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9781905209279

Vibration in Continuous Media

by
  • ISBN13:

    9781905209279

  • ISBN10:

    1905209274

  • Edition: 1st
  • Format: Hardcover
  • Copyright: 2006-09-22
  • Publisher: Wiley-ISTE

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Supplemental Materials

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Summary

Three aspects are developed in this book: modeling, a description of the phenomena and computation methods. A particular effort has been made to provide a clear understanding of the limits associated with each modeling approach. Examples of applications are used throughout the book to provide a better understanding of the material presented.

Author Biography

Jean-Louis Guyader is the director of the vibration and acoustics laboratory and a professor of vibration and acoustics in the mechanical engineering department at the Institut National des Sciences AppliquTes–Lyon.

Table of Contents

Preface 13(4)
Vibrations of Continuous Elastic Solid Media
17(28)
Objective of the chapter
17(1)
Equations of motion and boundary conditions of continuous media
18(10)
Description of the movement of continuous media
18(3)
Law of conservation
21(2)
Conservation of mass
23(1)
Conservation of momentum
23(2)
Conservation of energy
25(1)
Boundary conditions
26(2)
Study of the vibrations: small movements around a position of static, stable equilibrium
28(16)
Linearization around a configuration of reference
28(4)
Elastic solid continuous media
32(1)
Summary of the problem of small movements of an elastic continuous medium in adiabatic mode
33(1)
Position of static equilibrium of an elastic solid medium
34(1)
Vibrations of elastic solid media
35(2)
Boundary conditions
37(1)
Vibrations equations
38(1)
Notes on the initial conditions of the problem of vibrations
39(1)
Formulation in displacement
40(1)
Vibration of viscoelastic solid media
40(4)
Conclusion
44(1)
Variational Formulation for Vibrations of Elastic Continuous Media
45(32)
Objective of the chapter
45(1)
Concept of the functional, bases of the variational method
46(10)
The problem
46(1)
Fundamental lemma
46(1)
Basis of variational formulation
47(3)
Directional derivative
50(5)
Extremum of a functional calculus
55(1)
Reissner's functional
56(5)
Basic functional
56(3)
Some particular cases of boundary conditions
59(1)
Case of boundary conditions effects of rigidity and mass
60(1)
Hamilton's functional
61(2)
The basic functional
61(1)
Some particular cases of boundary conditions
62(1)
Approximate solutions
63(1)
Euler equations associated to the extremum of a functional
64(11)
Introduction and first example
64(4)
Second example: vibrations of plates
68(4)
Some results
72(3)
Conclusion
75(2)
Equation of Motion for Beams
77(34)
Objective of the chapter
77(1)
Hypotheses of condensation of straight beams
78(2)
Equations of longitudinal vibrations of straight beams
80(9)
Basic equations with mixed variables
80(5)
Equations with displacement variables
85(1)
Equations with displacement variables obtained by Hamilton's functional
86(3)
Equations of vibrations of torsion of straight beams
89(4)
Basic equations with mixed variables
89(2)
Equation with displacements
91(2)
Equations of bending vibrations of straight beams
93(11)
Basic equations with mixed variables: Timoshenko's beam
93(4)
Equations with displacement variables: Timoshenko's beam
97(4)
Basic equations with mixed variables: Euler-Bernoulli beam
101(1)
Equations of the Euler-Bernoulli beam with displacement variable
102(2)
Complex vibratory movements: sandwich beam with a flexible inside
104(5)
Conclusion
109(2)
Equation of Vibration for Plates
111(28)
Objective of the chapter
111(1)
Thin plate hypotheses
112(4)
General procedure
112(1)
In plane vibrations
112(1)
Transverse vibrations: Mindlin's hypotheses
113(1)
Transverse vibrations: Love-Kirchhoff hypotheses
114(1)
Plates which are non-homogenous in thickness
115(1)
Equations of motion and boundary conditions of in plane vibrations
116(5)
Equations of motion and boundary conditions of transverse vibrations
121(9)
Mindlin's hypotheses: equations with mixed variables
121(2)
Mindlin's hypotheses: equations with displacement variables
123(1)
Love-Kirchhoff hypotheses: equations with mixed variables
124(3)
Love-Kirchhoff hypotheses: equations with displacement variables
127(2)
Love-Kirchhoff hypotheses: equations with displacement variables obtained using Hamilton's functional
129(1)
Some comments on the formulations of transverse vibrations
130(1)
Coupled movements
130(3)
Equations with polar co-ordinates
133(5)
Basic relations
133(2)
Love-Kirchhoff equations of the transverse vibrations of plates
135(3)
Conclusion
138(1)
Vibratory Phenomena Described by the Wave Equation
139(42)
Introduction
139(1)
Wave equation: presentation of the problem and uniqueness of the solution
140(5)
The wave equation
140(2)
Equation of energy and uniqueness of the solution
142(3)
Resolution of the wave equation by the method of propagation (d'Alembert's methodology)
145(9)
General solution of the wave equation
145(2)
Taking initial conditions into account
147(4)
Taking into account boundary conditions: image source
151(3)
Resolution of the wave equation by separation of variables
154(14)
General solution of the wave equation in the form of separate variables
154(3)
Taking boundary conditions into account
157(6)
Taking initial conditions into account
163(2)
Orthogonality of mode shapes
165(3)
Applications
168(10)
Longitudinal vibrations of a clamped-free beam
168(4)
Torsion vibrations of a line of shafts with a reducer
172(6)
Conclusion
178(3)
Free Bending Vibration of Beams
181(48)
Introduction
181(1)
The problem
182(2)
Solution of the equation of the homogenous beam with a constant cross-section
184(5)
Solution
184(2)
Interpretation of the vibratory solution, traveling waves, vanishing waves
186(3)
Propagation in infinite beams
189(8)
Introduction
189(2)
Propagation of a group of waves
191(6)
Introduction of boundary conditions: vibration modes
197(13)
Introduction
197(1)
The case of the supported-supported beam
197(4)
The case of the supported-clamped beam
201(5)
The free-free beam
206(3)
Summary table
209(1)
Stress-displacement connection
210(1)
Influence of secondary effects
211(16)
Influence of rotational inertia
212(3)
Influence of transverse shearing
215(6)
Taking into account shearing and rotational inertia
221(6)
Conclusion
227(2)
Bending Vibration of Plates
229(50)
Introduction
229(1)
Posing the problem: writing down boundary conditions
230(4)
Solution of the equation of motion by separation of variables
234(5)
Separation of the space and time variables
234(1)
Solution of the equation of motion by separation of space variables
235(2)
Solution of the equation of motion (second method)
237(2)
Vibration modes of plates supported at two opposite edges
239(15)
General case
239(2)
Plate supported at its four edges
241(3)
Physical interpretation of the vibration modes
244(4)
The particular case of square plates
248(3)
Second method of calculation
251(3)
Vibration modes of rectangular plates: approximation by the edge effect method
254(9)
General issues
254(1)
Formulation of the method
255(4)
The plate clamped at its four edges
259(2)
Another type of boundary conditions
261(2)
Approximation of the mode shapes
263(1)
Calculation of the free vibratory response following the application of initial conditions
263(2)
Circular plates
265(12)
Equation of motion and solution by separation of variables
265(7)
Vibration modes of the full circular plate clamped at the edge
272(4)
Modal system of a ring-shaped plate
276(1)
Conclusion
277(2)
Introduction to Damping: Example of the Wave Equation
279(30)
Introduction
279(2)
Wave equation with viscous damping
281(6)
Damping by dissipative boundary conditions
287(10)
Presentation of the problem
287(1)
Solution of the problem
288(6)
Calculation of the vibratory response
294(3)
Viscoelastic beam
297(6)
Properties of orthogonality of damped systems
303(5)
Conclusion
308(1)
Calculation of Forced Vibrations by Modal Expansion
309(46)
Objective of the chapter
309(1)
Stages of the calculation of response by modal decomposition
310(12)
Reference example
310(7)
Overview
317(4)
Taking damping into account
321(1)
Examples of calculation of generalized mass and stiffness
322(2)
Homogenous, isotropic beam in pure bending
322(1)
Isotropic homogenous beam in pure bending with a rotational inertia effect
323(1)
Solution of the modal equation
324(12)
Solution of the modal equation for a harmonic excitation
324(6)
Solution of the modal equation for an impulse excitation
330(2)
Unspecified excitation, solution in frequency domain
332(1)
Unspecified excitation, solution in time domain
333(3)
Example response calculation
336(11)
Response of a bending beam excited by a harmonic force
336(4)
Response of a beam in longitudinal vibration excited by an impulse force (time domain calculation)
340(3)
Response of a beam in longitudinal vibrations subjected to an impulse force (frequency domain calculation)
343(4)
Convergence of modal series
347(6)
Convergence of modal series in the case of harmonic excitations
347(3)
Acceleration of the convergence of modal series of forced harmonic responses
350(3)
Conclusion
353(2)
Calculation of Forced Vibrations by Forced Wave Decomposition
355(32)
Introduction
355(1)
Introduction to the method on the example of a beam in torsion
356(9)
Example: homogenous beam in torsion
356(2)
Forced waves
358(1)
Calculation of the forced response
359(2)
Heterogenous beam
361(2)
Excitation by imposed displacement
363(2)
Resolution of the problems of bending
365(4)
Example of an excitation by force
365(3)
Excitation by torque
368(1)
Damped media (case of the longitudinal vibrations of beams)
369(2)
Example
369(2)
Generalization: distributed excitations and non-harmonic excitations
371(8)
Distributed excitations
371(4)
Non-harmonic excitations
375(2)
Unspecified homogenous mono-dimensional medium
377(2)
Forced vibrations of rectangular plates
379(6)
Conclusion
385(2)
The Rayleigh-Ritz Method based on Reissner's Functional
387(22)
Introduction
387(1)
Variational formulation of the vibrations of bending of beams
388(3)
Generation of functional spaces
391(1)
Approximation of the vibratory response
392(1)
Formulation of the method
392(5)
Application to the vibrations of a clamped-free beam
397(9)
Construction of a polynomial base
397(2)
Modeling with one degree of freedom
399(3)
Model with two degrees of freedom
402(2)
Model with one degree of freedom verifying the displacement and stress boundary conditions
404(2)
Conclusion
406(3)
The Rayleigh-Ritz Method based on Hamilton's Functional
409(26)
Introduction
409(1)
Reference example: bending vibrations of beams
409(6)
Hamilton's variational formulation
409(2)
Formulation of the Rayleigh-Ritz method
411(3)
Application: use of a polynomial base for the clamped-free beam
414(1)
Functional base of the finite elements type: application to longitudinal vibrations of beams
415(5)
Functional base of the modal type: application to plates equipped with heterogenities
420(3)
Elastic boundary conditions
423(3)
Introduction
423(1)
The problem
423(1)
Approximation with two terms
424(2)
Convergence of the Rayleigh-Ritz method
426(6)
Introduction
426(1)
The Rayleigh quotient
426(2)
Introduction to the modal system as an extremum of the Rayleigh quotient
428(3)
Approximation of the normal angular frequencies by the Rayleigh quotient or the Rayleigh-Ritz method
431(1)
Conclusion
432(3)
Bibliography and Further Reading 435(4)
Index 439

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