10.5 RC Circuits

Circuits with Resistance and Capacitance

An RC circuit is a circuit containing resistance and capacitance. As presented in Capacitance, the capacitor is an electrical component that stores electric charge, storing energy in an electric field.

Figure 10.38(a) shows a simple RC circuit that employs a dc (direct current) voltage source [latex]\epsilon[/latex], a resistor R, a capacitor C, and a two-position switch. The circuit allows the capacitor to be charged or discharged, depending on the position of the switch. When the switch is moved to position A, the capacitor charges, resulting in the circuit in part (b). When the switch is moved to position B, the capacitor discharges through the resistor.

Charging a Capacitor

We can use Kirchhoff’s loop rule to understand the charging of the capacitor. This results in the equation [latex]\epsilon -{V}_{R}-{V}_{c}=0.[/latex] This equation can be used to model the charge as a function of time as the capacitor charges. Capacitance is defined as [latex]C=q\text{/}V,[/latex] so the voltage across the capacitor is [latex]{V}_{C}=\frac{q}{C}[/latex]. Using Ohm’s law, the potential drop across the resistor is [latex]{V}_{R}=IR[/latex], and the current is defined as [latex]I=dq\text{/}dt.[/latex]

This differential equation can be integrated to find an equation for the charge on the capacitor as a function of time.

Let [latex]u=\epsilon C-q[/latex], then [latex]du=\text{−}dq.[/latex] The result is

Simplifying results in an equation for the charge on the charging capacitor as a function of time:

A graph of the charge on the capacitor versus time is shown in Figure 10.39(a). First note that as time approaches infinity, the exponential goes to zero, so the charge approaches the maximum charge [latex]Q=C\epsilon[/latex] and has units of coulombs. The units of RC are seconds, units of time. This quantity is known as the time constant:

At time [latex]t=\tau =RC[/latex], the charge is equal to [latex]1-{e}^{-1}=1-0.368=0.632[/latex] of the maximum charge [latex]Q=C\epsilon[/latex]. Notice that the time rate change of the charge is the slope at a point of the charge versus time plot. The slope of the graph is large at time [latex]t=0.0\phantom{\rule{0.2em}{0ex}}\text{s}[/latex] and approaches zero as time increases.

As the charge on the capacitor increases, the current through the resistor decreases, as shown in Figure 10.39(b). The current through the resistor can be found by taking the time derivative of the charge.

At time [latex]t=0.00\phantom{\rule{0.2em}{0ex}}\text{s},[/latex] the current through the resistor is [latex]{I}_{0}=\frac{\epsilon }{R}[/latex]. As time approaches infinity, the current approaches zero. At time [latex]t=\tau[/latex], the current through the resistor is [latex]I\left(t=\tau \right)={I}_{0}{e}^{-1}=0.368{I}_{0}.[/latex]

Figure 10.39(c) and Figure 10.39(d) show the voltage differences across the capacitor and the resistor, respectively. As the charge on the capacitor increases, the current decreases, as does the voltage difference across the resistor[latex]{V}_{R}\left(t\right)=\left({I}_{0}R\right){e}^{\text{−}t\text{/}\tau }=\epsilon {e}^{\text{−}t\text{/}\tau }.[/latex] The voltage difference across the capacitor increases as[latex]{V}_{C}\left(t\right)=\epsilon \left(1-{e}^{\text{−}t\text{/}\tau }\right).[/latex]

Discharging a Capacitor

When the switch in Figure 10.38(a) is moved to position B, the circuit reduces to the circuit in part (c), and the charged capacitor is allowed to discharge through the resistor. A graph of the charge on the capacitor as a function of time is shown in Figure 10.40(a). Using Kirchhoff’s loop rule to analyze the circuit as the capacitor discharges results in the equation [latex]\text{−}{V}_{R}-{V}_{c}=0[/latex], which simplifies to [latex]IR+\frac{q}{C}=0[/latex]. Using the definition of current[latex]\frac{dq}{dt}R=-\frac{q}{C}[/latex] and integrating the loop equation yields an equation for the charge on the capacitor as a function of time:

Here, Q is the initial charge on the capacitor and [latex]\tau =RC[/latex] is the time constant of the circuit. As shown in the graph, the charge decreases exponentially from the initial charge, approaching zero as time approaches infinity.

The current as a function of time can be found by taking the time derivative of the charge:

The negative sign shows that the current flows in the opposite direction of the current found when the capacitor is charging. Figure 10.40(b) shows an example of a plot of charge versus time and current versus time. A plot of the voltage difference across the capacitor and the voltage difference across the resistor as a function of time are shown in parts (c) and (d) of the figure. Note that the magnitudes of the charge, current, and voltage all decrease exponentially, approaching zero as time increases.

Now we can explain why the flash camera mentioned at the beginning of this section takes so much longer to charge than discharge: The resistance while charging is significantly greater than while discharging. The internal resistance of the battery accounts for most of the resistance while charging. As the battery ages, the increasing internal resistance makes the charging process even slower.

RC circuits have many applications. They can be used effectively as timers for applications such as intermittent windshield wipers, pace makers, and strobe lights. Some models of intermittent windshield wipers use a variable resistor to adjust the interval between sweeps of the wiper. Increasing the resistance increases the RC time constant, which increases the time between the operation of the wipers.

Another application is the pacemaker. The heart rate is normally controlled by electrical signals, which cause the muscles of the heart to contract and pump blood. When the heart rhythm is abnormal (the heartbeat is too high or too low), pace makers can be used to correct this abnormality. Pacemakers have sensors that detect body motion and breathing to increase the heart rate during physical activities, thus meeting the increased need for blood and oxygen, and an RC timing circuit can be used to control the time between voltage signals to the heart.

Looking ahead to the study of ac circuits (Alternating-Current Circuits), ac voltages vary as sine functions with specific frequencies. Periodic variations in voltage, or electric signals, are often recorded by scientists. These voltage signals could come from music recorded by a microphone or atmospheric data collected by radar. Occasionally, these signals can contain unwanted frequencies known as “noise.” RC filters can be used to filter out the unwanted frequencies.

In the study of electronics, a popular device known as a 555 timer provides timed voltage pulses. The time between pulses is controlled by an RC circuit. These are just a few of the countless applications of RC circuits.

The RC circuit has thousands of uses and is a very important circuit to study. Not only can it be used to time circuits, it can also be used to filter out unwanted frequencies in a circuit and used in power supplies, like the one for your computer, to help turn ac voltage to dc voltage.