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 : Φ ( 2 = r ) q = ― ( r2 + c2 2cr cos x ) ( 3.45 ) where c2 -1 = a2 + b2 and a = tan - 1 ( a ...
... 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 : Φ ( 2 = r ) q = ― ( r2 + c2 2cr cos x ) ( 3.45 ) where c2 -1 = a2 + b2 and a = tan - 1 ( a ...
Page 166
... axis has components πΝΙ 2πNI B B , ~ TNI ( C ) с C 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 < Ia ) . The current density is uniform ...
... axis has components πΝΙ 2πNI B B , ~ TNI ( C ) с C 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 < Ia ) . The current density is uniform ...
Page 422
... axis v . 110 ΠΙΟ v1 2 + v2 2 = vo2 ( 12.126 ) where vo 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 V1 V10 = B Bo ( 12.127 ) ...
... axis v . 110 ΠΙΟ v1 2 + v2 2 = vo2 ( 12.126 ) where vo 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 V1 V10 = B Bo ( 12.127 ) ...
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BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ