Classical ElectromagnetismCLASSICAL ELECTROMAGNETISM features a friendly, informal writing style. The text has received numerous accolades. |
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Page 74
... force on a charge Q , moving at velocity v , we obtain the fundamental Lorentz force : F = QE + Qv x B ( 3.12 ) If the charge is stationary , the force depends on E ; if it moves , there is an addi- tional force proportional to v and B ...
... force on a charge Q , moving at velocity v , we obtain the fundamental Lorentz force : F = QE + Qv x B ( 3.12 ) If the charge is stationary , the force depends on E ; if it moves , there is an addi- tional force proportional to v and B ...
Page 467
... Lorentz force . The magnetic field is still there , but it has no effect . The force that was entirely magnetic is now entirely electrostatic . Examining the distri- bution of charges , we find that the negative charges are moving and ...
... Lorentz force . The magnetic field is still there , but it has no effect . The force that was entirely magnetic is now entirely electrostatic . Examining the distri- bution of charges , we find that the negative charges are moving and ...
Page 485
... Lorentz force Qv x B : We move downwards along with the charge . Now the charge is stationary , Figure 18.35b , and the wire is moving towards it . An E field must spring up , as shown , to replace the lost Lorentz force . But where is ...
... Lorentz force Qv x B : We move downwards along with the charge . Now the charge is stationary , Figure 18.35b , and the wire is moving towards it . An E field must spring up , as shown , to replace the lost Lorentz force . But where is ...
Contents
Vector Analysis | 1 |
Electric Field EGausss Law | 33 |
Magnetic Field BAmpères Law | 66 |
Copyright | |
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acceleration Ampère's law ANSWER antenna axis Biot-Savart Biot-Savart law calculate capacitance capacitor charge density charge Q circuit component conducting conductor constant coordinates Coulomb's law curl current density cylinder dielectric differential direction distance divergence E field electric dipole electric field electromagnetic electrons electrostatic energy example Faraday's law field lines Figure flux frequency Gauss's law inductance inductor infinite inside integral Laplace's equation line charge loop Lorentz force Lorentz transformation magnetic dipole magnetic field magnetic monopoles Maxwell's equations meter momentum moving negative parallel perpendicular plane plasma plates polarization positive potential Poynting's vector primed frame Problem radiation radius reference frame relative relativistic resistor right-hand rule scalar Section solenoid speed sphere spherical stationary surface charge theorem tion unit velocity voltage waveguide wire zero Απεργ Απερτ μο ду дх