Capacitor

NEET Physics · 98 questions · Page 1 of 10 · Click an option or "Show Solution" to reveal answer

Q1
Five capacitors of capacitances C1=C2=C3=C4=10μ FC_1=C_2=C_3=C_4=10 \mu \mathrm{~F} and C5=2.5μ FC_5=2.5 \mu \mathrm{~F} are connected as shown, along with a battery of 50 V . The equivalent capacitance and the charges on each capacitor respectively are:
A 5μ F,125μC5 \mu \mathrm{~F}, 125 \mu \mathrm{C} on C1C_1 to C4C_4 and 25μC25 \mu \mathrm{C} on C5C_5
B 5μ F,125μC5 \mu \mathrm{~F}, 125 \mu \mathrm{C} on all capacitors
C 5μ F,250μC5 \mu \mathrm{~F}, 250 \mu \mathrm{C} on all capacitors
D 4μ F,250μC4 \mu \mathrm{~F}, 250 \mu \mathrm{C} on C1C_1 to C4C_4 and 125μC125 \mu \mathrm{C} on C5C_5
Correct Answer
Option B
Solution
Ceq=2.5+2.5=5μ Fˋq1=q2=q3=q4=2.5×50=125μCq5=2.5×50=125μC\begin{aligned} & C_{\mathrm{eq}}=2.5+2.5=5 \mu \mathrm{~F}^ˋ \\ & q_1=q_2=q_3=q_4=2.5 \times 50=125 \mu \mathrm{C} \\ & q_5=2.5 \times 50=125 \mu \mathrm{C} \end{aligned}
Q2
Consider two uncharged capacitors of equal capacitance 200 pF . One of them is charged by a 100 V supply and disconnected. Now this capacitor is connected to the uncharged capacitor. The amount of electrostatic energy lost in the process is:
A 0.5×106 J0.5 \times 10^{-6} \mathrm{~J}
B 1.0 J
C 1.0×106 J1.0 \times 10^{-6} \mathrm{~J}
D 0.5 J
Correct Answer
Option A
Solution

Energy loss =12C1C2C1+C2V2=\dfrac{1}{2} \dfrac{C_1 C_2}{C_1+C_2} V^2

=12(200×200400)×1012(100)2=12×106×1012=0.5×106 J\begin{aligned} & =\frac{1}{2}\left(\frac{200 \times 200}{400}\right) \times 10^{-12}(100)^2 \\ & =\frac{1}{2} \times 10^6 \times 10^{-12}=0.5 \times 10^{-6} \mathrm{~J} \end{aligned}
Q3
The plates of a parallel plate capacitor are separated by dd. Two slabs of different dielectric constant K1K_1 and K2K_2 with thickness 38d\dfrac{3}{8} d and d2\dfrac{d}{2}, respectively are inserted in the capacitor. Due to this, the capacitance becomes two times larger than when there is nothing between the plates. If K1=1.25K2K_1=1.25 K_2, the value of K1K_1 is:
A 1.60
B 1.33
C 2.66
D 2.33
Correct Answer
Option C
Solution

Using Ceq=ε0At1K1+t2K2+t3K3C_{e q}=\dfrac{\varepsilon_0 A}{\dfrac{t_1}{K_1}+\dfrac{t_2}{K_2}+\dfrac{t_3}{K_3}} here C0=ε0Ad,t1=3d8,t2=d2,t3=d8C_0=\dfrac{\varepsilon_0 A}{d}, t_1=\dfrac{3 d}{8}, t_2=\dfrac{d}{2}, t_3=\dfrac{d}{8}

K1=K1,K2=K11.25 and K3=1K_1=K_1, \quad K_2=\frac{K_1}{1.25} \text{ and } K_3=1

Given Ceq =2C0C_{\text{eq }}=2 C_0

2C0=ε0A3d8k1+d×1.252k1+d82ε0Ad=ε0A3d8k1+d2k1×54+d82=138k1+58k1+18k1=83=2.66\begin{aligned} & \Rightarrow 2 C_0=\frac{\varepsilon_0 A}{\frac{3 d}{8 k_1}+\frac{d \times 1.25}{2 k_1}+\frac{d}{8}} \\ & \Rightarrow \frac{2 \varepsilon_0 A}{d}=\frac{\varepsilon_0 A}{\frac{3 d}{8 k_1}+\frac{d}{2 k_1} \times \frac{5}{4}+\frac{d}{8}} \\ & \Rightarrow 2=\frac{1}{\frac{3}{8 k_1}+\frac{5}{8 k_1}+\frac{1}{8}} \Rightarrow k_1=\frac{8}{3}=2.66 \end{aligned}
Q4
A 12 pF12 \mathrm{~pF} capacitor is connected to a 50 V50 \mathrm{~V} battery, the electrostatic energy stored in the capacitor in nJ\mathrm{nJ} is
A 15
B 7.5
C 0.3
D 150
Correct Answer
Option A
Solution

The electrostatic energy stored in a capacitor can be calculated using the formula:

U=12CV2U = \frac{1}{2} C V^2

Where:

UU

is the stored energy in joules (J)

CC

is the capacitance in farads (F)

VV

is the voltage in volts (V) Given:

C=12 pFC = 12 \mathrm{~pF}

(which is

12×101212 \times 10^{-12}

F)

V=50 VV = 50 \mathrm{~V}

Substitute the values into the formula:

U=12×12×1012×(50)2U = \frac{1}{2} \times 12 \times 10^{-12} \times (50)^2

Calculate the values inside the parentheses first:

502=250050^2 = 2500

Now substitute this back into the equation:

U=12×12×1012×2500U = \frac{1}{2} \times 12 \times 10^{-12} \times 2500

Perform the multiplication:

U=12×30000×1012U = \frac{1}{2} \times 30000 \times 10^{-12}

Which simplifies to:

U=15000×1012U = 15000 \times 10^{-12}

Convert this to nanojoules (nJ) by recognizing that

1 nJ=109 J1 \mathrm{~nJ} = 10^{-9} \mathrm{~J}

:

U=15 nJU = 15 \mathrm{~nJ}

Thus, the electrostatic energy stored in the capacitor is: Option A: 15 nJ

Q5
The capacitance of a capacitor with charge qq and a potential difference VV depends on
A both qq and VV
B the geometry of the capacitor
C qq only
D VV only
Correct Answer
Option B
Solution

The correct answer is Option B: the geometry of the capacitor .

Here's why: Capacitance (denoted by *C*) is a fundamental property of a capacitor that describes its ability to store electrical energy.

It's defined by the ratio of the charge stored on the capacitor ( q ) to the potential difference across its plates ( V ):

C=qVC = \frac{q}{V}

While the formula seems to suggest that capacitance depends on both charge and voltage, the reality is that the geometry of the capacitor determines its capacitance.

Here's a breakdown: Charge ( q ) : The charge stored on a capacitor is directly proportional to the applied voltage.

If you increase the voltage, you increase the charge stored.

However, the capacitance itself remains constant for a given capacitor.

Voltage ( V ) : Similarly, the voltage across a capacitor is directly proportional to the charge stored.

Increasing the charge increases the voltage, but again, the capacitance remains unchanged.

Geometry : The geometry of a capacitor dictates how much electric field is created between its plates for a given charge.

This electric field determines the potential difference between the plates.

Here are some key factors: Area of plates (A) : Larger plates can hold more charge for a given voltage, resulting in higher capacitance.

Distance between plates (d) : Smaller distances between plates create a stronger electric field, which leads to higher capacitance.

Dielectric material : The material between the plates (dielectric) affects the strength of the electric field and therefore the capacitance.

A material with a higher dielectric constant increases the capacitance.

In summary, while charge and voltage are related to capacitance through the formula, they are not the determining factors.

It's the capacitor's physical characteristics – its geometry – that ultimately determine its capacitance.

Q6
The steady state current in the circuit shown below is :
A 0.67 A
B 1.5 A
C 2 A
D 1 A
Correct Answer
Option C
Solution

At steady state, capacitor will be completely charged and will not allow current to pass through it.

The simplified circuit will be :

i=VRi=102+3=2 Ai=\frac{V}{R} \Rightarrow i=\frac{10}{2+3}=2 \mathrm{~A}
Q7
In the following circuit, the equivalent capacitance between terminal A and terminal B is :
A 2 μ\muF
B 1 μ\muF
C 0.5 μ\muF
D 4 μ\muF
Correct Answer
Option A
Solution

Given circuit is balanced Wheatstone bridge

CAB=1+1=2μF\begin{aligned} C_{A B} & =1+1 \\ & =2 \mu F \end{aligned}
Q8
The equivalent capacitance of the arrangement shown in figure is:
A 30 μ\muF
B 15 μ\muF
C 25 μ\muF
D 20 μ\muF
Correct Answer
Option D
Solution
Ceq=5+15=20μFC_{eq}=5+15=20\mu F
Q9
To produce an instantaneous displacement current of 2 mA2 \mathrm{~mA} in the space between the parallel plates of a capacitor of capacitance 4 μF4 ~\mu \mathrm{F}, the rate of change of applied variable potential difference (dVdt)\left(\dfrac{\mathrm{dV}}{\mathrm{dt}}\right) must be :-
A 800 V/s800 \mathrm{~V} / \mathrm{s}
B 500 V/s500 \mathrm{~V} / \mathrm{s}
C 200 V/s200 \mathrm{~V} / \mathrm{s}
D 400 V/s400 \mathrm{~V} / \mathrm{s}
Correct Answer
Option B
Solution
Q=CVdQdt=CdVdtdVdt=IC=2×1034×106=1032=500Vs\begin{aligned} & \mathrm{Q}=\mathrm{CV} \\\\ & \begin{aligned} \frac{\mathrm{dQ}}{\mathrm{dt}}=\mathrm{C} \cdot \frac{\mathrm{dV}}{\mathrm{dt}} \Rightarrow \frac{\mathrm{dV}}{\mathrm{dt}} & =\frac{\mathrm{I}}{\mathrm{C}}=\frac{2 \times 10^{-3}}{4 \times 10^{-6}} \\ & =\frac{10^3}{2}=500 \frac{\mathrm{V}}{\mathrm{s}} \end{aligned} \end{aligned}
Q10
The equivalent capacitance of the system shown in the following circuit is:
A 3μ\muF
B 6μ\muF
C 9μ\muF
D 2μ\muF
Correct Answer
Option D
Solution
CAB=3×63+6=2μF\mathrm{C_{AB}=\frac{3\times6}{3+6}=2\mu F}
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