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 x = 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 x = tan - 1 ( a / b ) ...
Page 166
... axis has components 2πNI B2- B2 = " NI ( ) 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 ...
... axis has components 2πNI B2- B2 = " NI ( ) 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 ...
Page 422
... axis 2 2 2 v112 + v ̧2 = vo2 ( 12.126 ) where vo2 2 = V102 + 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 2 = U10 B Во 2 ( 12.127 ) where B ...
... axis 2 2 2 v112 + v ̧2 = vo2 ( 12.126 ) where vo2 2 = V102 + 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 2 = U10 B Во 2 ( 12.127 ) where B ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ