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Lab 6: R-C Circuits
Only 6 more labs to go!!
A capacitor is a device used to store energy. In this lab we will measure how a capacitor “stores” up
or discharges energy.
If we use Kirkchoff’s loop rule to the circuit below we get the following equation:
R
Vapplied VR VC 0
C
Q
Vapplied IR 0
C
Remember the definition of current is:
So the equation becomes:
Q
I
t
Q
Q
Vapplied
R 0
t
C
Switch
Vapplied
This equation is called a differential
equation.
t
RC
The solution to this differential equation is:
Q CVapplied 1 e
This tells us that the charge on the capacitor is exponential in time.
t
RC
Q CVapplied 1 e t
Q CVapplied 1 e CVapplied
Charge, Q
Q = CVapplied
t = RC =
time (s)
Since we now know how the capacitor charges up we can write an equation that describes the voltage
as a function of time:
t
Voltage, V
Vcap
Q
RC
Vapplied 1 e
C
t = RC =
time (s)
C is called the RC-time constant. It represents the time which the voltage drop across the capacitor
reaches 63% of it’s max value.
Let’s look at this example:
R = 105
C = 5 F
1. Find the time constant, C.
C RC 105 5F 0.5 sec
Switch
Vapplied = 12 V
2. Find the charge on the capacitor at t = 0.2 sec
t
0.2 sec
RC
0
.
5
sec
1.9 105 C
Q CVapplied 1 e 5F 12V 1 e
3. Find the voltage on the capacitor at t = 0.3 sec
Vcap
t
0.3sec
RC
0
.
5
sec
5.42V
Vapplied 1 e 12V 1 e
4. How long will it take the capacitor to charge to 9V?
Vcap
t
t
RC
0
.
5
sec
t 0.69 sec
Vapplied 1 e 9V 12V 1 e
Now we will look at how the capacitor discharges its energy.
Let’s look at this circuit:
R
C
Use Kirchoff’s loop:
VR VC 0
Switch
The solution to this
differential equation is:
Q Q0 e
t
RC
V0Ce
t
RC
If we take the derivative of this equation
with respect to time we can get the current:
Charge, Q
Q
IR 0
C
Q
Q
R 0
t
C
time (s)
Q0
I
e
RC
t
RC
1.
R=105
Find the voltage across the capacitor at time,
t = 0.3 s.
Vcap V0 e
t
RC
9Ve
0.3 sec
0.5 sec
C=5F
4.94V
Switch
2. How long will it take the capacitor to reach 3 v?
Vcap V0e
t
RC
Vcap
V0
e
t
RC
Vapplied = 9V
Vcap
t
ln
RC
V0
Vcap
3V
0.5 sec ln 0.55s
t RC ln
9V
V0