Pure odd-order oscillators with constant excitation

被引:20
作者
Cveticanin, L.
机构
[1] Faculty of Technical Sciences, 21000 Novi Sad
关键词
PERTURBATION METHOD; EQUATIONS; BEAMS; BEHAVIOR; COLUMNS; FORCE;
D O I
10.1016/j.jsv.2010.09.011
中图分类号
O42 [声学];
学科分类号
070206 ; 082403 ;
摘要
In this paper the excited vibrations of a truly nonlinear oscillator are analyzed. The excitation is assumed to be constant and the nonlinearity is pure (without a linear term). The mathematical model is a second-order nonhomogeneous differential equation with strong nonlinear term. Using the first integral, the exact value of period of vibration i.e., angular frequency of oscillator described with a pure nonlinear differential equation with constant excitation is analytically obtained. The closed form solution has the form of gamma function. The period of vibration depends on the value of excitation and of the order and coefficient of the nonlinear term. For the case of pure odd-order-oscillators the approximate solution of differential equation is obtained in the form of trigonometric function. The solution is based on the exact value of period of vibration. For the case when additional small perturbation of the pure oscillator acts, the so called 'Cveticanin's averaging method' for a truly nonlinear oscillator is applied. Two special cases are considered: one, when the additional term is a function of distance, and the second, when damping acts. To prove the correctness of the method the obtained results are compared with those for the linear oscillator. Example of pure cubic oscillator with constant excitation and linear damping is widely discussed. Comparing the analytically obtained results with exact numerical ones it is concluded that they are in a good agreement. The investigations reported in the paper are of special interest for those who are dealing with the problem of vibration reduction in the oscillator with constant excitation and pure nonlinear restoring force the examples of which can be found in various scientific and engineering systems. For example, such mechanical systems are seats in vehicles, supports for machines, cutting machines with periodical motion of the cutting tools, presses, etc. The examples can be find in electronics (electromechanical devices like micro-actuators and micro oscillators), in music instruments (hammers in piano), in human voice producing folds (voice cords), etc. (C) 2010 Elsevier Ltd. All rights reserved.
引用
收藏
页码:976 / 986
页数:11
相关论文
共 26 条
[1]  
Abramowitz M., 1979, Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables
[2]  
[Anonymous], 2010, Truly Nonlinear Oscillations
[3]  
BOGOLIUBOFF N, 1963, ASYMPTOTICAL METHODS
[4]   A PERTURBATION METHOD FOR CERTAIN NON-LINEAR OSCILLATORS [J].
BURTON, TD .
INTERNATIONAL JOURNAL OF NON-LINEAR MECHANICS, 1984, 19 (05) :397-407
[5]   Property distribution determination for nonuniform composite beams from vibration response measurements and Galerkin's method [J].
Chen, WH ;
Gibson, RF .
JOURNAL OF APPLIED MECHANICS-TRANSACTIONS OF THE ASME, 1998, 65 (01) :127-133
[6]  
Colm I.J., 1988, FORMING SHAPING WORK
[7]   Homotopy-perturbation method for pure nonlinear differential equation [J].
Cveticanin, L. .
CHAOS SOLITONS & FRACTALS, 2006, 30 (05) :1221-1230
[8]  
Cveticanin L, 2009, INT J NONLIN SCI NUM, V10, P1491
[9]   Oscillator with fraction order restoring force [J].
Cveticanin, L. .
JOURNAL OF SOUND AND VIBRATION, 2009, 320 (4-5) :1064-1077
[10]  
GRADSHTEIN IS, 1971, TABLICI INTEGRALOV S