Electricity and MagnetismA text for the standard electro-magnetism course for students in physics and engineering. Treats requisite theory with extensive examples of real-world applications. Offers coverage of topics neglected in most texts at this level, such as macroscopic vs. microscopic properties of matter. Also features a shorter, more student-oriented presentaton of the material, larger problem sets, and thorough discussion of alternative solution methods. |
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Page 372
... wires are located at x = ± a and are parallel to the y axis . The wires carry constant currents +1 , respectively . Another infinitely long parallel wire is moving with its instantaneous position at distances r , and r2 from the wires ...
... wires are located at x = ± a and are parallel to the y axis . The wires carry constant currents +1 , respectively . Another infinitely long parallel wire is moving with its instantaneous position at distances r , and r2 from the wires ...
Page 385
... wire carrying a current I2 is in the plane of the loop and at a distance d > R from the center of the loop . R Figure 12.6 Force between 12 a current- carrying wire and a current - carrying loop placed in the same plane . 2 Since we are ...
... wire carrying a current I2 is in the plane of the loop and at a distance d > R from the center of the loop . R Figure 12.6 Force between 12 a current- carrying wire and a current - carrying loop placed in the same plane . 2 Since we are ...
Page 514
... wire . Determine the vector potential of two infinitely long , parallel wires , 1 and 2 , at distances p1 and p2 from an observation point P in the plane of the wires . The distance between the wires is d . The current Io in wire 1 is ...
... wire . Determine the vector potential of two infinitely long , parallel wires , 1 and 2 , at distances p1 and p2 from an observation point P in the plane of the wires . The distance between the wires is d . The current Io in wire 1 is ...
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angle applied assume atoms axis becomes boundary conditions calculated called capacitor charge density charge distribution circuit coefficients components conducting conductor Consider constant continuous coordinates cylinder defined dependence derived Determine dielectric difference dipole direction discussed distance distribution effect electric field electrostatic element energy equal equation Example exists expression external fact Figure flux follows force frequency function given gives hence implies incidence inductance inside integral interface length loop magnetic field material medium method moving normal observer obtain origin parallel placed plane plates point charge polarization potential problem produced properties radiation radius reflection region relation resistance respectively result satisfy scalar shown in Fig solution solved space sphere spherical Substituting surface surface charge transformation unit vector volume wave wire write zero