## Principles of Electricity and Electromagnetism |

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Page 22

Hence the

they are zero. As an example consider the three conductors shown in Fig. 1.15.

Assume first that q3 = 0. In this case the discussion of the preceding section ...

Hence the

**coefficients**of induction are in general negative, though in some casesthey are zero. As an example consider the three conductors shown in Fig. 1.15.

Assume first that q3 = 0. In this case the discussion of the preceding section ...

Page 297

The integral is purely a geometrical quantity that can be calculated when the

positions of the circuits are specified though the computation is frequently difficult

to perform. The

The integral is purely a geometrical quantity that can be calculated when the

positions of the circuits are specified though the computation is frequently difficult

to perform. The

**coefficient**of ttf'i is known as the**coefficient**of mutual inductance ...Page 489

If the

are the same, to what frequency must the secondary be tuned for maximum

current at a signal frequency of 1 megacycle? 4. If the secondary circuit of the

preceding ...

If the

**coefficient**of coupling is 0.2 and the primary and secondary inductancesare the same, to what frequency must the secondary be tuned for maximum

current at a signal frequency of 1 megacycle? 4. If the secondary circuit of the

preceding ...

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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 grad grid hence hysteresis 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 Show shown in Fig solenoid solution surface temperature terminals theorem torque tube unit vector velocity voltage volts wire written zero