## Principles of Electricity and Electromagnetism |

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Page 108

For a complete solution Eqs. (4.1) and (4.2) must be applied systematically to the

network of conductors and the currents in every branch

conducting paths that can be traversed through a complex circuit can be chosen

in ...

For a complete solution Eqs. (4.1) and (4.2) must be applied systematically to the

network of conductors and the currents in every branch

**obtained**. The closedconducting paths that can be traversed through a complex circuit can be chosen

in ...

Page 145

Kirchhoff's laws yield the following equations: It = U + 2R V = Bi> + Ria RiR = Bi*

+ Rlil Eliminating iB, the following parametric equations are

and V: . = RiT - Bi\ tL R + RL Fia. 5.5. — Thyrite V = Bi\ + RiT - RiL (5.5) brid8e- On

...

Kirchhoff's laws yield the following equations: It = U + 2R V = Bi> + Ria RiR = Bi*

+ Rlil Eliminating iB, the following parametric equations are

**obtained**relating nand V: . = RiT - Bi\ tL R + RL Fia. 5.5. — Thyrite V = Bi\ + RiT - RiL (5.5) brid8e- On

...

Page 347

of the order of 10-2 were

cent in the determination of g. Table I gives the values of g

for various ions. The superscript indicates the valence and the quantity in ...

of the order of 10-2 were

**obtained**, which permitted an accuracy of about 5 percent in the determination of g. Table I gives the values of g

**obtained**by Sucksmithfor various ions. The superscript indicates the valence and the quantity in ...

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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