Analysis of dynamic instability of the wheel set of a railway vehicle using the method of generalized hill determinants

Janat Musayev1 , Algazy Zhauyt2 , Balzhan Bahtiyar3 , Rita Kibitova4 , Kushtar Kazhet5 , Alisher Kussyov6 , Anar Kabylkarim7

1, 3, 4Department of Highway Engineering, Academy of Logistics and Transport, Almaty, 050012, Kazakhstan

2, 5, 6, 7Department of Electronics and Robotics, Almaty University of Power Engineering and Telecommunications, Almaty, 050013, Kazakhstan

1Corresponding author

Vibroengineering PROCEDIA, Vol. 41, 2022, p. 186-190.
Received 2 March 2022; received in revised form 9 April 2022; accepted 13 April 2022; published 21 April 2022

55th International Conference on Vibroengineering, Almaty, Kazakhstan, April 21, 2022

Copyright © 2022 Janat Musayev, et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
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The article considers the tasks associate with the study of dynamic processes of interaction between rolling stock and railways. Studies of the interaction of a wheel with a rail, fitting the vehicle into curves when modeling critical and emergency situations do not allow oversimplification of basic differential equations. And they should be based on exact nonlinear equations that take into account the entire set of geometric and kinematic relationships without simplification. An objective assessment dynamic characteristic of the vehicle can only be obtained by simultaneously taking into account both its vertical and horizontal irregularities. In order to determine boundaries of parametric resonance, article proposes method of generalized Hill’s determinants, the application of which is possible without taking into account small parameters.

Analysis of dynamic instability of the wheel set of a railway vehicle using the method of generalized hill determinants

Keywords: wheel set, railway vehicle, kinematic relation, horizontal, vibration.

1. Introduction

As is well known, the issues related to vibrations of mechanical systems represent a very voluminous section of applied mechanics. This section is based on fundamental domestic and foreign research in field of nonlinear oscillation theory. This section of mechanics has effective methods and a wide range of solved problems. At the same time, development of modern transport equipment constantly puts forward new urgent problematic issues. One of these issues is related to the study of oscillation in elastic systems transport equipment. One of the most effective ways to improve design and reduce energy costs of transport equipment is based study of the phenomenon resonance. In an oscillating system, which is in resonance state, elastic and inertial forces are mutually balanced. And the energy of the exciter oscillations is spent only on overcoming dissipative forces, while the system itself performs its own motion.

2. Materials and methods

The most common method for finding boundary of the instability region is based on the Fourier series. Another method is the use of generalized Hill determinants. The equations of parametric oscillations linear systems with finite number degrees of freedom are generally represented as:


where qt is the vector of generalized coordinates, At, Bt and Ct square matrices whose elements are real functions of time. It is assumed that the matrix At is the positive definite for all t, and no restrictions are imposed on the other matrices. Unless otherwise stated, all matrix coefficients are continuous periodic functions of time with period T:

At+T=At,      Bt+T=Bt,     Ct+T=Ct.

The frequency corresponding to this period ω=2π/T is called the parametric excitation frequency. We write Eq. (1) in the Cauchy normal form by introducing the vector of phase variables x:


The method of generalized Hill determinants [1] is based on representation one of the solutions general Eq. (3) in the form:

qkt=ehktχkt,     k=1,2,,2n,

where χ(t)T periodic continuous functions:


Characteristic indices. Let the matrix function Gt in Eq. (3) be decomposed into a Fourier series in time:


with constant coefficients – matrices Gk and Hk. Expanding the periodic vector function in solution Eq. (4) into a similar series, we look for this solution in the form:


where h – is the unknown characteristic exponent, ak and bk – is the unknown number vectors. Substitution of series Eq. (6) and Eq. (7) into Eq. (3) after equating the coefficients for the same functions time leads to an infinite system linear homogeneous algebraic equations. These are equations for the components of the vectors – the coefficients of the series Eq. (7). The condition existence of a nontrivial solution system is that its determinant is equal to zero [3]. Thus, the characteristic exponents h are roots of the algebraic equation:


where K and E – matrices of infinite order and the matrix E – is identity matrix, and matrix K has following block structure:


where ω=2Ω.

Note that under sufficiently broad assumptions about properties matrices Gk and Hk the infinite determinant turns out to be convergent. Consequently, reduction to determinants of finite order is allowed [3].

Now we take into account the third harmonic in solving the Mathieu equation:


Further, following the above method, we get:


3. Results and discussion

Based on the results of analytical calculations, the authors obtained graphs of the main region of dynamic instability of the wheel set of a railway vehicle. As well parametric resonances when taking into account the third harmonic in solving the Mathieu equation and the zone of instability of the wheel set of the vehicle, taking into account the fifth harmonic in solving the Mathieu equation (see Figs. 1-3).

Fig. 1 shows the main region of dynamic instability of system under consideration.

Fig. 1. The main area of dynamic instability wheel set of the vehicle

The main area of dynamic instability wheel set of the vehicle

We determine eigenvalues of the matrix Eq. (11) and present results form of the corresponding graphs areas of instability in Fig. 2.

Fig. 2. Areas of parametric resonances when taking into account the third harmonics solution of the Mathieu equation

Areas of parametric resonances when taking into account  the third harmonics solution of the Mathieu equation

Let us add the fifth harmonic solution of the original equation and after simple transformations, we obtain a matrix of the form:


Determining its eigenvalues, we construct the boundaries of the parametric resonance regions shown in Fig. 3.

Fig. 3. Zones of instability wheel set of the vehicle taking into account the fifth harmonic solution of the Mathieu equation

Zones of instability wheel set of the vehicle taking into account  the fifth harmonic solution of the Mathieu equation

Note here that we have defined only odd zones of dynamic instability. So, to calculate boundaries of the second resonance region, solution of the Mathieu equation must be sought in the form:


It is easy to see that other areas of dynamic instability begin to appear in the figure. Therefore, by continuing to increase number of terms in series Eq. (7), we can refine boundaries of already established parametric resonance zones, while also finding new ones (after all, there are an infinite number of them).

4. Conclusions

As studies have shown, the possibilities of analytical methods are very limited. In practice, they can be used as a rule, only for relatively simple systems and only under certain restrictions on the characteristics of systems. For example, nonlinearity must be weak, i.e. must contain as a factor small parameter and/or random perturbations acting in the system. An analysis of the studies performed showed that in nonlinear problems, each method usually makes it possible to find far from all the statistical characteristics of the system's motion.


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