Classical ElectrodynamicsProblems after each chapter |
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Page 63
... axis the z axis and its center at z = b . The potential at a point P on the axis of symmetry with z = r is just q divided by the distance AP : q D ( z = r ) = ( r2 + c2 - 2cr cos α ) ( 3.45 ) where c2 = a2 + b2 and ∞ = tan - 1 ( a / b ) ...
... axis the z axis and its center at z = b . The potential at a point P on the axis of symmetry with z = r is just q divided by the distance AP : q D ( z = r ) = ( r2 + c2 - 2cr cos α ) ( 3.45 ) where c2 = a2 + b2 and ∞ = tan - 1 ( a / b ) ...
Page 166
... axis has components 2πNI ΠΝΙ B2 B. ~ с NI ( 6 ) с 5.3 A cylindrical conductor of radius a has a hole of radius b bored parallel to , and centered a distance d from , the cylinder axis ( d + b < a ) . The current density is uniform ...
... axis has components 2πNI ΠΝΙ B2 B. ~ с NI ( 6 ) с 5.3 A cylindrical conductor of radius a has a hole of radius b bored parallel to , and centered a distance d from , the cylinder axis ( d + b < a ) . The current density is uniform ...
Page 422
... axis 110 2 2 2 v12 + v ̧2 = v122 102 ( 12.126 ) where vo2 = √102 + V1 2 is the square of the speed at z = 0. If we assume that the flux linked is a constant of the motion , then ( 12.125 ) allows us to write 110 2 vi B = 1102 Во ...
... axis 110 2 2 2 v12 + v ̧2 = v122 102 ( 12.126 ) where vo2 = √102 + V1 2 is the square of the speed at z = 0. If we assume that the flux linked is a constant of the motion , then ( 12.125 ) allows us to write 110 2 vi B = 1102 Во ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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