Physical Properties of Crystals: Their Representation by Tensors and Matrices |
From inside the book
Results 1-3 of 66
Page vi
... Chapters I to X ) , Professor K. Lonsdale , F.R.S. ( for reading the first drafts of Chapters I , II , III , VIII and IX ) , and Sir Edward Bullard , F.R.S. Dr. D. Polder has helped me with Chapter XII and Dr. F. G. Fumi with Chapter ...
... Chapters I to X ) , Professor K. Lonsdale , F.R.S. ( for reading the first drafts of Chapters I , II , III , VIII and IX ) , and Sir Edward Bullard , F.R.S. Dr. D. Polder has helped me with Chapter XII and Dr. F. G. Fumi with Chapter ...
Page xiv
... Chapter I introduces the concept of a tensor and shows how tensors of zero , first and second rank may be used for studying crystal properties . Chapter II continues the mathematical development . In Chapters III to VI the tensor method ...
... Chapter I introduces the concept of a tensor and shows how tensors of zero , first and second rank may be used for studying crystal properties . Chapter II continues the mathematical development . In Chapters III to VI the tensor method ...
Page xv
... Chapter I. Chapter III . Chapter IV . Chapter V. The stress tensor Chapter VI . The strain tensor and thermal expansion Chapter VII . Piezoelectricity . Third - rank tensors Chapter VIII . Elasticity . Fourth - rank tensors Chapter XI ...
... Chapter I. Chapter III . Chapter IV . Chapter V. The stress tensor Chapter VI . The strain tensor and thermal expansion Chapter VII . Piezoelectricity . Third - rank tensors Chapter VIII . Elasticity . Fourth - rank tensors Chapter XI ...
Contents
THE GROUNDWORK OF CRYSTAL PHYSICS | 3 |
3 | 29 |
EQUILIBRIUM PROPERTIES | 51 |
23 other sections not shown
Common terms and phrases
angle anisotropic applied axial B₁ biaxial birefringence centre of symmetry Chapter coefficients components conductivity constant crystal classes crystal properties crystal symmetry cube cubic crystals D₁ defined denoted diad axis dielectric dijk direction cosines displacement electric field ellipsoid equal equation example expression follows forces given grad H₁ H₂ heat flow Hence hexagonal indicatrix isothermal isotropic k₁ magnetic magnitude matrix notation measured moduli monoclinic number of independent Onsager's Principle optic axis optical activity orientation orthorhombic Ox₁ P₁ parallel Peltier permittivity perpendicular photoelastic photoelastic effect piezoelectric effect plane plate polarization positive principal axes produced pyroelectric effect quadric radius vector referred refractive index relation representation quadric represents right-handed rotation S₁ scalar second-rank tensor shear shown strain stress symmetry elements Table temperature gradient thermal expansion thermodynamics thermoelectric effects Thomson heat tion transformation law triclinic trigonal uniaxial values wave normal x₁ zero әт