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