CBSE Class 12 Physics Chapter 4: Electric Potential and Capacitance NCERT Solutions
This resource provides comprehensive NCERT Solutions for Class 12 Physics, Chapter 4, focusing on Electric Potential and Capacitance. It covers key concepts such as electric potential due to point charges and systems of charges, and potential at the center of regular polygons. The solutions break down complex problems into manageable steps, explaining the underlying physics principles. Students will find detailed explanations for calculating potential at various points, including those between charges and outside charge distributions. These solutions are designed to aid in understanding the chapter's topics thoroughly and are an excellent tool for exam preparation, helping students build confidence and accuracy in their problem-solving skills for the board examinations.
Quick info
| Board | CBSE |
|---|---|
| Class | Class 12 |
| Subject | Physics |
| Session | 2026 |
| Language | English |
| Type | NCERT Solutions |
| Chapter | Chapter 4 |
Chapter summary
This chapter's NCERT Solutions for Class 12 Physics delve into the concepts of electric potential and capacitance. It includes exercises focused on calculating electric potential at different points in space due to various charge configurations, such as pairs of charges and charges at the vertices of regular polygons. The solutions emphasize the principle of superposition for electric potentials and the relationship between potential and distance. They provide a clear, step-by-step approach to solving problems, ensuring students grasp the quantitative aspects of electrostatics.
Learning outcomes
- Understand the concept of electric potential due to point charges.
- Calculate the electric potential at a point between two charges where it is zero.
- Determine the electric potential at a point outside a system of charges.
- Calculate the electric potential at the center of a regular hexagon with charges at its vertices.
- Apply the principle of superposition for electric potentials.
- Convert units of charge and distance for calculations.
Topics covered
Paper topics
- Electric Potential
- Potential due to a Point Charge
- Potential due to a System of Charges
- Potential at a Point Between Charges
- Potential at a Point Outside Charges
- Potential at the Center of a Regular Hexagon
- Superposition Principle for Potential
- Units of Charge and Potential
- Distance Calculations in Electrostatics
Important topics
- Calculating electric potential at points of zero potential
- Applying superposition principle for potential
- Potential at the center of symmetrical charge distributions
- Algebraic manipulation for distance calculations
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Questions and Solutions
Question 2.1
Let the two charges be <math>q_1 = 5 \times 10^{-8} \,\mathrm{C}</math> and <math>q_2 = -3 \times 10^{-8} \text{ C}</math>. The distance between them is <math>d = 16 \text{ cm} = 0.16 \text{ m}</math>.
We need to find the point(s) on the line joining these charges where the net electric potential is zero. The electric potential at any point due to a charge is given by <math>V = \frac{1}{4\pi\varepsilon_0} \cdot \frac{q}{r}</math>, where <math>q</math> is the charge and <math>r</math> is the distance from the charge.
Case 1: Point P is between the charges.
Let P be a point at a distance <math>r</math> from <math>q_1</math>. Then, the distance of P from <math>q_2</math> is <math>(d-r)</math>. The net potential at P is the sum of potentials due to <math>q_1</math> and <math>q_2</math>:
<math display="block">V = V_1 + V_2 = \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_1}{r} + \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_2}{(d-r)}</math>
For the potential to be zero (<math>V = 0</math>):
<math display="block">\frac{1}{4\pi\varepsilon_0} \cdot \frac{q_1}{r} + \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_2}{(d-r)} = 0</math>
<math display="block">\Rightarrow \frac{q_1}{r} = -\frac{q_2}{(d-r)}</math>
Substituting the values:
<math display="block">\Rightarrow \frac{5 \times 10^{-8}}{r} = -\frac{(-3 \times 10^{-8})}{(0.16-r)}</math>
<math display="block">\Rightarrow \frac{5}{r} = \frac{3}{(0.16-r)}</math>
<math display="block">\Rightarrow 5(0.16 - r) = 3r</math>
<math display="block">\Rightarrow 0.8 - 5r = 3r</math>
<math display="block">\Rightarrow 0.8 = 8r</math>
<math display="block">\Rightarrow r = \frac{0.8}{8} = 0.1 \text{ m} = 10 \text{ cm}</math>
So, the potential is zero at a point 10 cm from the positive charge <math>q_1</math>, between the two charges.
Case 2: Point P is outside the charges.
Since the charges have opposite signs, the potential can also be zero at a point outside the segment joining the charges. Let P be a point at a distance <math>s</math> from the negative charge <math>q_2</math>, such that it is on the line extending from <math>q_1</math> through <math>q_2</math>. The distance of P from <math>q_1</math> will be <math>(d+s)</math>. However, it is more convenient to consider the point P at a distance <math>s</math> from the positive charge <math>q_1</math>, outside the segment, on the side of <math>q_2</math>. In this case, the distance from <math>q_2</math> is <math>(s-d)</math>.
The net potential at P is:
<math display="block">V = V_1 + V_2 = \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_1}{s} + \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_2}{(s-d)}</math>
For the potential to be zero (<math>V = 0</math>):
<math display="block">\frac{1}{4\pi\varepsilon_0} \cdot \frac{q_1}{s} + \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_2}{(s-d)} = 0</math>
<math display="block">\Rightarrow \frac{q_1}{s} = -\frac{q_2}{(s-d)}</math>
Substituting the values:
<math display="block">\Rightarrow \frac{5 \times 10^{-8}}{s} = -\frac{(-3 \times 10^{-8})}{(s - 0.16)}</math>
<math display="block">\Rightarrow \frac{5}{s} = \frac{3}{(s - 0.16)}</math>
<math display="block">\Rightarrow 5(s - 0.16) = 3s</math>
<math display="block">\Rightarrow 5s - 0.8 = 3s</math>
<math display="block">\Rightarrow 2s = 0.8</math>
<math display="block">\Rightarrow s = \frac{0.8}{2} = 0.4 \text{ m} = 40 \text{ cm}</math>
Thus, the potential is also zero at a point 40 cm from the positive charge <math>q_1</math>, outside the system of charges.
Answer: The electric potential is zero at two points: 10 cm from the positive charge between the two charges, and 40 cm from the positive charge outside the system of charges.
Question 2.2
A regular hexagon has 6 vertices. Let the side length of the hexagon be <math>l = 10 \text{ cm} = 0.1 \text{ m}</math>. A charge of <math>q = 5 \mu C = 5 \times 10^{-6} C</math> is placed at each vertex.
In a regular hexagon, the distance from each vertex to the center is equal to the side length of the hexagon. Therefore, the distance of each vertex from the center (O) is <math>d = l = 0.1 \text{ m}</math>.
The electric potential at the center of the hexagon is the sum of the potentials due to the charges at all six vertices. Using the principle of superposition, the total potential <math>V</math> at the center is:
<math display="block">V = V_1 + V_2 + V_3 + V_4 + V_5 + V_6</math>
Since all charges are equal (<math>q</math>) and the distance from each vertex to the center is the same (<math>d</math>), the potential due to each charge at the center is <math>\frac{1}{4\pi\varepsilon_0} \cdot \frac{q}{d}</math>.
Therefore, the total potential is:
<math display="block">V = 6 \times \left( \frac{1}{4\pi\varepsilon_0} \cdot \frac{q}{d} \right)</math>
We know that <math>\frac{1}{4\pi\varepsilon_0} = 9 \times 10^9 \text{ Nm}^2/\text{C}^2</math>.
Substituting the values:
<math display="block">V = 6 \times \left( 9 \times 10^9 \frac{\text{Nm}^2}{\text{C}^2} \times \frac{5 \times 10^{-6} \text{ C}}{0.1 \text{ m}} \right)</math>
<math display="block">V = 6 \times \left( 9 \times 10^9 \times 50 \times 10^{-6} \right) \text{ V}</math>
<math display="block">V = 6 \times (450 \times 10^3) \text{ V}</math>
<math display="block">V = 2700 \times 10^3 \text{ V} = 2.7 \times 10^6 \text{ V}</math>
Answer: The potential at the centre of the hexagon is <math>2.7 \times 10^6 \text{ V}</math>.
Common mistakes
- Incorrectly setting up the potential equation for points outside the charge system.
- Errors in algebraic manipulation when solving for distance.
- Forgetting to convert units (cm to m, µC to C) before calculation.
- Assuming the potential is zero only between charges, neglecting external points.
Revision tips
- Review the formula for electric potential due to a point charge and the principle of superposition.
- Practice solving problems involving potential being zero at different locations (between charges, outside charges).
- Pay close attention to the signs of charges and the distances involved in calculations.
- Ensure all units are consistent (SI units) before substituting values into formulas.
Practice MCQs
Q1. For two charges q1 and q2 separated by a distance d, at what point on the line joining them is the electric potential zero?
Explanation: The electric potential can be zero at a point between the charges if they have opposite signs, or at a point outside the charges (closer to the smaller magnitude charge) if they have opposite signs.
Q2. If a regular hexagon has identical charges at each vertex, where is the electric potential calculated?
Explanation: The problem typically asks for the potential at the center of the hexagon, where the distances from all vertices are equal.
Q3. What is the key principle used to calculate the total electric potential at a point due to multiple charges?
Explanation: The total electric potential at a point due to a system of charges is the algebraic sum of the potentials due to each individual charge.
Q4. In Question 2.1, if the potential is zero at a distance 'r' from q1 and 'd-r' from q2, what is the relationship between q1/r and q2/(d-r)?
Explanation: For the potential to be zero, the contributions from both charges must cancel out, meaning q1/r + q2/(d-r) = 0, which implies q1/r = -q2/(d-r).
Frequently asked questions
What is the main concept covered in CBSE Class 12 Physics Chapter 4 NCERT Solutions?
Chapter 4 of CBSE Class 12 Physics NCERT Solutions focuses on Electric Potential and Capacitance, covering calculations of electric potential due to various charge configurations and understanding capacitance.
How do these NCERT Solutions help in solving problems related to electric potential?
These solutions provide step-by-step explanations for complex problems, demonstrating how to apply formulas, handle signs of charges, and perform algebraic manipulations to find the electric potential at different points.
Are the questions in the NCERT Solutions the same as in the textbook?
Yes, the questions in these NCERT Solutions are kept the same as in the textbook, ensuring that students are practicing the exact problems prescribed by the board.
What is the significance of calculating the point where electric potential is zero?
Finding points where electric potential is zero is crucial for understanding the electric field's behavior and for analyzing charge distributions, especially when dealing with opposite charges.
How are the solutions presented for problems involving multiple charges?
Solutions for multiple charges utilize the principle of superposition, where the total potential is the algebraic sum of potentials due to each individual charge.
What is the distance of each vertex from the center of a regular hexagon?
For a regular hexagon, the distance of each vertex from the center is equal to the side length of the hexagon.
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