electromegnatic 22.2 EXERCISES 2-1 Show that 22-8) and (22-9) can also be -6 how that, in a li from (22-4) and (22-5) rather where P-0 and J,- Maxwell's equations first. be found completely fr...
EXERCISES 2-1 Show that 22-8) and (22-9) can also be -6 how that, in a li from (22-4) and (22-5) rather where P-0 and J,- Maxwell's equations first. be found completely fro and n by starting (22-4 an by going back to equation frst. t, if the free charge and current is, φ-, const. (zero is 1 equations determine N position and time, 227 Consider a re distributions and the polarization and ma gnetiza- tion are all given functions of then the general equations satisfied by the poten- M-0, while P is tials can be separated by using the form of the tion and time. S Lorentz condition appropriate for a vacuum. Find can be satistid and the differential equations satisfied by A and ф tained from a sin under these conditions. 22-3 Find the equations satisfied by the poten- the Her tials for a linear medium. B comple it leads to anys 22-8 This ex isotropic but non homogeneous Eand ding one
EXERCISES 2-1 Show that 22-8) and (22-9) can also be -6 how that, in a li from (22-4) and (22-5) rather where P-0 and J,- Maxwell's equations first. be found completely fro and n by starting (22-4 an by going back to equation frst. t, if the free charge and current is, φ-, const. (zero is 1 equations determine N position and time, 227 Consider a re distributions and the polarization and ma gnetiza- tion are all given functions of then the general equations satisfied by the poten- M-0, while P is tials can be separated by using the form of the tion and time. S Lorentz condition appropriate for a vacuum. Find can be satistid and the differential equations satisfied by A and ф tained from a sin under these conditions. 22-3 Find the equations satisfied by the poten- the Her tials for a linear medium. B comple it leads to anys 22-8 This ex isotropic but non homogeneous Eand ding one