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Page 121
space (p, q space) is proportional to the Boltzmann factor exp (-H/kT) (4.79)
where H is the Hamiltonian. In the simple problem of a harmonically bound
electron with an applied field in the z direction, the Hamiltonian is H = + p" + "
odox” — eEz ...
space (p, q space) is proportional to the Boltzmann factor exp (-H/kT) (4.79)
where H is the Hamiltonian. In the simple problem of a harmonically bound
electron with an applied field in the z direction, the Hamiltonian is H = + p" + "
odox” — eEz ...
Page 129
... and determine all the nonvanishing multipole moments. Write down the
potential at large distances as a finite expansion in Legendre polynomials. (b)
Determine the potential explicitly at any point in space, and show that near the
origin r?
... and determine all the nonvanishing multipole moments. Write down the
potential at large distances as a finite expansion in Legendre polynomials. (b)
Determine the potential explicitly at any point in space, and show that near the
origin r?
Page
The other components of f yield similar results, showing that (11.126) can be
written as f = | F.J., k = 1,2,3 (11.128) C The right-hand side of (11.128) is
evidently the space components of a 4-vector. Hence f must be the space part of
a 4-vector f.
The other components of f yield similar results, showing that (11.126) can be
written as f = | F.J., k = 1,2,3 (11.128) C The right-hand side of (11.128) is
evidently the space components of a 4-vector. Hence f must be the space part of
a 4-vector f.
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Contents
Introduction to Electrostatics | 1 |
Nš 3 | 3 |
Greens theorem | 14 |
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