RC Charging Circuit
Yaser Rahmati | یاسر رحمتی
Last updated
Yaser Rahmati | یاسر رحمتی
Last updated
The figure below shows a capacitor, ( ) in series with a resistor, ( ) forming an RC Charging Circuit connected across a DC battery supply ( ) via a mechanical switch.
At time zero, when the switch is first closed, the capacitor gradually charges up through the resistor until the voltage across it reaches the supply voltage of the battery. The manner in which the capacitor charges up is shown below.
So, we have:
0.5 time constant
0.5T = 0.5RC
39.3%
60.7%
0.7 time constant
0.7T = 0.7RC
50.3%
49.7%
1.0 time constants
1T = 1RC
63.2%
36.8%
2.0 time constants
2T = 1RC
86.5%
13.5%
3.0 time constants
3T = 1RC
95.0%
5.0%
4.0 time constant
4T = 1RC
98.2%
1.8%
5.0 time constants
5T = 1RC
99.3%
0.7%
Circuit Diagram
Voltage of Capacitor
Current
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Let us assume above, that the capacitor, is fully “discharged” and the switch (S) is fully open. These are the initial conditions of the circuit, then , and . When the switch is closed the time begins at and current begins to flow into the capacitor via the resistor.
Since the initial voltage across the capacitor is zero, ( ) at the capacitor appears to be a short circuit to the external circuit and the maximum current flows through the circuit restricted only by the resistor . Then by using Kirchhoff’s voltage law (KVL), the voltage drops around the circuit are given as:
This RC time constant only specifies a rate of charge where is in and in Farads.
Since voltage V is related to charge on a capacitor given by the equation, , the voltage across the capacitor ( ) at any instant in time during the charging period is given as: