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 P ( z = = r ) = - ( r2 + c2 2cr cos x ) ( 3.45 ) where c2 = a2 + b2 and α = 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 P ( z = = r ) = - ( r2 + c2 2cr cos x ) ( 3.45 ) where c2 = a2 + b2 and α = tan - 1 ( a / b ) ...
Page 165
... axis and near the center of the solenoid the magnetic induction is mainly parallel to the axis , but has a small radial component B 96π NI ( a2zp с LA correct to order a2 / L2 , and for z « L , p < a . The coordinate z is measured from ...
... axis and near the center of the solenoid the magnetic induction is mainly parallel to the axis , but has a small radial component B 96π NI ( a2zp с LA correct to order a2 / L2 , and for z « L , p < a . The coordinate z is measured from ...
Page 166
... axis has components 2πNI ΠΝΙ Bz B. ~ с с a 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 throughout ...
... axis has components 2πNI ΠΝΙ Bz B. ~ с с a 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 throughout ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ