak respective frequencies f i, f iReal part is R 1(f i), imaginary part is I 1(f i), phase place is Φ 1(f i), amplitude is y 1(f i); X 2(f) peak-peak frequency f j, phase place is Φ 2(f j); If emending frequency interval [f 1, f 2] interior peak-peak actual frequency is f 0, f 0Corresponding true phase place
Figure FSA00000278397300035
True amplitude A 0(f 0); If f iFrequency error be
Figure FSA00000278397300036
f iWith actual frequency f 0Difference
Figure FSA00000278397300037
For people's formula (1-3), obtain frequency error
Figure FSA00000278397300038
▿ f = - 2 [ Φ 1 ( f i ) - Φ 2 ( f j ) - π ( 2 f i - f j ) 2 ] / π - - - ( 1 - 3 )
Calculate actual frequency f 0
Figure FSA000002783973000310
Calculate true phase place
Figure FSA000002783973000311
Figure FSA000002783973000312
The spectral function of Hanning window
Figure FSA000002783973000313
Calculate amplitude A after the correction according to formula (1-6) 0(f 0), form actual frequency f 0Acceleration with correspondence
Figure FSA000002783973000314
Figure FSA000002783973000315
To sequence X 2nX LnY 1n, Y 2nY LnZ 1n, Z 2nZ LnWith the vibration acceleration signal sequence X 1nCarry out same processing, obtain the humorous inferior excitation frequency f of engine speed w η respectively 2xF Lxf 1y, f 2yF Lyf 1z, f 2zF Lz
(1≤H≤L), the engine excitation frequency that records its directions X is f for any sensor H in L the sensor test point Hx, corresponding acceleration is
Figure FSA000002783973000316
The engine excitation frequency that records the Y direction is f Hy, corresponding acceleration is
Figure FSA000002783973000317
The engine excitation frequency that records the Z direction is f Hz, corresponding acceleration is
Figure FSA000002783973000318
The directions X displacement of sensor H is dX H, the displacement of Y direction is dY H, the displacement of Z direction is dZ H, obtain the transposed matrix of sensor H thus:
Figure FSA00000278397300041
The excitation frequency of L sensor
Figure FSA00000278397300042
And corresponding transposed matrix
Figure FSA00000278397300043
2. application according to claim 1 changes the engine exciting force measuring method of window appearance potential difference correction method, it is characterized in that: described crankshaft free-end is the end that bent axle connects belt pulley.
3. application according to claim 1 changes the engine exciting force measuring method of window appearance potential difference correction method, it is characterized in that: described engine is defined as suspension point with the contact point that suspends that supports it.
4. application according to claim 1 changes the engine exciting force measuring method of window appearance potential difference correction method, and it is characterized in that: described operate as normal rotating speed w is 750r/min to 5500r/min; Described operating mode is stable to be meant that the engine speed fluctuation is in 20r/min.
5. application according to claim 1 changes the engine exciting force measuring method of window appearance potential difference correction method, and it is characterized in that: described engine moment inertia experiment table adopts three string pendulum method of testing experiment tablees.
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CN102680270A (en) * 2012-06-07 2012-09-19 哈尔滨工程大学 Indirect measurement method for ship excitation load caused by equipment under combined effect of unbalanced excitation force and unbalanced bending moment
CN102680270B (en) * 2012-06-07 2014-08-06 哈尔滨工程大学 Indirect measurement method for ship excitation load caused by equipment under combined effect of unbalanced excitation force and unbalanced bending moment
CN106855119A (en) * 2015-12-08 2017-06-16 通用汽车环球科技运作有限责任公司 Control using Fast Fourier Transform (FFT) to buncher
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CN105403344A (en) * 2015-12-16 2016-03-16 浙江大学 Pipeline real-time stress obtaining method
CN105403344B (en) * 2015-12-16 2018-03-16 浙江大学 The acquisition methods of the real-time stress of pipeline
CN106970264A (en) * 2017-03-02 2017-07-21 浙江大学 A kind of improvement phase difference correction method for considering mains frequency rate of change
CN106970264B (en) * 2017-03-02 2020-02-21 浙江大学 Improved phase difference correction method considering power grid frequency change rate
CN109507495A (en) * 2018-10-17 2019-03-22 华北水利水电大学 It is a kind of to become the long quasi- simultaneous interconnecting measurement method of parameters of window
CN109507495B (en) * 2018-10-17 2020-12-15 华北水利水电大学 Variable-window-length quasi-synchronization grid-connected parameter measurement method

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