ROUTERA


Current Electricity

Class 12th Physics Chapter HOTs


Question 1:

Q: A current of 2 A flows through a conductor of length 10 cm and cross-sectional area 1mm21 \, \text{mm}^2 . The resistivity of the material of the conductor is 1.6×107Ωm1.6 \times 10^{-7} \, \Omega \, \text{m} . Calculate the potential difference across the conductor.

Solution:
Given:

  • Current, I=2AI = 2 \, \text{A}
  • Length, L=10cm=0.1mL = 10 \, \text{cm} = 0.1 \, \text{m}
  • Cross-sectional area, A=1mm2=1×106m2A = 1 \, \text{mm}^2 = 1 \times 10^{-6} \, \text{m}^2
  • Resistivity, ρ=1.6×107Ωm\rho = 1.6 \times 10^{-7} \, \Omega \, \text{m}

The resistance RR of the conductor is given by:

R=ρLAR = \frac{\rho L}{A}

Substitute the values:

R=(1.6×107)(0.1)1×106=0.016ΩR = \frac{(1.6 \times 10^{-7}) (0.1)}{1 \times 10^{-6}} = 0.016 \, \Omega

Now, use Ohm’s Law to find the potential difference:

V=IR=2×0.016=0.032VV = IR = 2 \times 0.016 = 0.032 \, \text{V}

Thus, the potential difference across the conductor is 0.032V0.032 \, \text{V} .


Question 2:

Q: Derive the expression for the drift velocity of charge carriers in a conductor.

Solution:
The drift velocity vdv_d of charge carriers in a conductor can be derived from the relationship between current, charge, and drift velocity.

  1. The current II is the flow of charge QQ per unit time, and the charge per unit time is:
I=Qt=nAvdqI = \frac{Q}{t} = n A v_d q

where:

  • nn = number of charge carriers per unit volume,
  • AA = cross-sectional area of the conductor,
  • vdv_d = drift velocity of the charge carriers,
  • qq = charge of an electron.
  1. Rearranging for vdv_d :
vd=InAqv_d = \frac{I}{n A q}

Thus, the drift velocity is vd=InAqv_d = \frac{I}{n A q} .


Question 3:

Q: A cell of emf EE and internal resistance rr is connected to a load resistance RR . Derive the expression for the power delivered to the load resistance RR .

Solution:
The total resistance in the circuit is the sum of the internal resistance and the load resistance:

Rtotal=R+rR_{\text{total}} = R + r

The current in the circuit is given by Ohm's Law:

I=ER+rI = \frac{E}{R + r}

The power delivered to the load resistance is:

P=I2RP = I^2 R

Substituting I=ER+rI = \frac{E}{R + r} :

P=(ER+r)2R=E2R(R+r)2P = \left( \frac{E}{R + r} \right)^2 R = \frac{E^2 R}{(R + r)^2}

Thus, the power delivered to the load resistance is P=E2R(R+r)2P = \frac{E^2 R}{(R + r)^2} .


Question 4:

Q: A conductor is stretched to twice its original length. How does its resistance change?

Solution:
The resistance RR of a conductor is given by:

R=ρLAR = \rho \frac{L}{A}

where:

  • ρ\rho is the resistivity of the material,
  • LL is the length of the conductor,
  • AA is the cross-sectional area of the conductor.

If the conductor is stretched to twice its original length, then:

  • New length, L=2LL' = 2L ,
  • New area, A=A2A' = \frac{A}{2} (since the volume remains constant, and A=A2A' = \frac{A}{2} ).

Thus, the new resistance RR' is:

R=ρLA=ρ2LA/2=4ρLA=4RR' = \rho \frac{L'}{A'} = \rho \frac{2L}{A/2} = 4 \cdot \rho \frac{L}{A} = 4R

Therefore, the resistance increases by a factor of 4.


Question 5:

Q: Explain the effect of temperature on the resistance of a conductor.

Solution:
The resistance RR of a conductor is temperature dependent. The relationship between resistance and temperature is given by the equation:

RT=R0(1+αT)R_T = R_0 (1 + \alpha T)

where:

  • RTR_T is the resistance at temperature TT ,
  • R0R_0 is the resistance at a reference temperature (usually 0°C),
  • α\alpha is the temperature coefficient of resistance,
  • TT is the temperature change from the reference temperature.

For most metals, the resistance increases with temperature due to increased collisions between charge carriers and atoms.


Question 6:

Q: Two resistors of resistances R1R_1 and R2R_2 are connected in parallel. Derive the expression for the equivalent resistance.

Solution:
For resistors in parallel, the reciprocal of the equivalent resistance ReqR_{\text{eq}} is the sum of the reciprocals of the individual resistances:

1Req=1R1+1R2\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2}

Thus, the equivalent resistance is:

Req=R1R2R1+R2R_{\text{eq}} = \frac{R_1 R_2}{R_1 + R_2}

Question 7:

Q: Derive the expression for the potential difference across a resistor in a series combination of resistors.

Solution:
In a series combination, the same current flows through all resistors. The total resistance in the series combination is:

Rtotal=R1+R2++RnR_{\text{total}} = R_1 + R_2 + \cdots + R_n

The potential difference VtotalV_{\text{total}} across the series combination is the sum of the potential differences across each resistor:

Vtotal=V1+V2++VnV_{\text{total}} = V_1 + V_2 + \cdots + V_n

Since V=IRV = IR , the potential difference across each resistor is:

Vi=IRiV_i = I R_i

Thus:

Vtotal=I(R1+R2++Rn)V_{\text{total}} = I(R_1 + R_2 + \cdots + R_n)

Question 8:

Q: A wire of resistance RR is bent into the shape of a circle. What is the effective resistance between two points on the wire that are diametrically opposite?

Solution:
When the wire is bent into a circle, the total resistance of the wire remains RR . The wire is divided into two equal halves, each with resistance R/2R/2 . Since the two halves are in parallel, the effective resistance ReffR_{\text{eff}} between the two opposite points is:

1Reff=1R/2+1R/2=4R\frac{1}{R_{\text{eff}}} = \frac{1}{R/2} + \frac{1}{R/2} = \frac{4}{R}

Thus:

Reff=R4R_{\text{eff}} = \frac{R}{4}

Question 9:

Q: Calculate the current flowing through a 10 Ω\Omega resistor when a 10 V battery is connected in series with it and a 5 Ω\Omega resistor.

Solution:
The total resistance in the circuit is:

Rtotal=10+5=15ΩR_{\text{total}} = 10 + 5 = 15 \, \Omega

The current in the circuit is:

I=VRtotal=1015=23AI = \frac{V}{R_{\text{total}}} = \frac{10}{15} = \frac{2}{3} \, \text{A}

Question 10:

Q: Derive the expression for the energy stored in a capacitor in terms of the potential difference and capacitance.

Solution:
The energy stored in a capacitor is the work done to charge it. The energy UU stored in a capacitor with charge QQ and potential difference VV is:

U=12QVU = \frac{1}{2} Q V

Using the relation Q=CVQ = C V , where CC is the capacitance, we get:

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

Thus, the energy stored in a capacitor is U=12CV2U = \frac{1}{2} C V^2 .


Question 11:

Q: A current of 2 A is flowing through a conductor. Calculate the drift velocity if the number density of electrons in the conductor is 8×1028m38 \times 10^{28} \, \text{m}^{-3} , and the cross-sectional area of the conductor is 106m210^{-6} \, \text{m}^2 .

Solution:
Using the formula for drift velocity:

vd=InAev_d = \frac{I}{n A e}

where:

  • I=2AI = 2 \, \text{A} ,
  • n=8×1028m3n = 8 \times 10^{28} \, \text{m}^{-3} ,
  • A=106m2A = 10^{-6} \, \text{m}^2 ,
  • e=1.6×1019Ce = 1.6 \times 10^{-19} \, \text{C} .

Substituting the values:

vd=2(8×1028)(106)(1.6×1019)v_d = \frac{2}{(8 \times 10^{28})(10^{-6})(1.6 \times 10^{-19})} vd=1.56×104m/sv_d = 1.56 \times 10^{-4} \, \text{m/s}

Thus, the drift velocity is 1.56×104m/s1.56 \times 10^{-4} \, \text{m/s} .


Question 12:

Q: A 6 V battery is connected in series with two resistors, 10 Ω\Omega and 5 Ω\Omega . Find the total power dissipated in the circuit.

Solution:
First, calculate the total resistance in the circuit:

Rtotal=10+5=15ΩR_{\text{total}} = 10 + 5 = 15 \, \Omega

Now, calculate the total current in the circuit using Ohm’s Law:

I=VRtotal=615=0.4AI = \frac{V}{R_{\text{total}}} = \frac{6}{15} = 0.4 \, \text{A}

Now, calculate the total power dissipated:

P=I2Rtotal=(0.4)2×15=0.16×15=2.4WP = I^2 R_{\text{total}} = (0.4)^2 \times 15 = 0.16 \times 15 = 2.4 \, \text{W}

Thus, the total power dissipated in the circuit is 2.4W2.4 \, \text{W} .


Question 13:

Q: Explain the phenomenon of "current leakage" in resistors and how it affects the overall resistance in a circuit.

Solution:
Current leakage refers to the unwanted loss of current from a conductor, often due to the presence of external factors such as humidity, temperature fluctuations, or insulation defects. This leads to an increase in effective resistance because the leakage path provides an alternative route for current flow, which diverts a portion of the current and reduces the efficiency of the circuit.

The leakage current creates an additional path for current, thus increasing the total resistance. In extreme cases, it can cause the circuit to behave unpredictably, reducing the current flowing through the intended load and causing potential safety hazards. Proper insulation and shielding are critical to preventing current leakage.


Question 14:

Q: Derive the relation for the electric field inside a uniformly charged spherical shell using Gauss's Law.

Solution: Gauss’s Law states that the electric flux through a closed surface is proportional to the charge enclosed within that surface:

ΦE=Qencϵ0\Phi_E = \frac{Q_{\text{enc}}}{\epsilon_0}

Consider a uniformly charged spherical shell with charge QQ and radius RR . Let the Gaussian surface be a sphere with radius rr inside the shell.

Since the charge is distributed uniformly on the shell, the electric field inside the shell at any point (where r<Rr < R ) is zero. This is because no charge is enclosed by the Gaussian surface inside the shell.

Therefore, by Gauss’s Law:

ΦE=EdA=Qencϵ0\Phi_E = \int \mathbf{E} \cdot d\mathbf{A} = \frac{Q_{\text{enc}}}{\epsilon_0}

Since there is no charge enclosed inside the spherical shell, Qenc=0Q_{\text{enc}} = 0 , so the electric flux is zero:

ΦE=0\Phi_E = 0

Thus, the electric field inside the shell is zero:

E=0E = 0

Question 15:

Q: A capacitor of capacitance C=4μFC = 4 \, \mu\text{F} is charged to a potential difference of 20V20 \, \text{V} . Calculate the energy stored in the capacitor.

Solution:
The energy stored in a capacitor is given by the formula:

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

Substitute the given values:

U=12×4×106×(20)2U = \frac{1}{2} \times 4 \times 10^{-6} \times (20)^2 U=12×4×106×400=800×106J=0.8mJU = \frac{1}{2} \times 4 \times 10^{-6} \times 400 = 800 \times 10^{-6} \, \text{J} = 0.8 \, \text{mJ}

Thus, the energy stored in the capacitor is 0.8mJ0.8 \, \text{mJ} .


Question 16:

Q: Explain the concept of "Kirchhoff's loop rule" and apply it to calculate the current in a circuit consisting of three resistors in series.

Solution: Kirchhoff’s loop rule states that the sum of the potential differences (voltages) around any closed loop or circuit is always zero:

V=0\sum V = 0

Consider a circuit with three resistors in series, R1R_1 , R2R_2 , and R3R_3 , connected to a battery with emf EE . The current II flows through all resistors, so the total voltage drop across the resistors should equal the emf of the battery.

The voltage drop across each resistor is given by Ohm's Law:

V1=IR1,V2=IR2,V3=IR3V_1 = I R_1, \quad V_2 = I R_2, \quad V_3 = I R_3

Using Kirchhoff's loop rule:

E=I(R1+R2+R3)E = I (R_1 + R_2 + R_3)

Solving for the current II :

I=ER1+R2+R3I = \frac{E}{R_1 + R_2 + R_3}

Thus, the current in the circuit is ER1+R2+R3\frac{E}{R_1 + R_2 + R_3} .


Question 17:

Q: How does the resistance of a conductor depend on the temperature? Derive the expression for the change in resistance with temperature.

Solution: The resistance of a conductor depends on temperature according to the equation:

RT=R0(1+αT)R_T = R_0 (1 + \alpha T)

where:

  • RTR_T is the resistance at temperature TT ,
  • R0R_0 is the resistance at reference temperature (usually 0C0^\circ C ),
  • α\alpha is the temperature coefficient of resistance,
  • TT is the temperature change from 0C0^\circ C .

This equation indicates that the resistance increases linearly with temperature for most metallic conductors.


Question 18:

Q: Two capacitors of capacitance 5μF5 \, \mu\text{F} and 10μF10 \, \mu\text{F} are connected in series across a 12V12 \, \text{V} battery. Calculate the equivalent capacitance of the combination.

Solution: For capacitors in series, the reciprocal of the equivalent capacitance CeqC_{\text{eq}} is the sum of the reciprocals of the individual capacitances:

1Ceq=1C1+1C2\frac{1}{C_{\text{eq}}} = \frac{1}{C_1} + \frac{1}{C_2}

Substitute the given values:

1Ceq=15+110=210+110=310\frac{1}{C_{\text{eq}}} = \frac{1}{5} + \frac{1}{10} = \frac{2}{10} + \frac{1}{10} = \frac{3}{10} Ceq=103=3.33μFC_{\text{eq}} = \frac{10}{3} = 3.33 \, \mu\text{F}

Thus, the equivalent capacitance is 3.33μF3.33 \, \mu\text{F} .


Question 19:

Q: A wire of resistance 10Ω10 \, \Omega is stretched to double its length. What is the new resistance of the wire?

Solution: When a wire is stretched, its length LL becomes twice the original length. The resistance RR of a wire is given by:

R=ρLAR = \rho \frac{L}{A}

where:

  • ρ\rho is the resistivity of the material,
  • LL is the length,
  • AA is the cross-sectional area.

If the length is doubled, the cross-sectional area AA becomes halved (because the volume of the wire remains constant). Thus, the new resistance is:

R=ρ2LA/2=4RR' = \rho \frac{2L}{A/2} = 4R

Therefore, the new resistance is 4×10=40Ω4 \times 10 = 40 \, \Omega .


Question 20:

Q: A current of 3 A flows through a conductor of length 2 m and cross-sectional area 1mm21 \, \text{mm}^2 . If the resistivity of the material is 2×107Ωm2 \times 10^{-7} \, \Omega \, \text{m} , calculate the potential difference across the conductor.

Solution: The resistance RR of the conductor is given by:

R=ρLAR = \frac{\rho L}{A}

Substitute the given values:

R=(2×107)(2)1×106=0.4ΩR = \frac{(2 \times 10^{-7}) (2)}{1 \times 10^{-6}} = 0.4 \, \Omega

Now, using Ohm’s Law, the potential difference VV across the conductor is:

V=IR=3×0.4=1.2VV = IR = 3 \times 0.4 = 1.2 \, \text{V}

Thus, the potential difference is 1.2V1.2 \, \text{V} .


Question 21:

Q: Explain the concept of "superconductivity" and its significance in practical applications.

Solution: Superconductivity is a phenomenon in which certain materials, at very low temperatures, exhibit zero electrical resistance. This means that once an electrical current is established in a superconducting material, it can flow indefinitely without any energy loss.

The significance of superconductivity lies in its potential applications, such as in the development of highly efficient power transmission lines, powerful magnets for MRI machines, and advanced particle accelerators. However, the requirement for extremely low temperatures (near absolute zero) currently limits its widespread use.


Question 22:

Q: A wire of resistance RR is bent into a circular loop. Find the effective resistance between two points on the wire when the loop is connected to a battery.

Solution: When a wire is bent into a circular loop, the resistance between two points is equivalent to two resistors (half the length each) connected in parallel. Each half of the loop has resistance R/2R/2 .

Thus, the effective resistance between the two points is:

Reff=R/2×R/2R/2+R/2=R4R_{\text{eff}} = \frac{R/2 \times R/2}{R/2 + R/2} = \frac{R}{4}

Thus, the effective resistance between the two points is R/4R/4 .


Question 23:

Q: Derive the expression for the time constant of an RC circuit and explain its significance.

Solution: The time constant τ\tau of an RC circuit is given by:

τ=RC\tau = R C

This represents the time required for the charge on the capacitor to either charge up to 63% of its maximum value or discharge to 37% of its initial value.

Significance: The time constant determines the speed of charging and discharging of a capacitor in an RC circuit. A larger time constant means slower charging/discharging.


Question 24:

Q: A battery of emf 12 V is connected in series with two resistors 4Ω4 \, \Omega and 8Ω8 \, \Omega . Find the current in the circuit and the potential difference across each resistor.

Solution: The total resistance in the circuit is:

Rtotal=4+8=12ΩR_{\text{total}} = 4 + 8 = 12 \, \Omega

Now, calculate the total current using Ohm’s Law:

I=VRtotal=1212=1AI = \frac{V}{R_{\text{total}}} = \frac{12}{12} = 1 \, \text{A}

Now, calculate the potential difference across each resistor:

V1=IR1=1×4=4V,V2=IR2=1×8=8VV_1 = IR_1 = 1 \times 4 = 4 \, \text{V}, \quad V_2 = IR_2 = 1 \times 8 = 8 \, \text{V}

Thus, the current is 1A1 \, \text{A} , and the potential differences are 4V4 \, \text{V} across 4Ω4 \, \Omega and 8V8 \, \text{V} across 8Ω8 \, \Omega .


Question 25:

Q: What is the effect of temperature on the resistance of a thermistor? Derive the relationship between the resistance and temperature for a thermistor.

Solution: A thermistor is a type of resistor whose resistance changes significantly with temperature. Unlike ordinary resistors, thermistors have a negative temperature coefficient (NTC) or positive temperature coefficient (PTC), meaning their resistance decreases or increases with temperature, respectively.

For an NTC thermistor, the relationship between resistance RR and temperature TT is given by the equation:

R(T)=R0exp(Eak(1T1T0))R(T) = R_0 \exp\left(\frac{-E_a}{k} \left(\frac{1}{T} - \frac{1}{T_0}\right)\right)

Where:

  • R0R_0 is the resistance at reference temperature T0T_0 ,
  • EaE_a is the activation energy of the material,
  • kk is the Boltzmann constant,
  • TT is the temperature in Kelvin.

This equation shows that as the temperature increases, the resistance of an NTC thermistor decreases exponentially.


Question 26:

Q: A battery of emf 12V is connected in parallel with two resistors of 4Ω4 \, \Omega and 6Ω6 \, \Omega . Calculate the total current in the circuit and the current through each resistor.

Solution: For resistors connected in parallel, the equivalent resistance ReqR_{\text{eq}} is given by:

1Req=1R1+1R2\frac{1}{R_{\text{eq}}} = \frac{1}{R_1} + \frac{1}{R_2}

Substitute the values:

1Req=14+16=312+212=512\frac{1}{R_{\text{eq}}} = \frac{1}{4} + \frac{1}{6} = \frac{3}{12} + \frac{2}{12} = \frac{5}{12} Req=125=2.4ΩR_{\text{eq}} = \frac{12}{5} = 2.4 \, \Omega

Now, calculate the total current using Ohm’s Law:

I=VReq=122.4=5AI = \frac{V}{R_{\text{eq}}} = \frac{12}{2.4} = 5 \, \text{A}

Now, calculate the current through each resistor using Ohm’s Law:

I1=VR1=124=3A,I2=VR2=126=2AI_1 = \frac{V}{R_1} = \frac{12}{4} = 3 \, \text{A}, \quad I_2 = \frac{V}{R_2} = \frac{12}{6} = 2 \, \text{A}

Thus, the total current is 5A5 \, \text{A} , with 3A3 \, \text{A} through 4Ω4 \, \Omega and 2A2 \, \text{A} through 6Ω6 \, \Omega .


Question 27:

Q: How does the energy stored in a capacitor change when it is connected to a battery of higher voltage? Derive the expression for the energy stored in a capacitor.

Solution: The energy stored in a capacitor is given by the formula:

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

Where:

  • UU is the energy stored,
  • CC is the capacitance,
  • VV is the voltage across the capacitor.

If the voltage across the capacitor increases, the energy stored in the capacitor increases exponentially with the square of the voltage. For example, if the voltage is doubled, the energy stored increases by a factor of four.

Thus, if the capacitor is connected to a battery with higher voltage, the energy stored in the capacitor increases as the square of the applied voltage.


Question 28:

Q: A current of 5 A flows through a conductor of length 3 m and cross-sectional area 1mm21 \, \text{mm}^2 . If the resistivity of the material is 1.5×107Ωm1.5 \times 10^{-7} \, \Omega \, \text{m} , calculate the potential difference across the conductor.

Solution: The resistance RR of the conductor is given by:

R=ρLAR = \rho \frac{L}{A}

Substitute the given values:

R=(1.5×107)(3)1×106=0.45ΩR = \frac{(1.5 \times 10^{-7}) (3)}{1 \times 10^{-6}} = 0.45 \, \Omega

Now, using Ohm’s Law, the potential difference VV across the conductor is:

V=IR=5×0.45=2.25VV = I R = 5 \times 0.45 = 2.25 \, \text{V}

Thus, the potential difference across the conductor is 2.25V2.25 \, \text{V} .


Question 29:

Q: A battery of emf 10 V is connected in series with two resistors of 2Ω2 \, \Omega and 4Ω4 \, \Omega . Calculate the power dissipated in the circuit.

Solution: The total resistance in the circuit is:

Rtotal=2+4=6ΩR_{\text{total}} = 2 + 4 = 6 \, \Omega

Now, calculate the total current in the circuit using Ohm’s Law:

I=VRtotal=106=1.67AI = \frac{V}{R_{\text{total}}} = \frac{10}{6} = 1.67 \, \text{A}

Now, calculate the power dissipated in the circuit using the formula P=I2RtotalP = I^2 R_{\text{total}} :

P=(1.67)2×6=2.78×6=16.68WP = (1.67)^2 \times 6 = 2.78 \times 6 = 16.68 \, \text{W}

Thus, the power dissipated in the circuit is approximately 16.68W16.68 \, \text{W} .


Question 30:

Q: A battery of emf 24V is connected to a series combination of two resistors, 6Ω6 \, \Omega and 12Ω12 \, \Omega . What will be the potential difference across the 6 Ω\Omega resistor?

Solution: The total resistance in the series combination is:

Rtotal=6+12=18ΩR_{\text{total}} = 6 + 12 = 18 \, \Omega

Now, calculate the total current in the circuit using Ohm’s Law:

I=VRtotal=2418=1.33AI = \frac{V}{R_{\text{total}}} = \frac{24}{18} = 1.33 \, \text{A}

Now, calculate the potential difference across the 6 Ω\Omega resistor using Ohm’s Law:

V1=IR1=1.33×6=8VV_1 = I R_1 = 1.33 \times 6 = 8 \, \text{V}

Thus, the potential difference across the 6 Ω\Omega resistor is 8V8 \, \text{V} .