## Principles of Electricity and Electromagnetism |

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Page 49

The batteries then act as additional sources of charge and

the change in electrostatic

the conductors in which the potentials remain unaltered is given by SU = IXtqiVi ...

The batteries then act as additional sources of charge and

**energy**. From Eq. (2.1)the change in electrostatic

**energy**associated with a change in the positions ofthe conductors in which the potentials remain unaltered is given by SU = IXtqiVi ...

Page 244

cient

factor of the order of 100 before the effect is detectable. Even then the ionization

per centimeter path under the same conditions is generally smaller, though in ...

cient

**energy**. But this**energy**must be larger than that of an ionizing electron by afactor of the order of 100 before the effect is detectable. Even then the ionization

per centimeter path under the same conditions is generally smaller, though in ...

Page 296

It is evident from any of these expressions that a circuit carrying a constant

current tends to take up such a position as to include the largest possible flux

through it in the positive sense of the right-hand-screw notation. The

small ...

It is evident from any of these expressions that a circuit carrying a constant

current tends to take up such a position as to include the largest possible flux

through it in the positive sense of the right-hand-screw notation. The

**energy**of asmall ...

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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