Classical Electrodynamics |
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Page 396
... mass m1 is ( 12.20 ) Similarly M2 + m12 2 2 m2 E1 = 2M M2 + m22 — m2 2 - E2 = 2M ( 12.21 ) ( 12.22 ) Often it is more convenient to have expressions for the kinetic energies than for the total energies . Using ( 12.15 ) , it is easy to ...
... mass m1 is ( 12.20 ) Similarly M2 + m12 2 2 m2 E1 = 2M M2 + m22 — m2 2 - E2 = 2M ( 12.21 ) ( 12.22 ) Often it is more convenient to have expressions for the kinetic energies than for the total energies . Using ( 12.15 ) , it is easy to ...
Page 400
... mass , the mass difference is AM = m „ 0 135.0 Mev , while the target mass is m2 = m , = 938.5 Mev . Then the threshold energy is Tth = 135.0 [ 1 1 + 135.0 2 ( 938.5 ) = 135.0 ( 1.072 ) = 144.7 Mev As another example consider the ...
... mass , the mass difference is AM = m „ 0 135.0 Mev , while the target mass is m2 = m , = 938.5 Mev . Then the threshold energy is Tth = 135.0 [ 1 1 + 135.0 2 ( 938.5 ) = 135.0 ( 1.072 ) = 144.7 Mev As another example consider the ...
Page 534
... mass m collides with a fixed , smooth , hard sphere of radius R. Assuming that the collision is elastic , show that in the dipole approximation ( neglecting retardation effects ) the classical differential cross section for the emission ...
... mass m collides with a fixed , smooth , hard sphere of radius R. Assuming that the collision is elastic , show that in the dipole approximation ( neglecting retardation effects ) the classical differential cross section for the emission ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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