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i = 1 N V i = 0 .

This equation is often referred to as Kirchhoff’s loop law, which we will look at in more detail later in this chapter. For [link] , the sum of the potential drop of each resistor and the voltage supplied by the voltage source should equal zero:

V V 1 V 2 V 3 = 0 , V = V 1 + V 2 + V 3 , = I R 1 + I R 2 + I R 3 , I = V R 1 + R 2 + R 3 = V R eq .

Since the current through each component is the same, the equality can be simplified to an equivalent resistance, which is just the sum of the resistances of the individual resistors.

Any number of resistors can be connected in series. If N resistors are connected in series, the equivalent resistance is

R eq = R 1 + R 2 + R 3 + + R N 1 + R N = i = 1 N R i .

One result of components connected in a series circuit is that if something happens to one component, it affects all the other components. For example, if several lamps are connected in series and one bulb burns out, all the other lamps go dark.

Equivalent resistance, current, and power in a series circuit

A battery with a terminal voltage of 9 V is connected to a circuit consisting of four 20 - Ω and one 10 - Ω resistors all in series ( [link] ). Assume the battery has negligible internal resistance. (a) Calculate the equivalent resistance of the circuit. (b) Calculate the current through each resistor. (c) Calculate the potential drop across each resistor. (d) Determine the total power dissipated by the resistors and the power supplied by the battery.

The figure shows four resistors of 20 Ω and one resistor of 10 Ω connected in series to a 9 V voltage source.
A simple series circuit with five resistors.

Strategy

In a series circuit, the equivalent resistance is the algebraic sum of the resistances. The current through the circuit can be found from Ohm’s law and is equal to the voltage divided by the equivalent resistance. The potential drop across each resistor can be found using Ohm’s law. The power dissipated by each resistor can be found using P = I 2 R , and the total power dissipated by the resistors is equal to the sum of the power dissipated by each resistor. The power supplied by the battery can be found using P = I ε .

Solution

  1. The equivalent resistance is the algebraic sum of the resistances:
    R eq = R 1 + R 2 + R 3 + R 4 + R 5 = 20 Ω + 20 Ω + 20 Ω + 20 Ω + 10 Ω = 90 Ω .
  2. The current through the circuit is the same for each resistor in a series circuit and is equal to the applied voltage divided by the equivalent resistance:
    I = V R eq = 9 V 90 Ω = 0.1 A.
  3. The potential drop across each resistor can be found using Ohm’s law:
    V 1 = V 2 = V 3 = V 4 = ( 0.1 A ) 20 Ω = 2 V , V 5 = ( 0.1 A ) 10 Ω = 1 V , V 1 + V 2 + V 3 + V 4 + V 5 = 9 V .

    Note that the sum of the potential drops across each resistor is equal to the voltage supplied by the battery.
  4. The power dissipated by a resistor is equal to P = I 2 R , and the power supplied by the battery is equal to P = I ε :
    P 1 = P 2 = P 3 = P 4 = ( 0.1 A ) 2 ( 20 Ω ) = 0.2 W , P 5 = ( 0.1 A ) 2 ( 10 Ω ) = 0.1 W , P dissipated = 0.2 W + 0.2 W + 0.2 W + 0.2 W + 0.1 W = 0.9 W , P source = I ε = ( 0.1 A ) ( 9 V ) = 0.9 W .

Significance

There are several reasons why we would use multiple resistors instead of just one resistor with a resistance equal to the equivalent resistance of the circuit. Perhaps a resistor of the required size is not available, or we need to dissipate the heat generated, or we want to minimize the cost of resistors. Each resistor may cost a few cents to a few dollars, but when multiplied by thousands of units, the cost saving may be appreciable.

Practice Key Terms 1

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Source:  OpenStax, University physics volume 2. OpenStax CNX. Oct 06, 2016 Download for free at http://cnx.org/content/col12074/1.3
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