Principles of Electricity and Electromagnetism |
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Page 23
... condenser with charges q and -q . The difference of V C ( a ) 91-9 affa affa q C1 C2 C3 ( b ) 92 C2 ・ 921 all - a C3 ( c ) FIG . 1.16 . - Combinations of condensers . ( a ) Condenser . ( b ) Condensers in series . ( c ) Condensers in ...
... condenser with charges q and -q . The difference of V C ( a ) 91-9 affa affa q C1 C2 C3 ( b ) 92 C2 ・ 921 all - a C3 ( c ) FIG . 1.16 . - Combinations of condensers . ( a ) Condenser . ( b ) Condensers in series . ( c ) Condensers in ...
Page 224
... condenser . The power loss that occurs in a condenser depends on the nature of the dielectric and the frequency . If the dielectric is " leaky , " ie . , if it has an appreciable conductivity , the condenser can be represented to a ...
... condenser . The power loss that occurs in a condenser depends on the nature of the dielectric and the frequency . If the dielectric is " leaky , " ie . , if it has an appreciable conductivity , the condenser can be represented to a ...
Page 454
... condenser as a function of the time . What is the charge on the condenser after 10 complete oscillations ? What is the time interval between the shorting of the condenser and the next time that there is no current through the inductance ...
... condenser as a function of the time . What is the charge on the condenser after 10 complete oscillations ? What is the time interval between the shorting of the condenser and the next time that there is no current through the inductance ...
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alternating current alternating-current amplitude angle angular velocity anode applied approximately armature assumed atom axis calculated capacity cathode cell centimeter characteristic charge q circuit coefficient coil component condenser conduction conductor considered copper current density current flowing curve cylinder deflection determined dielectric constant direct-current discharge distance effective electric field electromotive force electrons electrostatic element energy equal equation ferromagnetic filament flux force frequency function galvanometer given grad grid hence hysteresis impedance induction insulating integral known Laplace's equation linear load magnetic field magnetic moment magnitude maximum measured medium metal meter molecules negative normal obtained ohms parallel plate polarization potential difference potential wave potentiometer produced proportional quantity R₁ radius ratio rectifier region represents resistance rotation Show shown in Fig solenoid solution substance surface temperature terminals theorem torque tube V₁ vector voltage volts wire written zero