Introduction to Solid State Physicsproblems after each chapter |
From inside the book
Results 1-3 of 81
Page 159
The constant N is known as the depolarization factor ; it is precisely the same as
the demagnetization factor , and its value depends on the axial 1.0 0.8 0.6 N / 40
0.4 0.2 0 5 cla Fig . 7.2 . Demagnetization factor N parallel to the figure axis of ...
The constant N is known as the depolarization factor ; it is precisely the same as
the demagnetization factor , and its value depends on the axial 1.0 0.8 0.6 N / 40
0.4 0.2 0 5 cla Fig . 7.2 . Demagnetization factor N parallel to the figure axis of ...
Page 237
We expect the charge transported to be proportional to the charge density Ne ;
the factor e / m enters because the acceleration in a given electric field is
proportional to e and inversely proportional to the mass m ; the time t describes
the free ...
We expect the charge transported to be proportional to the charge density Ne ;
the factor e / m enters because the acceleration in a given electric field is
proportional to e and inversely proportional to the mass m ; the time t describes
the free ...
Page 359
In writing ( 13.26 ) we have omitted in the interest of simplicity a factor of which
often is seen in front of the exponential . The factor arises when one takes into
account the fact that the energy of a spindegenerate donor level occupied by two
...
In writing ( 13.26 ) we have omitted in the interest of simplicity a factor of which
often is seen in front of the exponential . The factor arises when one takes into
account the fact that the energy of a spindegenerate donor level occupied by two
...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
DIFFRACTION OF XRAYS BY CRYSTALS | 44 |
CLASSIFICATION OF SOLIDS LATTICE ENERGY | 63 |
ELASTIC CONSTANTS OF CRYSTALS | 85 |
Copyright | |
17 other sections not shown
Other editions - View all
Common terms and phrases
alloys applied approximately associated atoms axis band boundary calculated cell chapter charge concentration condition conductivity consider constant crystal cubic density dependence determined dielectric diffusion direction discussion dislocation distribution domain effect elastic electric electron elements energy equal equation equilibrium experimental expression factor field force frequency function germanium give given heat capacity hexagonal holes important impurity increase interaction ionic ions lattice levels London magnetic magnetic field mass material measurements metals method motion normal observed obtained parallel particles Phys physics plane polarization positive possible potential problem properties range reference reflection region relation resistivity result room temperature rotation shown in Fig simple solid solution space space group specimen structure surface symmetry Table temperature theory thermal tion transition unit usually values vector volume wave zero zone