Q 1 :    

A parallel plate capacitor made of circular plates is being charged such that the surface charge density on its plates is increasing at a constant rate with time. The magnetic field arising due to displacement current is        [2025]

  • non-zero everywhere with maximum at the imaginary cylindrical surface connecting peripheries of the plates

     

  • zero between the plates and non-zero outside

     

  • zero at all places

     

  • constant between the plates and zero outside the plates.

     

(1)

The magnetic field arising due to displacement current is non zero everywhere with maximum at the imaginary cylindrical surface connecting peripheries of the plates. This is because the displacement current is strongest there, where the changing electric field is most concentrated.

 



Q 2 :    

A parallel plate capacitor is charged by connecting it to a battery through a resistor. If I is the current in the circuit, then in the gap between the plates          [2024]

  • there is no current.

     

  • displacement current of magnitude equal to I flows in the same direction as I.

     

  • displacement current of magnitude equal to I flows in a direction opposite to that of I.

     

  • displacement current of magnitude greater than I flows but can be in any direction.

     

(2)

Displacement current is equal to the conduction current and flows from positive plate towards negative plate in the direction of conduction current.

 



Q 3 :    

To produce an instantaneous displacement current of 2 mA in the space between the parallel plates of a capacitor of capacitance 4 μF, the rate of change of applied variable potential difference (dVdt) must be            [2023]
 

  • 800 V/s

     

  • 500 V/s

     

  • 200 V/s

     

  • 400 V/s

     

(2)

Displacement current, ID=ε0dϕEdt=ε0ddt(EA)

=ε0Addt(Vd)  or  ID=ε0AddVdt

  ID=CdVdt  or  dVdt=IDC

Given, ID=2mA=2×10-3A; C=4×10-6F

So, dVdt=2×10-34×10-6=500V/s



Q 4 :    

An AC source is connected to a capacitor C. Due to decrease in its operating frequency            [2023]

  • displacement current decreases

     

  • capacitive reactance remains constant

     

  • capacitive reactance decreases

     

  • displacement current increases

     

(1)

Capacitive inductance, XC=12πfC

As frequency decreases, XC increases.

[IMAGE 264]------------------------------

So, conduction current decreases. Hence, displacement current decreases.



Q 5 :    

A capacitor of capacitance 'C', is connected across an AC source of voltage V, given by 

V=V0sinωt

The displacement current between the plates of the capacitor, would then be given by                   [2021]

  • Id=V0ωCsinωt

     

  • Id=V0ωCcosωt

     

  • Id=V0ωCcosωt

     

  • Id=V0ωCsinωt

     

(2)

The instantaneous voltage, V=V0sinωt                    ...(i)

Displacement current is given by

id=CdVdt                                                                    ...(ii)

id=Cddt(V0sinωt)    id=CV0ωcosωt



Q 6 :    

A parallel plate capacitor of capacitance 20 μF is being charged by a voltage source whose potential is changing at the rate of 3 V/s. The conduction current through the connecting wires, and the displacement current through the plates of the capacitor, would be, respectively        [2019]

  • zero, zero

     

  • zero, 60 μA

     

  • 60 μA, 60 μA

     

  • 60 μA, zero

     

(3)

Here, C=20μF

The rate of change of potential, dVdt=3V/s

The charge on the capacitor, Q=CV

  dQdt=ID=CdVdt=20μF×3Vs=60μA

Displacement current is equal to the conduction current.



Q 7 :    

A 100 Ω resistance and a capacitor of 100 Ω reactance are connected in series across a 220 V source. When the capacitor is 50% charged, the peak value of the displacement current is              [2016]

  • 2.2 A

     

  • 11 A

     

  • 4.4 A

     

  • 112A

     

(1)

Here, R=100Ω,  XC=100Ω

Net impedance, Z=R2+XC2=1002Ω

Peak value of displacement current = Maximum conduction current in the circuit

=ε0Z=22021002=2.2A