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E-raamat: Seismic Waves and Rays in Elastic Media

(Department of Earth Sciences, Memorial University of Newfoundland, St. John's, NF, Canada)
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This book seeks to explore seismic phenomena in elastic media and emphasizes the interdependence of mathematical formulation and physical meaning. The purpose of this title - which is intended for senior undergraduate and graduate students as well as scientists interested in quantitative seismology - is to use aspects of continuum mechanics, wave theory and ray theory to describe phenomena resulting from the propagation of waves.



The book is divided into three parts: Elastic continua, Waves and rays, and Variational formulation of rays. In Part I, continuum mechanics are used to describe the material through which seismic waves propagate, and to formulate a system of equations to study the behaviour of such material. In Part II, these equations are used to identify the types of body waves propagating in elastic continua as well as to express their velocities and displacements in terms of the properties of these continua. To solve the equations of motion in anisotropic inhomogeneous continua, the high-frequency approximation is used and establishes the concept of a ray. In Part III, it is shown that in elastic continua a ray is tantamount to a trajectory along which a seismic signal propagates in accordance with the variational principle of stationary travel time.

Arvustused

"The purpose of this title...is to use aspects of continuum mechanics, wave theory, and ray theory to describe phenomena resulting from the propagation of waves." --M.A. Slawinski, FIRST BREAK, Volume 23

I Elastic continua
1(124)
Introduction to Part I
3(4)
Deformations
7(26)
Preliminary remarks
7(1)
Notion of continuum
8(1)
Material and spatial descriptions
9(6)
Fundamental concepts
9(1)
Material time derivative
10(2)
Conditions of linearized theory
12(3)
Strain
15(9)
Derivation of strain tensor
15(4)
Physical meaning of strain tensor
19(5)
Rotation tensor and rotation vector
24(9)
Closing remarks
25(1)
Exercises
25(8)
Forces and balance principles
33(28)
Preliminary remarks
33(1)
Conservation of mass
34(2)
Integral equation
34(2)
Equation of continuity
36(1)
Time derivative of volume integral
36(2)
Stress
38(1)
Stress as description of surface forces
38(1)
Traction
38(1)
Balance of linear momentum
39(1)
Stress tensor
40(7)
Traction on coordinate planes
40(3)
Traction on arbitrary planes
43(4)
Cauchy's equations of motion
47(4)
General formulation
47(2)
Example: Surface-forces formulation
49(2)
Balance of angular momentum
51(3)
Integral equation
52(1)
Symmetry of stress tensor
52(2)
Fundamental equations
54(7)
Closing remarks
56(1)
Exercises
56(5)
Stress-strain equations
61(8)
Preliminary remarks
61(1)
Formulation of stress-strain equations
62(4)
Tensorial form
63(1)
Matrix form
64(2)
Determined system
66(3)
Closing remarks
67(1)
Exercises
68(1)
Strain energy
69(16)
Preliminary remarks
69(1)
Strain-energy function
70(1)
Strain-energy function and elasticity-tensor symmetry
71(3)
Fundamental considerations
71(2)
Stress-strain equations
73(1)
Coordinate transformations
74(1)
Stability conditions
74(2)
Physical justification
74(1)
Mathematical formulation
75(1)
Constraints on elasticity parameters
75(1)
System of equations for elastic continua
76(9)
Elastic continua
76(1)
Governing equations
77(2)
Closing remarks
79(1)
Exercises
80(5)
Material symmetry
85(40)
Preliminary remarks
85(1)
Orthogonal transformations
86(1)
Transformation matrix
86(1)
Symmetry group
86(1)
Transformation of coordinates
87(5)
Transformation of stress-tensor components
87(3)
Transformation of strain-tensor components
90(1)
Stress-strain equations in transformed coordinates
91(1)
Condition for material symmetry
92(2)
Point symmetry
94(1)
Generally anisotropic continuum
94(1)
Monoclinic continuum
95(3)
Elasticity matrix
95(1)
Natural coordinate system
96(2)
Orthotropic continuum
98(2)
Tetragonal continuum
100(1)
Transversely isotropic continuum
101(5)
Elasticity matrix
101(1)
Rotation invariance
102(4)
Isotropic continuum
106(19)
Elasticity matrix
106(1)
Lame's parameters
107(1)
Tensorial formulation
108(1)
Physical meaning of Lame's parameters
109(1)
Closing remarks
110(1)
Exercises
111(14)
II Waves and rays
125(140)
Introduction to Part II
127(2)
Equations of motion: Isotropic homogeneous continua
129(34)
Preliminary remarks
129(1)
Wave equations
130(4)
Equation of motion
130(2)
Wave equation for P waves
132(1)
Wave equation for S waves
133(1)
Plane waves
134(3)
Displacement potentials
137(4)
Helmholtz's decomposition
137(1)
Equation of motion
138(1)
P and S waves
139(2)
Solutions of one-dimensional wave equation
141(3)
Reduced wave equation
144(1)
Extensions of wave equation
145(18)
Standard wave equation
146(1)
Wave equation and elliptical velocity dependence
146(3)
Wave equation and weak inhomogeneity
149(5)
Closing remarks
154(1)
Exercises
155(8)
Equations of motion: Anisotropic inhomogeneous continua
163(10)
Preliminary remarks
163(1)
Formulation of equations
164(1)
Formulation of solutions
165(2)
Eikonal equation
167(6)
Closing remarks
170(1)
Exercises
170(3)
Hamilton's ray equations
173(24)
Preliminary remarks
173(1)
Method of characteristics
174(5)
Level-set functions
174(1)
Characteristic equations
175(3)
Consistency of formulation
178(1)
Time parametrization of characteristic equations
179(4)
General formulation
179(1)
Equations with variable scaling factor
180(1)
Equations with constant scaling factor
181(1)
Formulation of Hamilton's ray equations
182(1)
Example: Ray equations in isotropic inhomogeneous continua
183(14)
Parametric form
183(1)
Explicit form
184(1)
Closing remarks
185(1)
Exercises
186(11)
Lagrange's ray equations
197(20)
Preliminary remarks
197(1)
Transformation of Hamilton's ray equations
198(3)
Formulation of Lagrange's ray equations
198(2)
Beltrami's identity
200(1)
Relation between p and x
201(16)
Phase and ray velocities
201(3)
Phase and ray angles
204(2)
Geometrical illustration
206(1)
Closing remarks
206(1)
Exercises
207(10)
Christoffel's equations
217(28)
Preliminary remarks
217(1)
Explicit form of Christoffel's equations
218(3)
Christoffel's equations and anisotropic continua
221(11)
Monoclinic continua
222(4)
Transversely isotropic continua
226(6)
Phase-slowness surfaces
232(13)
Convexity of innermost sheet
233(1)
Intersection points
233(2)
Closing remarks
235(1)
Exercises
236(9)
Reflection and transmission
245(20)
Preliminary remarks
245(1)
Angles at interface
246(5)
Phase angles
246(1)
Ray angles
247(1)
Example: Elliptical velocity dependence
248(3)
Amplitudes at interface
251(14)
Kinematic and dynamic boundary conditions
251(4)
Reflection and transmission amplitudes
255(4)
Closing remarks
259(1)
Exercises
260(5)
III Variational formulation of rays
265(72)
Introduction to Part III
267(2)
Euler's equations
269(24)
Preliminary remarks
269(1)
Mathematical background
270(1)
Formulation of Euler's equation
271(3)
Beltrami's identity
274(1)
Generalizations of Euler's equation
274(3)
Case of several variables
274(1)
Case of several functions
275(1)
Higher-order derivatives
276(1)
Special cases of Euler's equation
277(5)
Independence of z
277(1)
Independence of x and z
277(1)
Independence of x
278(1)
Total derivative
279(1)
Function of x and z
279(3)
First integrals
282(1)
Lagrange's ray equations as Euler's equations
283(10)
Closing remarks
284(1)
Exercises
284(9)
Fermat's principle
293(26)
Preliminary remarks
293(1)
Formulation of Fermat's principle
294(7)
Statement of Fermat's principle
294(1)
Properties of Hamiltonian H
294(2)
Variational equivalent of Hamilton's ray equations
296(1)
Properties of Lagrangian L
296(2)
Parameter-independent Lagrange's ray equations
298(1)
Ray velocity
299(1)
Proof of Fermat's principle
300(1)
Illustration of Hamilton's principle
301(18)
Action
301(2)
Lagrange's equations of motion
303(1)
Wave equation
304(4)
Closing remarks
308(1)
Exercises
308(11)
Ray parameters
319(18)
Preliminary remarks
319(1)
Traveltime integrals
320(1)
Ray parameters as first integrals
320(2)
Example: Ellipticity and linearity
322(6)
Rays
323(3)
Traveltimes
326(1)
Isotropic extension
327(1)
Rays in isotropic continua
328(1)
Lagrange's ray equations in xz-plane
329(2)
Conserved quantities and Hamilton's ray equations
331(6)
Closing remarks
332(1)
Exercises
332(5)
IV Appendices
337(4)
Introduction to Part IV
339(2)
A Euler's homogeneous-function theorem
341(6)
Preliminary remarks
341(1)
A.1 Homogeneous functions
342(1)
A.2 Homogeneous-function theorem
343(4)
Closing remarks
345(2)
B Legendre's transformation
347(8)
Preliminary remarks
347(1)
B.1 Geometrical context
348(2)
B.1.1 Surface and its tangent planes
348(1)
B.1.2 Single-variable case
348(2)
B.2 Duality of transformation
350(1)
B.3 Transformation between L and H
350(2)
B.4 Transformation and ray equations
352(3)
Closing remarks
353(2)
C List of symbols
355(4)
C.1 Mathematical relations and operations
355(2)
C.2 Physical quantities
357(2)
C.2.1 Greek letters
357(1)
C.2.2 Roman letters
358(1)
Bibliography 359(15)
Index 374(27)
About the author 401


http://www.rug.nl/rechten/faculteit/vakgroepen/beof/ecof/mdw/WoerdmanE