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6 Numerical Techniques Marie D. Dahleh Harvard University
6.1 Introduction ....................................................................... 6-1
6.2 Single-Degree-of-Freedom System ................................... 6-2
Forced Single-Degree-of-Freedom System † Summary of
Single-Degree-of-Freedom System
6.3 Systems with Two or More Degrees of Freedom ............ 6-8
Example † Summary of Two-Degree-of-Freedom System
6.4 Finite Difference Method for a Continuous System ...... 6-11
Bar † Beam † Summary of Finite Difference Methods for a
Continuous System
6.5 Matrix Methods ................................................................. 6-14
Example: Three-Degree-of-Freedom System † Bisection
Method † Directly Calculating the Eigenvalues and
Eigenvectors from the Matrix Equation † Summary of
Matrix Methods
6.6 Approximation Methods for the Fundamental
Frequency ........................................................................... 6-18
Rayleigh Method † Dunkerley’s Formula † Summary of
Approximations for the Fundamental Frequency
6.7 Finite Element Method ..................................................... 6-20
Bar Element † Beam † Summary of Finite Element Method
Appendix 6A Introduction to MATLABw ...................... 6-24
Summary
This chapter gives an overview of numerical techniques for vibration analysis. The centered difference
approximation for the first, second, and fourth derivative are given. These form the basis for the finite difference
approximation of both spring – mass systems and the continuous problem. The fourth-order Runge – Kutta method
is presented. Both of these approaches are used to solve the single-degree-of-freedom (single-DoF) system. In order
to demonstrate these techniques for the multiple-degree-of-freedom (multi-DoF) system a two-degree-of-freedom
(two-DoF) system is explored. Finite element and finite difference methods are presented as solution techniques for
the continuous problem (also see Chapter 9). The bar and beam are used for examples. The Rayleigh method and
Dunkerley’s formula are presented. These are methods for computing the fundamental frequency.
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