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Basically, in a battery, the electric charges in the atoms and molecules have potential energy of position, due to certain electrostatic binding forces present. When the battery delivers current to an external load, chemical reactions occur in the battery in which the atoms and molecules are rearranged, and in the rearrangement the potential energy of the charges is reduced, being transformed into the kinetic energy required to move the charges against the internal eld of the battery. There are, as you may know, a number of di erent types of cell, each type having certain advantages and disadvantages. All cells, however, produce a relatively low value of potential di erence between their electrodes, ranging in value from 1.2 to 2.2 volts, approximately. In order to obtain higher potential di erences, which are often required in practical applications, it is generally necessary to connect two or more cells together to form a battery of cells, as illustrated in Figs. 19 and 20.

Figure 19 is the symbol used, when drawing schematic circuit diagrams, to indicate the presence of a single cell. Notice that the longer horizontal line represents the positive electrode and the shorter horizontal line represents the negative electrode. As mentioned above, in order to provide higher potential di erences it is necessary to stack or series-connect a number of cells to form a battery. This is indicated schematically in Fig. 20, where a is the negative terminal of the battery and b is the positive terminal; together, a and b are the positive and negative output terminals of the battery. Note that, going from a to b through the battery, the positive electrode of each cell connects to the negative electrode of the next cell. If n such cells are thus seriesconnected to form a battery, the potential di erence between the battery output terminals will be n times the potential di erence of a single cell. In Fig. 20, V is the potential di erence between the output terminals a and b. Since potential di erence is measured in volts, it is customary to call V the battery voltage.

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And Coffee Too!

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Let us now return to Fig. 17 and replace the two charged plates with a battery of V volts. Since the battery is a source of constant emf, it will be able to maintain a constant current of I amperes* owing in the circuit, as in Fig. 21. (For reasons discussed in section 2.1, we will always assume current to consist of a ow of positive charges which ow out of the positive terminal of the battery, for the same reason that they ow out of the positive plate in Fig. 17.)

* Both i and I are used to represent electric current. i generally designates current that changes from instant to instant, while I designates a constant value of current. Thus in Figs. 21 and 22 the current would have a constant value of I amperes for given, xed values of V and R.

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In Fig 21, the tungsten lament of the light bulb o ers a considerable amount of opposition, or what is called ELECTRICAL RESISTANCE, to the passage of electric current through it Because of the high resistance of the lament, the battery voltage V must be relatively high in order to produce the amount of current I required to heat the lament to incandescence On the other hand, the copper wires used to connect the battery to the bulb have very little resistance; as a matter of fact, in almost all cases we can disregard the very small resistance of the wires used to connect the various parts of the circuit together, and assume that, for practical purposes, the connecting wires have zero resistance to the passage of current through them We will always assume this to be the case, unless otherwise stated.

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