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Electrostatic Potential And Capacitance

Question
CBSEENPH12038011

An alternating emf is applied across a capacitor. Show mathematically that current in it leads the applied emf by a phase angle of π/2. What is its capacitive reactance ? Draw a graph showing the variation of capacitive reactance with the frequency of the a.c. source. 

Solution
Let an alternating emf, E = E0 sin ωt is applied across a capacitor of capacitance C.
The current flowing in the circuit transfers charge to the plates of the capacitor due to which a potential difference develops across its plates. Also, assume that 'q' be the charge on each plate of the capacitor at any instant t.

Therefore, potential difference across the plates of capacitor,
                         V = qC.

At every instant potential difference V must be equal to the applied emf. 

i.e.,      V = qC = E = E0 sin  ωt     ...(i) V = E =E0 sin ωt

           q = CE0 sin ωt 

 Instantaneous current,

           I  =dqdt = ddt (CE0 sin ωt)               = CE0 cos ωt.ω  

           I = E01ωC sin ωt+π2       ...(ii) sin θ + π2 = cos θ 

The current is maximum, i.e., I  = I0 when

                sin ωt+π2 = 1 

From equation (i),

I0 = E01ωC×1 = E01ωC                ...(iii) 

Putting in equation (ii), we get 

I = I0 sin  ωt + π2 

Comparing equations (i) and (iii), we see that in an a.c. circuit containing capacitor only, current leads the emf by a phase angle of  π/2

Comparing (iii) with I0 = E0/R, we find 1/ωC is the effective resistance of the capacitive a.c. circuit. It is called capacitive reactance. 

i.e., χC = 1ωC = 12πfC.

Fig. Variation of capacitive reactance with frequency.


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