Principles of Electricity and Electromagnetism |
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Page 71
The electric field E is of course the force per unit charge on a test charge located
at the point, but when dimensions of atomic magnitude are considered, E may no
longer be considered uniform. Also, the average value of E over a region is not ...
The electric field E is of course the force per unit charge on a test charge located
at the point, but when dimensions of atomic magnitude are considered, E may no
longer be considered uniform. Also, the average value of E over a region is not ...
Page 291
If a current equal to that in the bounding circuit is considered to flow around each
element, the effects of coincident paths exactly cancel one another since they are
traversed in opposite directions and the net effect is simply that due to the ...
If a current equal to that in the bounding circuit is considered to flow around each
element, the effects of coincident paths exactly cancel one another since they are
traversed in opposite directions and the net effect is simply that due to the ...
Page 300
By Stokes's theorem <t>j = J" B • ds = <£,k . dl, This is the energy from the point of
view of closed filamentary circuits that may be considered to be distributed in any
way throughout a conductor or series of conductors. The sum of the current ...
By Stokes's theorem <t>j = J" B • ds = <£,k . dl, This is the energy from the point of
view of closed filamentary circuits that may be considered to be distributed in any
way throughout a conductor or series of conductors. The sum of the current ...
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alternating current alternating-current ampere amplifier amplitude angle angular anode antenna applied approximately armature assumed atom axis calculated capacity cathode cell characteristic charge circuit coefficient coil component condenser conducting conductor considered constant curl current flowing curve deflection density determined dielectric dielectric constant direct-current direction discharge effective electric field electromagnetic electromotive force electrons electrostatic element energy equal equation flux force frequency function galvanometer given grid hence impedance induction integral ions known Laplace's equation length linear load magnetic field magnetic induction magnitude maximum measured metal meter negative normal obtained ohms oscillations output parallel phase plane plate polarization positive potential difference potential wave potentiometer produced proportional quantities radiation radius ratio reactance region represents resistance resonant rotation scalar Show shown in Fig solenoid solution surface temperature terminals theorem torque tube unit vector velocity voltage volts wire written zero