Ohm's Law m58732 Ohm's Law By the end of this section, you will be able to: Describe Ohm’s law Recognize when Ohm’s law applies and when it does not a7dfdf47-5742-4be9-a6ae-4398ce8f93d7 We have been discussing three electrical properties so far in this chapter: current, voltage, and resistance. It turns out that many materials exhibit a simple relationship among the values for these properties, known as Ohm’s law. Many other materials do not show this relationship, so despite being called Ohm’s law, it is not considered a law of nature, like Newton’s laws or the laws of thermodynamics. But it is very useful for calculations involving materials that do obey Ohm’s law.
Description of Ohm’s Law The current that flows through most substances is directly proportional to the voltage V applied to it. The German physicist Georg Simon Ohm (1787–1854) was the first to demonstrate experimentally that the current in a metal wire is directly proportional to the voltage applied: This important relationship is the basis for Ohm’s law. It can be viewed as a cause-and-effect relationship, with voltage the cause and current the effect. This is an empirical law, which is to say that it is an experimentally observed phenomenon, like friction. Such a linear relationship doesn’t always occur. Any material, component, or device that obeys Ohm’s law, where the current through the device is proportional to the voltage applied, is known as an ohmic material or ohmic component. Any material or component that does not obey Ohm’s law is known as a nonohmic material or nonohmic component.
Ohm’s Experiment In a paper published in 1827, Georg Ohm described an experiment in which he measured voltage across and current through various simple electrical circuits containing various lengths of wire. A similar experiment is shown in . This experiment is used to observe the current through a resistor that results from an applied voltage. In this simple circuit, a resistor is connected in series with a battery. The voltage is measured with a voltmeter, which must be placed across the resistor (in parallel with the resistor). The current is measured with an ammeter, which must be in line with the resistor (in series with the resistor).
The experimental set-up used to determine if a resistor is an ohmic or nonohmic device. (a) When the battery is attached, the current flows in the clockwise direction and the voltmeter and ammeter have positive readings. (b) When the leads of the battery are switched, the current flows in the counterclockwise direction and the voltmeter and ammeter have negative readings.
In this updated version of Ohm’s original experiment, several measurements of the current were made for several different voltages. When the battery was hooked up as in (a), the current flowed in the clockwise direction and the readings of the voltmeter and ammeter were positive. Does the behavior of the current change if the current flowed in the opposite direction? To get the current to flow in the opposite direction, the leads of the battery can be switched. When the leads of the battery were switched, the readings of the voltmeter and ammeter readings were negative because the current flowed in the opposite direction, in this case, counterclockwise. Results of a similar experiment are shown in .
A resistor is placed in a circuit with a battery. The voltage applied varies from −10.00 V to +10.00 V, increased by 1.00-V increments. A plot shows values of the voltage versus the current typical of what a casual experimenter might find.
In this experiment, the voltage applied across the resistor varies from −10.00 to +10.00 V, by increments of 1.00 V. The current through the resistor and the voltage across the resistor are measured. A plot is made of the voltage versus the current, and the result is approximately linear. The slope of the line is the resistance, or the voltage divided by the current. This result is known as Ohm’s law: V=IR, where V is the voltage measured in volts across the object in question, I is the current measured through the object in amps, and R is the resistance in units of ohms. As stated previously, any device that shows a linear relationship between the voltage and the current is known as an ohmic device. A resistor is therefore an ohmic device. Measuring Resistance A carbon resistor at room temperature (20°C) is attached to a 9.00-V battery and the current measured through the resistor is 3.00 mA. (a) What is the resistance of the resistor measured in ohms? (b) If the temperature of the resistor is increased to 60°C by heating the resistor, what is the current through the resistor? Strategy (a) The resistance can be found using Ohm’s law. Ohm’s law states that V=IR, so the resistance can be found using R=V/I. (b) First, the resistance is temperature dependent so the new resistance after the resistor has been heated can be found using R=R0(1+αΔT). The current can be found using Ohm’s law in the form I=V/R. Solution Using Ohm’s law and solving for the resistance yields the resistance at room temperature: The resistance at 60°C can be found using R=R0(1+αΔT) where the temperature coefficient for carbon is α=−0.0005. R=R0(1+αΔT)=3.00×103(1−0.0005(60°C−20°C))=2.94kΩ. The current through the heated resistor is Significance A change in temperature of 40°C resulted in a 2.00% change in current. This may not seem like a very great change, but changing electrical characteristics can have a strong effect on the circuits. For this reason, many electronic appliances, such as computers, contain fans to remove the heat dissipated by components in the electric circuits. The voltage supplied to your house varies as V(t)=Vmaxsin(2πft). If a resistor is connected across this voltage, will Ohm’s law V=IR still be valid? Yes, Ohm’s law is still valid. At every point in time the current is equal to I(t)=V(t)/R, so the current is also a function of time, I(t)=VmaxRsin(2πft). See how the equation form of Ohm’s law relates to a simple circuit by engaging the simulation below. Adjust the voltage and resistance, and see the current change according to Ohm’s law. The sizes of the symbols in the equation change to match the circuit diagram.