Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 87
Page 2
... Electric Field Although the thing that eventually gets measured is a force , it is useful to introduce a concept one step removed from the forces , the concept of an electric field due to some array of charged bodies . At the moment ...
... Electric Field Although the thing that eventually gets measured is a force , it is useful to introduce a concept one step removed from the forces , the concept of an electric field due to some array of charged bodies . At the moment ...
Page 298
... fields will be the same as if the hole were not there , namely , normal E , and tangential Bo . The electric field lines might appear as shown in Fig . 9.12 . Since the departures of the fields E and B from their unperturbed values E ...
... fields will be the same as if the hole were not there , namely , normal E , and tangential Bo . The electric field lines might appear as shown in Fig . 9.12 . Since the departures of the fields E and B from their unperturbed values E ...
Page 614
... electric field is dimensionally different from force per unit charge , There is , however , nothing to be gained by this extra freedom in the definition of E , since E is the first derived field quantity to be defined . Only when we ...
... electric field is dimensionally different from force per unit charge , There is , however , nothing to be gained by this extra freedom in the definition of E , since E is the first derived field quantity to be defined . Only when we ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
18 other sections not shown
Other editions - View all
Common terms and phrases
4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ