CBSE Class 12 Physics: Current Electricity NCERT Solutions (Chapter 3)

NCERT Solutions PDF Class 12 PDF

This resource provides detailed NCERT Solutions for Class 12 Physics, Chapter 3: Current Electricity, focusing on additional exercises. It covers complex problems involving the calculation of time required to neutralize the Earth's surface charge, considering its surface charge density and the global atmospheric current. It also delves into the characteristics of secondary cells, including calculating the current drawn and terminal voltage when cells are connected in series to a load resistance, and determining the maximum current a used cell can supply and its suitability for starting a car. These solutions offer step-by-step explanations, helping students understand the application of fundamental principles like Ohm's law and charge conservation in real-world and theoretical scenarios. They are designed to aid students in grasping the concepts thoroughly and preparing effectively for their board examinations by providing clear, accurate, and well-explained answers to challenging problems.

Quick info

BoardCBSE
ClassClass 12
SubjectPhysics
Session2026
LanguageEnglish
TypeNCERT Solutions
ChapterChapter 3: Current Electricity - NCERT Additional Exercises Solutions

Chapter summary

This chapter's NCERT Solutions for Class 12 Physics focus on additional exercises related to Current Electricity. It includes problems on calculating the time for neutralization of Earth's surface charge using its surface charge density and global current. It also covers series combinations of secondary cells, calculating total emf, internal resistance, current drawn, and terminal voltage. Furthermore, it addresses the maximum current from a single aged cell and its practical limitations, like starting a car motor. These solutions reinforce concepts of electric current, resistance, and cell behavior.

Learning outcomes

  • Calculate the time required to neutralize the Earth's surface charge.
  • Determine the total emf and internal resistance of cells connected in series.
  • Calculate the current drawn from a battery of secondary cells.
  • Compute the terminal voltage of a battery under load.
  • Find the maximum current that can be drawn from a secondary cell.
  • Analyze the suitability of a cell for high-current applications like starting a car.

Topics covered

Paper topics

  • Earth's surface charge density
  • Global atmospheric current
  • Time for neutralization
  • Secondary cells
  • Emf of cells
  • Internal resistance
  • Cells in series
  • Terminal voltage
  • Maximum current from a cell
  • Application of cells (car starter motor)

Important topics

  • Cells in series combination
  • Terminal voltage calculation
  • Maximum current from a cell
  • Earth's surface charge and neutralization time
  • Internal resistance effects

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Questions and Solutions

Question 3.14

The earth's surface has a negative surface charge density of $10^{-9}$ C m$^{-2}$. The potential difference of 400 kV between the top of the atmosphere and the surface results (due to the low conductivity of the lower atmosphere) in a current of only 1800 A over the entire globe. If there were no mechanism of sustaining atmospheric electric field, how much time (roughly) would be required to neutralise the earth's surface? (This never happens in practice because there is a mechanism to replenish electric charges, namely the continual thunderstorms and lightning in different parts of the globe). (Radius of earth = $6.37 \times 10^6$ m.)
Solution:

We are given the following information:

  • Surface charge density of the earth, $\sigma = 10^{-9} \text{ C m}^{-2}$
  • Current over the entire globe, $I = 1800 \text{ A}$
  • Radius of the earth, $r = 6.37 \times 10^6 \text{ m}$

First, we calculate the total surface area of the Earth, which is a sphere:

A = 4\pi r^2

Substituting the given radius:

A = 4\pi \times (6.37 \times 10^6 \text{ m})^2

A \approx 5.09 \times 10^{14} \text{ m}^2

Next, we find the total charge ($q$) on the Earth's surface using the surface charge density:

q = \sigma \times A

q = (10^{-9} \text{ C m}^{-2}) \times (5.09 \times 10^{14} \text{ m}^2)

q = 5.09 \times 10^{5} \text{ C}

The time ($t$) required to neutralize this charge is given by the relationship between current, charge, and time ($I = q/t$). We can rearrange this to solve for time:

t = \frac{q}{I}

Now, we substitute the values of total charge and global current:

t = \frac{5.09 \times 10^{5} \text{ C}}{1800 \text{ A}}

t \approx 282.77 \text{ seconds}

Therefore, the time required to neutralize the Earth's surface, under these hypothetical conditions, is approximately 282.77 seconds.

Question 3.15

(a) Six lead-acid type of secondary cells each of emf 2.0 V and internal resistance $0.015~\Omega$ are joined in series to provide a supply to a resistance of 8.5 $\Omega$. What are the current drawn from the supply and its terminal voltage?
Solution:

We are given:

  • Number of secondary cells, $n = 6$
  • Emf of each cell, $E = 2.0 \text{ V}$
  • Internal resistance of each cell, $r = 0.015 \Omega$
  • External resistance, $R = 8.5 \Omega$

When cells are connected in series, the total emf is the sum of individual emfs, and the total internal resistance is the sum of individual internal resistances.

Total emf of the combination:

E_{total} = n \times E = 6 \times 2.0 \text{ V} = 12.0 \text{ V}

Total internal resistance of the combination:

r_{total} = n \times r = 6 \times 0.015 \Omega = 0.09 \Omega

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

R_{circuit} = R + r_{total} = 8.5 \Omega + 0.09 \Omega = 8.59 \Omega

The current drawn from the supply ($I$) is given by Ohm's law applied to the entire circuit:

I = \frac{E_{total}}{R_{circuit}} = \frac{12.0 \text{ V}}{8.59 \Omega}

I \approx 1.39 \text{ A}

The terminal voltage ($V$) of the battery is the voltage across the external resistance $R$. It can be calculated as:

V = I \times R = 1.39 \text{ A} \times 8.5 \Omega

V \approx 11.87 \text{ V}

Alternatively, the terminal voltage can be calculated as the total emf minus the voltage drop across the internal resistance: $V = E_{total} - I \times r_{total} = 12.0 \text{ V} - (1.39 \text{ A} \times 0.09 \Omega) \approx 12.0 \text{ V} - 0.125 \text{ V} \approx 11.875 \text{ V}$.

Therefore, the current drawn from the supply is approximately 1.39 A, and the terminal voltage is approximately 11.87 V.

Question 3.15 (continued)

(b) A secondary cell after long use has an emf of 1.9 V and a large internal resistance of 380 $\Omega$. What maximum current can be drawn from the cell? Could the cell drive the starting motor of a car?
Solution:

We are given the characteristics of the aged secondary cell:

  • Emf of the cell, $E = 1.9 \text{ V}$
  • Internal resistance of the cell, $r = 380 \Omega$

The maximum current that can be drawn from a cell is when the external resistance is negligible (ideally zero, representing a short circuit). In this case, the current is limited only by the cell's internal resistance. Using Ohm's law:

I_{max} = \frac{E}{r}

Substituting the given values:

I_{max} = \frac{1.9 \text{ V}}{380 \Omega}

I_{max} = 0.005 \text{ A}

The maximum current that can be drawn from this aged cell is 0.005 A.

Regarding driving the starting motor of a car: A car's starting motor requires a very large surge of current, typically hundreds of amperes, to crank the engine. Since the maximum current this cell can provide is only 0.005 A (which is 5 milliamperes), it is far too low to power a car's starting motor.

Therefore, this cell could not drive the starting motor of a car.

Common mistakes

  • Incorrectly calculating the total surface area of the Earth.
  • Errors in applying Ohm's law for series combinations of cells and external resistance.
  • Confusing total emf with individual cell emf in series calculations.
  • Misinterpreting terminal voltage calculations.
  • Underestimating the high current requirements for starting a car engine.

Revision tips

  • Review the formula for the surface area of a sphere and apply it to Earth-related problems.
  • Practice calculating total emf and internal resistance for cells in series.
  • Understand the difference between emf and terminal voltage, especially under load.
  • Analyze the practical limitations of batteries based on their internal resistance and emf.
  • Use the provided solutions to verify your own calculations for these additional exercises.

Practice MCQs

Q1. What is the approximate time required to neutralize the Earth's surface if the global current were the only factor?

Q2. When six 2.0 V cells with 0.015 Ohm internal resistance are connected in series to an 8.5 Ohm resistor, what is the total emf of the combination?

Q3. What is the total internal resistance of six 0.015 Ohm cells connected in series?

Q4. An old secondary cell with emf 1.9 V and internal resistance 380 Ohm can draw a maximum current of:

Q5. Why can't the old secondary cell (1.9 V, 380 Ohm) drive a car's starting motor?

Frequently asked questions

What is the surface charge density of the Earth mentioned in the problem?

The Earth's surface has a negative surface charge density of $10^{-9}$ C m$^{-2}$.

How is the time to neutralize the Earth's surface calculated?

It's calculated by finding the total charge on the Earth's surface (charge density × surface area) and dividing it by the total global current.

What is the total emf when multiple cells are connected in series?

When cells are connected in series, their individual emfs add up to give the total emf of the combination.

How is the terminal voltage of a battery calculated?

Terminal voltage (V) is calculated as the total emf (E) minus the product of the total current (I) and the total internal resistance (r): V = E - Ir.

Why is a large current needed to start a car?

A car's starting motor requires a very large current to overcome the inertia of the engine and initiate combustion.

What limits the maximum current from a secondary cell?

The maximum current is limited by the cell's emf and its internal resistance, calculated as emf divided by internal resistance.

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