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Transcript
Engineering Science EAB_S_127
Electricity Chapter 4
Introduction




Capacitance
Energy stored in a capacitor
Charging and Discharging through a resistor
Time constants
Capacitance



Capacitors are devices which store electrical charge
A capacitor consists of two plates separated by an
insulator, as shown in Figure 4.1
The negative plate is connected to a low potential and
the positive plate to a high potential
Insulator
Q
-
+
-
+
-
+
V
Negative plate
Figure 4.1
Positive plate
Capacitance continued




The total amount of the charge stored, is denoted by Q
and the voltage across the plates by V
Q
The capacitance then is defined as
C
[F ]
V
Where C is in Farads
1 Farad = 1 Coulomb per Volt
Insulator
Q
-
+
-
+
-
+
V
Negative plate
Figure 4.1
Positive plate
Energy Stored in a Capacitor




When charged, a capacitor stores electrical energy
Recall the formula for electrical energy in a circuit, which
is W = VQ
However, we need to be careful as the voltage between
the plates in a capacitor varies from 0 to V
Hence, to be more accurate we should use the average
0  Vab Vab
voltage
Vm 
W  VmQ 

So

Hence W 
Vab
Q
2
2

2
and we know
Vab
1
CVab  CVab2
2
2
Q  CVab
Energy Stored in a Capacitor: Example


Question: A capacitor is supplied with 10 V in a circuit. If
its capacitance is 150µF, what is the electrical energy
stored in the capacitor?
Answer:
W
1
1
CVab2  150 10 6 10 2  75 10  4 J  7.5mJ
2
2
Charging and Discharging a Capacitor

Charging and discharging a capacitor from a DC (direct
current) source is shown below
V


We assume that the voltage source,V, has no internal
resistance
If the switch was held in position 2 for a long time, then the
capacitor would be completely discharged, Vc = 0V
Charging a Capacitor


If the switch is then moved to position 1, current will start
to flow through the resistor R, thereby charging the
capacitor, C
The voltage across the plates of the capacitor will rise in
time, until after a long time, the capacitor will have the same
voltage as the supply,V
V
VC
Discharging a Capacitor


If the switch is then moved back to position 2, current will
start to flow through the resistor R, thereby discharging
the capacitor, C
The voltage across the plates of the capacitor will fall in
time, until after a long time, the capacitor will have no
charge at all and again, Vc = 0V
V
VC
Time Constant of an RC Circuit



It can be shown mathematically, that the time for the
voltage to fall to 37% of its original voltage, t = RC
The charging and discharging curves have an exponential
nature
When discharging
VC

When charging
VC
RC Time Constant: Example




Question: If R = 1000W and C = 0.1mF, what is the time
constant of the circuit?
Answer: t = RC = 1000x0.1x10-6 = 0.1 x10-3 = 100ms
Hence, when discharging, the following equation can be
used to calculate the voltage
When charging
Summary

Learning Outcomes:





Capacitors and capacitance
Energy stored in a capacitor
Charging a capacitor
Time constants
Exponential charging and discharging curves