Does the Impedance of a Capacitor Affect AC Circuits?

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In a purely capacitive AC circuit, the relationship between current and voltage is defined by Im = Vm * ω * C, where Im is the amplitude of current and Vm is the amplitude of voltage. Voltage lags behind current by a phase difference of π/2 radians, leading to the equations I = Im sin(ωt + π/2) and V = Vm sin(ωt). Kirchhoff's Loop Rule is applied to derive the relationship between charge and current, resulting in the conclusion that Vm = Im * ω/C. The discussion highlights a correction in the integration process, emphasizing that the impedance of a capacitor affects AC circuits by introducing a factor of 1/ωC, which impedes the AC flow. The analysis confirms that the impedance plays a crucial role in the behavior of capacitive circuits.
Prashasti
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In a purely capacitive ac circuit, we get,
Im = Vm*ω*C, ...(1)
Where, Im = Amplitude of the current
Vm = Amplitude of the voltage

Now, what I think is,
We know that in a purely capacitive circuit, voltage lags behind current by a phase difference of ∏/2 rad. So, at any time 't',
I = Im sin(ωt+∏/2)
V = Vm sinωt

Using Kirchhoff's Loop Rule,

V = Vmsinωt = q/C

Where q = charge on the capacitor at time 't',

To find the current, I = dq/dt,
dq = Idt,

q = ∫Idt

q = ∫Imcosωt dt
q = Im∫cosωt dt
q = Im*ω*sinωt

So, Vmsinωt = Im*ω*sinωt /C
Vm = Im*ω/C

Im = Vm*C/ω, which is apparently, not equal to equation (1).

Am I wrong in my approach?
 
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Have you applied a result to a situation where it does not occur.
If there is no resistance in the circuit, then the voltage across the capacitor is going to be the same as the applied voltage - instantly. Draw the circuit diagram and see.
 
q = Im∫cosωt dt
q = Im*ω*sinωt

this is wrong..

q = (Im/ω)*sinωt.. You are integrating. remember not differentiating.
Vm = Im*ω/C

So this becomes

Vm = Im*1/ωC

compare this to V = IR

so 1/ωC plays the role of impeding the AC.
 
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It may be shown from the equations of electromagnetism, by James Clerk Maxwell in the 1860’s, that the speed of light in the vacuum of free space is related to electric permittivity (ϵ) and magnetic permeability (μ) by the equation: c=1/√( μ ϵ ) . This value is a constant for the vacuum of free space and is independent of the motion of the observer. It was this fact, in part, that led Albert Einstein to Special Relativity.
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