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Page 63
... axis it is only necessary , according to ( 3.33 ) and ( 3.38 ) , to multiply each term in ( 3.44 ) by P ( cos y ) ... 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 ...
... axis it is only necessary , according to ( 3.33 ) and ( 3.38 ) , to multiply each term in ( 3.44 ) by P ( cos y ) ... 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 ...
Page 166
... axis has components 2πNI πΝΙ B2 ~ 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 B2 ~ 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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... axis 110 .ע 2 || v1 2 + v 2 = v02 where vo2 2 = 2 V10 2 + V1 2 is the 110 ( 12.126 ) 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 υ B = V102 Bo ...
... axis 110 .ע 2 || v1 2 + v 2 = v02 where vo2 2 = 2 V10 2 + V1 2 is the 110 ( 12.126 ) 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 υ B = V102 Bo ...
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Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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