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Page 370
... space - like " and " time - like " separations between two events . Con- sider Fig . 11.10 , in which the time axis ( actually ct ) is vertical and the space axes are perpendicular to it . For simplicity only one space dimension is ...
... space - like " and " time - like " separations between two events . Con- sider Fig . 11.10 , in which the time axis ( actually ct ) is vertical and the space axes are perpendicular to it . For simplicity only one space dimension is ...
Page 384
... space components of a 4 - vector . Hence f must be the space part of a 4 - vector f1 = ( 1 , i2 ) , where : 1 fu = F ( 11.129 ) To see the meaning of the fourth component of the force - density 4 - vector we write out F42J2 { ƒ1 ...
... space components of a 4 - vector . Hence f must be the space part of a 4 - vector f1 = ( 1 , i2 ) , where : 1 fu = F ( 11.129 ) To see the meaning of the fourth component of the force - density 4 - vector we write out F42J2 { ƒ1 ...
Page 495
... space - time depended on the behavior of the particle at one earlier point in space - time , the retarded position . This situation corre- sponds in the left side of Fig . 14.14 to the fact that a given point lies on only one circle ...
... space - time depended on the behavior of the particle at one earlier point in space - time , the retarded position . This situation corre- sponds in the left side of Fig . 14.14 to the fact that a given point lies on only one circle ...
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Common terms and phrases
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