Or
Explain in brief about the step response of
series RC circuits.
Consider
series RC circuit as shown in fig. The switch k is in open state initially.
There is no charge on condenser and A0 voltage across it. At instant t = 0,
switch k is closed.
Immediately
after closing a switch, the capacitor acts as a short circuit, so current at
the time of switching is high. A voltage across capacitor is zero at t = 0+.
As capacitor acts as a short circuit, the current is maximum and is given by
The current is maximum at t=0 + which is charging current. As the capacitor starts charging, the voltage across capacitor VC starts increasing and charging current starts decreasing. After some time, when the capacitor charges to V volts, it achieves steady state. In steady state, it acts as a open circuit so current will be zero finally.
After
switching instant applying Kirchoff’s voltage law.
Where VR
is voltage across resistor and VC is voltage across capacitor.
When the
steady state is achieved, total charge on the capacitor is Q coulombs.
So at t = 0, i = V/R is maximum current and in steady state it becomes zero.
The variation of voltage across capacitor and charging with respect to time is shown in fig.
The term RC in equation of VC is called time constant and denoted by measured in seconds When
So time constant of series RC circuit is defined as time required
by capacitor voltage to rise from zero to 0.632 of its final steady state value
during charging.
Thus, time constant of RC circuit can be defined as time in
seconds, during which the voltage across capacitor would reach its final steady
state value of its rate of change was maintained constant at its initial value
throughout charging period.
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