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准晶数学的弹性理论及应用

准晶数学的弹性理论及应用

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  • ISBN:9787030256690
  • 装帧:暂无
  • 册数:暂无
  • 重量:暂无
  • 开本:16开
  • 页数:暂无
  • 出版时间:2010-10-01
  • 条形码:9787030256690 ; 978-7-03-025669-0

本书特色

《准晶数学的弹性理论及应用(英文版)》:The dynamic and non-linear analysis of deformation and fracture of quasicrystals in this volume presents an innovative approach. It gives a clear-cut, strict and systematic mathematical overview of the field. Comprehensive and detailed mathematical derivations guide readers through the work. By combining mathematical calculations and experimental data, theoretical analysis and practical applications, and analytical and numerical studies, readers will gain systematic, comprehensive and in-depth knowledge on continuum mechanics, condensed matter physics and applied mathematics.

目录

PrefaceChapter1 Crystals1.1 Periodicity of crystal structure, crystal cell1.2 Three-dimensional lattice types1.3 Symmetry and point groups1.4 Reciprocal lattice1.5 Appendix of Chapter1: Some basic conceptsReferencesChapter 2 Framework of the classical theory of elasticity2.1 Review on some basic concepts2.2 Basic assumptions of theory of elasticity2.3 Displacement and deformation2.4 Stress analysis and equations of motion2.5 Generalized Hooke's law2.6 Elastodynamics, wave motion2.7 SummaryReferencesChapter 3 Quasicrystal and its properties3.1 Discovery of quasicrystal3.2 Structure and symmetry of quasicrystals3.3 A brief introduction on physical properties of quasicrystals3.4 One-, two- and three-dimensional quasicrystals3.5 Two-dimensional quasicrystals and planar quasicrystalsReferencesChapter 4 The physical basis of elasticity of quasicrystals4.1 Physical basis of elasticity of quasicrystals4.2 Deformation tensors4.3 Stress tensors and the equations of motion4.4 Free energy and elastic constants4.5 Generalized Hooke's law4.6 Boundary conditions and initial conditions4.7 A brief introduction on relevant material constants of quasicrystals4.8 Summary and mathematical solvability of boundary value or initial- boundary value problem4.9 Appendix of Chapter 4: Description on physical basis of elasticity of quasicrystals based on the Landau density wave theoryReferencesChapter 5 Elasticity theory of one-dimensional quasicrystals and simplification5.1 Elasticity of hexagonal quasicrystals5.2 Decomposition of the problem into plane and anti-plane problems5.3 Elasticity of monoclinic quasicrystals5.4 Elasticity of orthorhombic quasicrystals5.5 Tetragonal quasicrystals5.6 The space elasticity of hexagonal quasicrystals5.7 Other results of elasticity of one-dimensional quasicrystalsReferencesChapter 6 Elasticity of two-dimensional quasicrystals and simplification6.1 Basic equations of plane elasticity of two-dimensional quasicrystals: point groups 5m and10mm in five- and ten-fold symmetries6.2 Simplification of the basic equation set: displacement potential function method6.3 Simplification of the basic equations set: stress potential function method6.4 Plane elasticity of point group 5, pentagonal and point group10, decagonal quasicrystals6.5 Plane elasticity of point group12mm of dodecagonal quasicrystals6.6 Plane elasticity of point group 8mm of octagonal quasicrystals, displacement potential6.7 Stress potential of point group 5, pentagonal and point group10, decagonal quasicrystals6.8 Stress potential of point group 8mm octagonal quasicrystals6.9 Engineering and mathematical elasticity of quasicrystalsReferencesChapter 7 Application I: Some dislocation and interface problems and solutions in one- and two,dimensional quasicrystals7.1 Dislocations in one-dimensional hexagonal quasicrystals7.2 Dislocations in quasicrystals with point groups 5m and10mm symmetries7.3 Dislocations in quasicrystals with point groups 5, five-fold and10, ten-fold symmetries7.4 Dislocations in quasicrystals with eight-fold symmetry7.5 Dislocations in dodecagonal quasicrystals7.6 Interface between quasicrystal and crystal7.7 Conclusion and discussionReferencesChapter 8 Application II: Solutions of notch and crack problems of one-and two-dimensional quasicrystals8.1 Crack problem and solution of one-dimensional quasicrystals8.2 Crack problem in finite-sized one-dimensional quasicrystals8.3 Griffith crack problems in point groups 5m and10mm quasicrystals based on displacement potential function method8.4 Stress potential function formulation and complex variable function method for solving notch and crack problems of quasicrystals of point groups 5, and10, 8.5 Solutions of crack/notch problems of two-dimensional octagonal quasicrystals8.6 Other solutions of crack problems in one-and two-dimensional quasicrystals8.7 Appendix of Chapter 8: Derivation of solution of Section 8.1ReferencesChapter 9 Theory of elasticity of three-dimensional quasicrystals and its a
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《准晶数学的弹性理论及应用(英文版)》内容简介:This inter-disciplinary work covering the continuum mechanics of novel materials, condensed matter phyics and partial differential equations discusses the mathematical theory of elasticity of quasicrystals (a new condensed matter) and its applications by setting up new partial differential equations of higher order and their solutions under complicated boundary value and initial value conditions. The new theories developed here dramatically simplify the solving of complicated elasticity equation systems. Large numbers of complicated equations involving elasticity are reduced to a single or a few partial differential equations of higher order. Systematical and direct methods of mathematical physics and complex variable functions are developed to solve the equations under appropriate boundary value and initial value conditions, and many exact analytical solutions are constructed.

相关资料

插图:In general, the course of crystallography does not contain the contents given in this section. Because the discussion here is dependent on quasicrystals, especially with the elasticity of quasicrystals, we have to introduce some of the simplest relevant arguments.In 1900, Planck put forward the quantum theory. Soon after Einstein developed the theory and explained the photo-electric effect, which leads to the photon concept. Einstein also studied the specific heat c~ of crystals by using the Planck quantum theory. There are some unsatisfactory points in the work of Einstein although his formula explained the phenomenon of c~ = 0 at T = 0, where T denotes the absolute temperature. To improve Einstein's work, Debye[3] and Born et al. [4,5] applied the quantum theory to study the specific heat arising from lattice vibration in 1912 and 1913 respectively, and got a great success. The theoretical prediction is in excellent agreement to the experimental results, at least for the atom crystals. The propagation of the lattice vibration is called the lattice wave. Under thelong-wavelength approximation, the lattice vibration can be seen as continuum elastic vibration, i.e., the lattice wave can be approximately seen as the continuum elastic wave. The motion is a mechanical motion, but Debye and Born assumed that the energy can be quantized based on Planck's hypothesis. With the elastic wave approximation and quantization, Debye and Born successfully explained the specific heat of crystals at low temperature, and the theoretical prediction is consistent with the experimental results in all range of temperature, at least for the atomic crystals. The quanta of the elastic vibration, or the smallest unit of energy of the elastic wave is named phonon, because the elastic wave is one of acoustic waves. Unlike photon, the phonon is not an elementary particle, but in the sense of quantization, the phonon presents natural similarity to that of photon and other elementary particles, thus can be named quasi-particle. The concept created by Debye and Born opened the study on lattice dynamics, an important branch of solid state physics. Yet according to the view point at present, the Debye and Born theory on solid belongs to a phenomenological theory, though they used the classical quantum theory.

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