SAE AIR 1289A-1992 Evaluation of Helicopter Turbine Engine Linear Vibration Environment.pdf
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1、SAE AIR*1289A 92 m 79113725 05062L8 7111 m REV. AIR1289 A mA =For The Advancing Engimhg Mobility Sociey AEROSPACE INFORMATION -Land Sea Air and Space INTERNATIONA L Issued 1976-09 Revised 1992-03-31 400 Commonwealth Drive, Warrendale, PA 15096-0001 RE PORT Submitted for recognition as an American Na
2、tional Standard I EVALUATION OF HELICOPTER TURBINE ENGINE LINEAR VIBRATION ENVIRONMENT 1. SCOPE: This SAE Aerospace Informat i on Report (AIR) out1 ines a recommended procedure for evaluation of the vibration environment to which the gas turbine engine powerplant is subjected in the helicopter insta
3、llation. This analysis of engine vibration is normally demonstrated on a one-time basis upon initial certification, or after a major modification, of an engine/hel icopter configuration. This AIR deals with linear vibration as measured on the basic case structure of the engine and not, for example,
4、torsional vibration in drive shafting or vibration of a component within the engine such as a compressor or turbine airfoil. In summary, this AIR discusses the engine manufacturers “Installation Test Code“ aspects of engine vi bration and proposes an appropriate measurement method. 2. REFERENCES: Th
5、ere are no referenced pub1 ications specified herein. 3. BACKGROUND: 3.1 The vibratory excitation which a gas turbine engine experiences is a function of the vibration produced by the engine and the vibration produced by the installation. level be within a range to which the engine is tolerant. 3.2
6、The vibrations measured on the engine casing may provide only an indication of the state of vibratory motions and stresses of individual components within the engine. The method of measurement, the chosen limits, and the location of the sensor should ensure a credible evaluation appropriate to the m
7、ajority of cases. A satisfactory system requires that this combined vibratory SAE Technical Standards Board Rules provide that: “This report is published by SAE to advance the state of technical and engineering sciences. The use of this report is entirely voluntary. and its applicability and suitabi
8、lity tor any particular use, including any patent infringement arising therefrom, is the sole responsibility of the user.“ SAE reviews each technical report at least every five years at which time it may be reaffirmed, revised, or cancelled. SAE invites your written comments and suggestions. C Copyr
9、ight 1992 Society of Automotive Engineers, Inc. All rights reserved. Printed in U.S.A. SAE AIR*kL287A 72 m 7743725 050b2l17 650 m SAE AIR1289 Revision A 3.3 3.4 3.5 The source of a vibratory input is normally detectable by the frequency of the excitation which is measured in cycles per second and ex
10、pressed as “Hertz“ (Hz). approximately 60 to 15 O00 Hz; however, frequencies above 2000 Hz are generally of no interest due to the low input energy level. Engine-generated vi brat ion may be produced at frequencies corresponding to the rotational speeds of the engine output shaft, the gas generator
11、and power turbine rotors, major accessories and at gear tooth meshing frequencies, bearings, and harmonics of this and possible subharmonic resonance of shaft i ng . The helicopter may expose the engine to vibratory inputs from 3 Hz to as high as approximately 1000 Hz if the engine is direct-mounted
12、 to the main transmission. The major sources of low frequency excitation from the he1 icopter are: The gas turbine engine may produce frequencies from a. b. c. Harmonics of the latter Main rotor forces and moments at one-per-rev Main rotor blade passing frequency (main rotor frequency times the numb
13、er of blades) Tail rotor and drive shafting produce other higher frequency vibrations. Airframe-aenerated vibrations may be amp1 ified or attenuated by the airframe structura7 dynamics. The stiffness and/or damping important factors of the eng inputs. The vibration spectrum to wh characteris ne/airf
14、rame ics of the engine mounts are dynamic response to vibratory ch the sens r is subjected is composed of a number of superimposed harmonic (sinusoidal) vibrations of different frequencies expressed by the general function: where: x, = Peak value of x,(t) oi = Angular frequency of the excitation -2-
15、 SAE AIRLL287A 92 7743725 050b220 372 SAE AIR1289 Revision A 3.5 (Continued): In a helicopter installation there are several main sources of excitation: he1 icopter main rotor frequency (U mr), he1 icopter rotor blade passing frequency (N O mr, N = number of blades), gas generator rotating frequency
16、 (U gg), engine drive shaft and reduction gearbox rotating frequency (U ds) and when applicable free power turbine rotating frequency. of the response to these excitations is: The summation S i=nl j=n2 1 =n3 - S(t) = E x, sin i o,t + E yj sin j o,t t E i=l j-1 1=1 m-4 z, sin 1 uqqt t C O m sin m odr
17、t m= 1 In practice the contributions from higher level harmonics corresponding to n 2 are generally quickly decreasing, have low energy, and therefore the significant vibratory signal can be limited to the second harmonic of each excitation (i .e., 2/rev of each excitation mentioned). In cases where
18、 the response to n 2 is significant, there usually is a resonance of an engine mode with that harmonic. 3.6 Vibration measurements may be accomplished by sensing various parameters which are characteristic of the excitation: a. b. c. Displacement magnitude Id“ in microns (.O01 nun) or mils (.O01 in)
19、 Velocity magnitude “v“ in centimeters per second or inches per second Acceleration magnitude “a“ in meters per second per second or in gs (vector quantity, 980 cm/s2 = 1 g or 386 in/s2 = 1 g) d. Frequency If“ in hertz (cycles per second) In practice accelerometers and velocimeters are used to measu
20、re the vi bration. The overall acceleration signals may be processed through different signal conditioning methods: a. Peak value method, correct only for a pure sinusoidal vibration signal b. Average value method, defined as -3- SAE AIR*1289A 92 7943725 050b221 209 SAE AIR1289 Revision A 3.6 (Conti
21、nued): which consists in averaging the signal. automatically compensating for frequency but has the disadvantage of masking peak values by flattening the sampling. sinusoidal function over which the average is calculated.) This method has the advantage of (T being the period of the c. The first two
22、methods are only mentioned for information, the rms value is the basis of the method used in this AIR, although any of the three can be used successfully as long as it is used consistently throughout engine deve1 opment. Root mean square value method (rms) which is more representative of the energy
23、content of the vibration. 3.6.1 RMS Value Method: For an instantaneous value of the general function xi (t) = x, sin o,t (where x, is the peak value) (Eq.4) the rms value is given by: where: T = Period of the sinusoidal function For a given harmonic, xi xi rms = - is the rms value of x,(t) 42 A typi
24、cal vibration spectrum is given in Figure 1. Acceleration, velocity, and displacement are used to characterize the oscillating motion with regard to the limits to be adopted for an engine. By measuring the acceleration through sensors fitted on the engine structure, the processing to transform it in
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