Introduction to Solid State Physics |
From inside the book
Results 1-3 of 47
Page 77
5 310 Be 1000 Li 328 - 430 235 C ( diamond ) 1860 290 NaCl 281 Mo 379 KCI
230 160 KBr 177 485 Ne CaF , 474 315 370 FeS2 630 DIATOMIC LATTICE One
can obtain an exact expression for the heat capacity of a diatomic lattice in one ...
5 310 Be 1000 Li 328 - 430 235 C ( diamond ) 1860 290 NaCl 281 Mo 379 KCI
230 160 KBr 177 485 Ne CaF , 474 315 370 FeS2 630 DIATOMIC LATTICE One
can obtain an exact expression for the heat capacity of a diatomic lattice in one ...
Page 232
In metals the values of T , are of the order of 104 to 106 °K , so that electronic
contributions to the heat capacity at room temperature of the order of 10 – 2R are
anticipated . At low temperatures the total heat capacity of a metal consists of the
...
In metals the values of T , are of the order of 104 to 106 °K , so that electronic
contributions to the heat capacity at room temperature of the order of 10 – 2R are
anticipated . At low temperatures the total heat capacity of a metal consists of the
...
Page 303
ELEMENTARY THEORY OF ORDER We give now a simple statistical treatment
of the dependence of order on temperature for the case of an AB alloy with a bcc
structure . 8 . 32 0 . 26 OTTT C = 8 . 32R 7 . 68€ 0 . 24 ) 7 . 04 Specific heat ( units
...
ELEMENTARY THEORY OF ORDER We give now a simple statistical treatment
of the dependence of order on temperature for the case of an AB alloy with a bcc
structure . 8 . 32 0 . 26 OTTT C = 8 . 32R 7 . 68€ 0 . 24 ) 7 . 04 Specific heat ( units
...
What people are saying - Write a review
We haven't found any reviews in the usual places.
Contents
LATTICE ENERGY OF IONIC CRYSTALS | 29 |
ELASTIC CONSTANTS OF CRYSTALS | 43 |
LATTICE VIBRATIONS | 60 |
Copyright | |
13 other sections not shown
Other editions - View all
Common terms and phrases
alloy applied approximation atoms axes axis band boundary calculated cell chapter charge chloride condition conductivity consider constant crystal cubic defined dependence determined dielectric diffusion direction discussed dislocations displacement distance distribution domains effect elastic electric electron energy equal equation equilibrium example excitation experimental expression factor field force frequency function given gives heat holes interaction ionic ions lattice levels London magnetic magnetic field material mean measurements mechanism metals method molecules motion negative neighbor normal observed obtained parallel particles Phys physical plane polarization positive possible potential problem properties quantum range reference reflection region relation resistivity result room temperature scattering Show shown in Fig sodium solids space specimen stress structure suppose Table temperature theory thermal tion transition unit usually vacancy values volume wave zero