Principles of Electricity and Electromagnetism |
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Page 23
... condenser with charges q and -q . The difference of 919 V2 V3 ੫॥੧੧॥੧੧॥੧ all - ai १ 9292 C2 C1 C2 C3 ( b ) C3 ( c ) C ( a ) FIG . 1.16 . - Combinations of condensers . ( a ) Condenser . ( b ) Condensers in series . ( c ) Condensers ...
... condenser with charges q and -q . The difference of 919 V2 V3 ੫॥੧੧॥੧੧॥੧ all - ai १ 9292 C2 C1 C2 C3 ( b ) C3 ( c ) C ( a ) FIG . 1.16 . - Combinations of condensers . ( a ) Condenser . ( b ) Condensers in series . ( c ) Condensers ...
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 , ” i.e. , 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 , ” i.e. , 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 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 dynamic resistance effective electric field electromagnetic electromotive force electrons electrostatic element energy equal equation flux force frequency function galvanometer grad harmonic hence impedance induction integral ions known length linear load magnetic field magnetic moment magnitude maximum measured meter negative obtained ohms oscillations output parallel phase plane plate current positive potential difference potentiometer quantities R₁ radiation radius ratio reactance region represents resistance resonant rotation scalar shown in Fig solution surface temperature terminals theorem torque transconductance triode tube unit vacuum tube vector velocity voltage volts wave wire written zero