Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 89
Page 16
... inside a volume V subject to either Dirichlet or Neumann boundary conditions on the closed bounding surface S. We suppose , to the contrary , that there exist two solutions 1 and P , satisfying the same boundary conditions . Let = U ...
... inside a volume V subject to either Dirichlet or Neumann boundary conditions on the closed bounding surface S. We suppose , to the contrary , that there exist two solutions 1 and P , satisfying the same boundary conditions . Let = U ...
Page 97
... inside a grounded cylindrical box defined by the surfaces z = 0 , z L , p = a . Show that the = potential inside the box can be expressed in the following alternative forms : XmnP ∞ etm ( - ) J , XmnP m m Þ ( x , x ' ) = a Σ Σ a a xmnL ...
... inside a grounded cylindrical box defined by the surfaces z = 0 , z L , p = a . Show that the = potential inside the box can be expressed in the following alternative forms : XmnP ∞ etm ( - ) J , XmnP m m Þ ( x , x ' ) = a Σ Σ a a xmnL ...
Page 236
... inside the conductors . The charges inside a perfect conductor are assumed to be so mobile that they move instantly in response to changes in the fields , no matter how rapid , and always produce the correct surface - charge density Σ ...
... inside the conductors . The charges inside a perfect conductor are assumed to be so mobile that they move instantly in response to changes in the fields , no matter how rapid , and always produce the correct surface - charge density Σ ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
21 other sections not shown
Other editions - View all
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ