RC CIRCUIT MEANS CONSIST RESISTOR AND CAPACITOR

Dear Theresh,

Circuits with resistors and batteries have time-independent solutions: the current doesn''t change as time goes by. Adding one or more capacitors changes this. The solution is then time-dependent: the current is a function of time.

Consider a series RC circuit with a battery, resistor, and capacitor in series. The capacitor is initially uncharged, but starts to charge when the switch is closed. Initially the potential difference across the resistor is the battery emf, but that steadily drops (as does the current) as the potential difference across the capacitor increases.

Applying Kirchoff''s loop rule:

e - IR - Q/C = 0

As Q increases I decreases, but Q changes because there is a current I. As the current decreases Q changes more slowly.

I = dQ/dt, so the equation can be written:

e - R (dQ/dt) - Q/C = 0

This is a differential equation that can be solved for Q as a function of time. The solution (derived in the text) is:

Q(t) = Q_o [ 1 - e^-t/t ]

where Q_o = C e and the time constant t = RC.

Differentiating this expression to get the current as a function of time gives:

I(t) = (Q_o/RC) e^-t/t = I_o e^-t/t

where I_o = e/R is the maximum current possible in the circuit.

The time constant t = RC determines how quickly the capacitor charges. If RC is small the capacitor charges quickly; if RC is large the capacitor charges more slowly.

An RC Circuit: Discharging

What happens if the capacitor is now fully charged and is then discharged through the resistor? Now the potential difference across the resistor is the capacitor voltage, but that decreases (as does the current) as time goes by.

Applying Kirchoff''s loop rule:

-IR - Q/C = 0

I = dQ/dt, so the equation can be written:

R (dQ/dt) = -Q/C

This is a differential equation that can be solved for Q as a function of time. The solution is:

Q(t) = Q_o e^-t/t

where Q_o is the initial charge on the capacitor and the time constant t = RC.

Differentiating this expression to get the current as a function of time gives:

I(t) = -(Q_o/RC) e^-t/t = -I_o e^-t/t

where I_o = Q_o/RC

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RC circuit u can use as low pass filter , it means it alows low freqency signal and attenute high frequency signal . This is beacause of at low frequency take w = 0 reactance of capacitor is ∞  then in circuit it is open circuit total voltage drope across open circuit , if it is high frequecny w = ∞ , reactance is 0 so it is act as short circuit  so no voltage drop. reactance of capacitor is ( 1/( 2XπXfrequencyXcapacitance)) .

If you want about transient response RC circuit you can again ask me

            thank u

RC circuit mainly used as low pass filter. That means it allows only low frequency signals and attenuates for large frequencies.

This can be explained from the impedance of the capacitor: Xc = 1/(jwc) 

If the w increases the Xc decreases so influence of capacitor decreases.

It has particular  frequency at which its response attenuates, this frequency known as cut off frequency.

This you can observe experimentally  by CRO.