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 $ ( z = r ) = ( r2 + c2 - 2cr cos α ) ( 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 $ ( z = r ) = ( r2 + c2 - 2cr cos α ) ( 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 Вр 96π NI ( a2zp с LA L correct to order a2 / L2 , and for z « L , p « a . The coordinate z is measured ...
... axis and near the center of the solenoid the magnetic induction is mainly parallel to the axis , but has a small radial component B Вр 96π NI ( a2zp с LA L correct to order a2 / L2 , and for z « L , p « a . The coordinate z is measured ...
Page 166
... axis has components B2 2πNI с B , 2 ΠΝΙ 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 B2 2πNI с B , 2 ΠΝΙ 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 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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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