Movement Equations 4 - Michel Borel - E-Book

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Michel Borel

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Beschreibung

An important instance of the application of unbuckled solid mechanics is that of its stability and small movements from this situation. The problem expressing goes through the linearization of the movement equations set up in the 3rd volume of this treaty, by their limited development. This book gives and develops the process which leads to the differential linear equations expressing this kind of movement and allowing the study of the equilibrium and the stability of an unbuckled solid.

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Veröffentlichungsjahr: 2018

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Table of Contents

Cover

Title

Copyright

Introduction

Table of Notations

1 Equilibrium, Stationary Movement and Oscillation of a Free Solid

1.1. Expression of the fundamental principle of dynamics for a free solid

1.2. Canonical form of the fundamental principle

1.3. Equilibrium of the free solid

1.4. General equations of small movements of a free solid

1.5. Matrix expression of small movements of a free solid

1.6. Stationary movement

2 Solving Equations of Small Movements

2.1. Linear differential systems with constant coefficients

2.2. Laplace transformation

3 Oscillator Studies

3.1. Physical nature of oscillatory motion

3.2. The single oscillator

3.3. Motion of coupled oscillators

3.4. Oscillatory device of

k

oscillators – equilibrium and stability

4 Gyroscopic Motion

4.1. Gyroscopic coupling

4.2. Gyroscopic pendulum

4.3. The gyro-compass

4.4. Applications: problem 7 – motion stabilizer

Bibliography

Index

End User License Agreement

List of Illustrations

1 Equilibrium, Stationary Movement and Oscillation of a Free Solid

Figure 1.1. Configuration of the oscillator

Figure 1.2. Configuration of the oscillatory device

Figure 1.3. Triangular plate

Figure 1.4. Configuration of the studied device

Figure 1.5. Layout of the rhomb

Figure 1.6. Relative position of the bases

2 Solving Equations of Small Movements

Figure 2.1. “Heaviside” function

Figure 2.2. “Step” function

3 Oscillator Studies

Figure 3.1. Oscillatory critical aperiodic motion – Case 1

Figure 3.2. Extremal values of t

e

Figure 3.3. Critical aperiodic function – solutions

Figure 3.4. Pseudo-periodic motion

Figure 3.5. Variation of the phase advance

Figure 3.6. Variation of the amplification factor

Figure 3.7. Graph of a modulated oscillatory signal

Figure 3.8. Diagram of the device

Figure 3.9. Position of the roots in the complex plane

Figure 3.10. Principle of the pivot method

4 Gyroscopic Motion

Figure 4.1. Principle of the coupling gyroscopic device

Figure 4.2. Position of the roots of characteristic a equation

Figure 4.3. Stability area of the gyroscopic pendulum

Figure 4.4. Unstable situation of equilibrium of the device

Figure 4.5. General framing of motion

Figure 4.6. Tables of relative positions of different bases

Landmarks

Cover

Table of Contents

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Non-deformable Solid Mechanics Setcoordinated byAbdelkhalak El Hami

Volume 4

Movement Equations 4

Equilibriums and Small Movements

Michel Borel

Georges Vénizélos

First published 2018 in Great Britain and the United States by ISTE Ltd and John Wiley & Sons, Inc.

Apart from any fair dealing for the purposes of research or private study, or criticism or review, as permitted under the Copyright, Designs and Patents Act 1988, this publication may only be reproduced, stored or transmitted, in any form or by any means, with the prior permission in writing of the publishers, or in the case of reprographic reproduction in accordance with the terms and licenses issued by the CLA. Enquiries concerning reproduction outside these terms should be sent to the publishers at the undermentioned address:

ISTE Ltd27-37 St George’s RoadLondon SW19 4EUUK

www.iste.co.uk

John Wiley & Sons, Inc.111 River StreetHoboken, NJ 07030USA

www.wiley.com

© ISTE Ltd 2018The rights of Michel Borel and Georges Vénizélos to be identified as the authors of this work have been asserted by them in accordance with the Copyright, Designs and Patents Act 1988.

Library of Congress Control Number: 2017962758

British Library Cataloguing-in-Publication DataA CIP record for this book is available from the British LibraryISBN 978-1-78630-035-5

Introduction

This fourth volume in the “Movement Equations” series is positioned in line with the third entry in that it applies the principles established in the third volume, such as the fundamental principle of dynamics as applied to the motion of non-deformable solids, and its various scalar consequences that lead to the movement equations.

During their motion through space, the bodies can encounter situations of equilibrium, static or can be under the form of uniform movements said to be stationary, the stability of which, meaning the ability to maintain itself, must be assessed if the bodies are subject to stresses that tend to move them away from this equilibrium. These stresses induce small movements that can either, after oscillations, bring the body back to its initial state of equilibrium, or amplify and break it. Furthermore, the combination of oscillatory components in a same device can, through the coupling of their respective behaviors, lead to stabilized and stabilizer systems such as the gyroscope.

This volume includes four chapters. Chapter 1, which states the problem, begins with the scalar consequences of the fundamental principle, identifies the conceivable situations of equilibrium, their conditions for acquisition and the values of the situation parameters that correspond to them. It then examines the consequences of infinitesimal variations of the parameters around the values of equilibrium we previously identified and deduces the equations that express the resulting movements. These small movements show the behavior of the mechanical device thus disturbed and give useful indications on its stability.

Chapter 2 is, in a way, a mathematical insert in the book. Studying the behavior of an oscillator requires solving the equations of small movements established in Chapter 1. These are second-order linear differential equations, with constant coefficients that possess an infinite number of solutions; because the motion we want to study is presumably oscillatory in nature, we are looking for solutions of which the form is compatible with this objective, either starting from the vector expression of the differential system to be solved, or by using the Laplace transformation.

Chapter 3 focuses on the study of oscillators. We start with the individual oscillator, the motion of which highlights the different modes of oscillation and the stability of such a device. We then focus on oscillator coupling that demonstrates the reciprocal influence of different mobile components of a system within which they are coupled and their role in the stability of the set. But, in this case, the study of the stability requires processing transfer functions that have no place in this title. However, to illustrate their use, the chapter presents, for example, the use of the Routh criteria, which are used to study the stability of dynamic systems in engineering and electronics, without giving theoretical validation.

Since the gyroscope is a device whose components are coupled, allowing it to display various stabilizer effects in a variety of applications, we dedicate Chapter 4 to it. After expanding on the principle of gyroscopic coupling, the study moves to its use in the case of the gyroscopic pendulum, used in particular for controlling satellites, and the gyro-compass as a navigational instrument that helps maintain true North. The presented problem demonstrates the use of a gyroscope on the swell of a ship.

The “Movement Equations” series will end with a fifth volume, through the study of sets of solids and with an introduction to robotics. The authors will thus have offered the readers a broad panorama on this subject of movement equations, which are at the core of the study of the motion of non-deformable solids, and the use of which is still current in the field of space, even though it is obvious that the ones used are clearly more complex. But the ground work is the same.