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Page xii
... coordinates , 47 . References and suggested reading , 50 . Problems , 51 . chapter 3. Boundary - Value Problems in Electrostatics , II 3.1 Laplace's equation in spherical coordinates , 54 . 3.2 Legendre polynomials , 56 . 3.3 Boundary ...
... coordinates , 47 . References and suggested reading , 50 . Problems , 51 . chapter 3. Boundary - Value Problems in Electrostatics , II 3.1 Laplace's equation in spherical coordinates , 54 . 3.2 Legendre polynomials , 56 . 3.3 Boundary ...
Page 381
... coordinates x1 = b , xq ' = 0 , xg ' = -vt ' , and is a distance r ' = √b2 + ( vt ' ) 2 away from q . We will need to express r ' in terms of the coordinates of K. The only coordinate needing transformation is the time t ' = y [ t — y ...
... coordinates x1 = b , xq ' = 0 , xg ' = -vt ' , and is a distance r ' = √b2 + ( vt ' ) 2 away from q . We will need to express r ' in terms of the coordinates of K. The only coordinate needing transformation is the time t ' = y [ t — y ...
Page 632
... coordinates , 376 in transforming delta functions , 79 Kinematics , relativistic , 394 f . Kirchhoff diffraction ... coordinates , 76 , 77 general solution of , in spherical co- ordinates , 67 in cylindrical coordinates , 69 in ...
... coordinates , 376 in transforming delta functions , 79 Kinematics , relativistic , 394 f . Kirchhoff diffraction ... coordinates , 76 , 77 general solution of , in spherical co- ordinates , 67 in cylindrical coordinates , 69 in ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ