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15.1: AC Sources

Most examples dealt with so far in this book, particularly those using batteries, have constant-voltage sources. Thus, once the current is established, it is constant. Direct current (dc) is the flow of electric charge in only one direction. It is the steady state of a constant-voltage circuit.

Most well-known applications, however, use a time-varying voltage source. Alternating current (ac) is the flow of electric charge that periodically reverses direction. An ac is produced by an alternating emf, which is generated in a power plant, as described in Induced Electric Fields. If the ac source varies periodically, particularly sinusoidally, the circuit is known as an ac circuit. Examples include the commercial and residential power that serves so many of our needs.

The ac voltages and frequencies commonly used in businesses and homes vary around the world. In a typical house, the potential difference between the two sides of an electrical outlet alternates sinusoidally with a frequency of 60 or 50 Hz and an amplitude of 156 or 311 V, depending on whether you live in the United States or Europe, respectively. Most people know the potential difference for electrical outlets is 120 V or 220 V in the US or Europe, but as explained later in the chapter, these voltages are not the peak values given here but rather are related to the common voltages we see in our electrical outlets. Figure \(\PageIndex{1}\) shows graphs of voltage and current versus time for typical dc and ac power in the United States.

Figures a and b show graphs of voltage and current versus time. Figure a shows direct voltage and direct current as horizontal lines on the graph, with positive y values. Current has a lower y-value than voltage. Figure b shows alternating voltage and alternating current as sinusoidal waves on the graph, with voltage having a greater amplitude than current. They have the same wavelength. Half-wavelength has an x-value of 8.33 and one wavelength has an x-value of 16.6. The maximum y-values of voltage and current are marked V0 and I0 respectively and the minimum y-values are marked minus V0 and minus I0 respectively

Figure \(\PageIndex{1}\): (a) The dc voltage and current are constant in time, once the current is established. (b) The voltage and current versus time are quite different for ac power. In this example, which shows 60-Hz ac power and time t in seconds, voltage and current are sinusoidal and are in phase for a simple resistance circuit. The frequencies and peak voltages of ac sources differ greatly.

Suppose we hook up a resistor to an ac voltage source and determine how the voltage and current vary in time across the resistor. Figure \(\PageIndex{2}\) shows a schematic of a simple circuit with an ac voltage source. The voltage fluctuates sinusoidally with time at a fixed frequency, as shown, on either the battery terminals or the resistor. Therefore, the ac voltage, or the “voltage at a plug,” can be given by

\[v(t) = V_0 \space \sin \space \omega t,\]

where

  • \(v\) is the voltage at time \(t\),
  • \(V_0\) is the peak voltage, and
  • \(\omega\) is the angular frequency in radians per second.

For a typical house in the United States, \(V_0 = 156 \space V\) and \(\omega = 120 \pi \space rad/s\), whereas in Europe, \(V_0 = 311 \space V\) and \(\omega = 100 \pi \space rad/s\).

Figure shows an AC sine wave. A circuit is shown at the top, pointing to the wave. It is labeled V source and has an AC voltage source connected to a resistor. The source is marked positive on one side and negative on the other. A circuit at the bottom, labeled V resistor, also points to the wave. It is similar to the top circuit but with the polarity of the source reversed

Figure \(\PageIndex{2}\): The potential difference V between the terminals of an ac voltage source fluctuates, so the source and the resistor have ac sine waves on top of each other. The mathematical expression for v is given by \(v = V_0 \space sin \space \omega t\).

For this simple resistance circuit, \(I = V/R\), so the ac current, meaning the current that fluctuates sinusoidally with time at a fixed frequency, is

\[i(t) = I_0 \space \sin \space \omega t,\]

where

  • \(i(t)\) is the current at time \(t\) and
  • \(I_0\) is the peak current and is equal to \(V_0/R\).

For this example, the voltage and current are said to be in phase, meaning that their sinusoidal functional forms have peaks, troughs, and nodes in the same place. They oscillate in sync with each other, as shown in Figure \(\PageIndex{1b}\). In these equations, and throughout this chapter, we use lowercase letters (such as \(i\)) to indicate instantaneous values and capital letters (such as \(I\)) to indicate maximum, or peak, values.

Current in the resistor alternates back and forth just like the driving voltage, since \(I = V/R\). If the resistor is a fluorescent light bulb, for example, it brightens and dims 120 times per second as the current repeatedly goes through zero. A 120-Hz flicker is too rapid for your eyes to detect, but if you wave your hand back and forth between your face and a fluorescent light, you will see the stroboscopic effect of ac.

Exercise \(\PageIndex{1}\)

If a European ac voltage source is considered, what is the time difference between the zero crossings on an ac voltage-versus-time graph?

Solution

10 ms

Contributors

Paul Peter Urone (Professor Emeritus at California State University, Sacramento) and Roger Hinrichs (State University of New York, College at Oswego) with Contributing Authors: Kim Dirks (University of Auckland) and Manjula Sharma (University of Sydney). This work is licensed by OpenStax University Physics under a Creative Commons Attribution License (by 4.0).