Page 292 - Schaum's Outline of Theory and Problems of Applied Physics
P. 292

CHAPTER 24







                                       Electric Current














        ELECTRIC CURRENT

        A flow of charge from one place to another constitutes an electric current.An electric circuit is a closed path
        in which an electric current carries energy from a source (such as a battery or generator) to a load (such as a
        motor or a lamp). In such a circuit (see Fig. 24-1), electric current is assumed to go from the positive terminal of
        the battery (or generator) through the circuit and back to the negative terminal of the battery. The direction of a
        current is conventionally considered to be that in which positive charge would have to move to produce the same
        effects as the actual current. Thus a current is always supposed to go from the positive terminal of a battery or
        generator to its negative terminal.
















                                                 Fig. 24-1

            Aconductorisasubstancethroughwhichchargecanfloweasily,andaninsulatorisonethroughwhichcharge
        can flow only with great difficulty. Metals, many liquids, and plasmas (gases whose molecules are charged) are
        conductors; nonmetallic solids, certain liquids, and gases whose molecules are electrically neutral are insulators.
        A number of substances, called semiconductors, are intermediate in their ability to conduct charge.
            Electric currents in metal wires always consist of flows of electrons; such currents are assumed to occur in
        the direction opposite to that in which the electrons move. Since a positive charge going one way is for most
        purposes equivalent to a negative charge going the other way, this assumption makes no practical difference.
        Both positive and negative charges move when a current is present in a liquid or gaseous conductor.
            If an amount of charge q passes a given point in a conductor in the time interval t, the current in the
        conductor is
                                                       q
                                                   I =
                                                       t
                                                          charge
                                        Electric current =
                                                       time interval
                                                   277
   287   288   289   290   291   292   293   294   295   296   297