CBSE Class 12 Physics Chapter 2: Electrostatic Potential and Capacitance - NCERT Solutions

NCERT Solutions PDF Class 12 PDF

This resource provides comprehensive NCERT Solutions for Class 12 Physics, Chapter 2: Electrostatic Potential and Capacitance. It covers key concepts such as calculating the electric potential at various points due to charges and understanding the potential at the center of geometric shapes like a regular hexagon. The solutions break down complex problems into manageable steps, explaining the underlying principles and formulas used. This detailed approach helps students grasp the nuances of electrostatic potential and capacitance, aiding in their preparation for board examinations and competitive entrance tests. By working through these solved examples, students can reinforce their understanding and build confidence in tackling similar problems.

Quick info

BoardCBSE
ClassClass 12
SubjectPhysics
Session2026
LanguageEnglish
TypeNCERT Solutions
ChapterChapter 2: Electrostatic Potential and Capacitance - NCERT Exercises Solutions

Chapter summary

This chapter's NCERT Solutions focus on electrostatic potential and capacitance. It includes problems requiring the calculation of electric potential at specific points along the line joining two charges, considering both internal and external points. Another key problem involves determining the potential at the center of a regular hexagon with charges at its vertices. The solutions emphasize the principle of superposition for electric potential and the properties of regular polygons in electrostatics.

Learning outcomes

  • Understand the concept of electric potential due to point charges.
  • Calculate the point where electric potential is zero along the line joining two charges.
  • Apply the principle of superposition to find the total electric potential.
  • Determine the electric potential at the center of a regular hexagon with charges at vertices.
  • Convert units of charge and distance for calculations.

Topics covered

Paper topics

  • Electric Potential
  • Potential due to a point charge
  • Superposition principle for potential
  • Potential due to a system of charges
  • Zero potential points
  • Electric potential of a regular hexagon
  • Relationship between potential and distance
  • Units of potential

Important topics

  • Calculating zero potential points for two charges
  • Potential at the center of a regular polygon
  • Superposition of electric potentials
  • Understanding potential due to multiple charges

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Questions and Solutions

Question 2.1

Two charges <math>5 \times 10^{-8}</math> C and <math>-3 \times 10^{-8}</math> C are located 16 cm apart. At what point(s) on the line joining the two charges is the electric potential zero? Take the potential at infinity to be zero.
Solution:

We are given two charges: <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 two 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 = \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>

This implies:

<math display="block">\frac{q_1}{r} = -\frac{q_2}{(d-r)}</math>

Substituting the values:

<math display="block">\frac{5 \times 10^{-8}}{r} = -\frac{(-3 \times 10^{-8})}{(0.16-r)}</math>

Simplifying the equation:

<math>5(0.16 - r) = 3r</math>

<math>0.8 - 5r = 3r</math>

<math>0.8 = 8r</math>

<math>r = \frac{0.8}{8} = 0.1 \text{ m} = 10 \text{ cm}</math>

So, the potential is zero at a distance of 10 cm from the positive charge (<math>q_1</math>), between the two charges.

Case 2: Point P is outside the two charges.

Let P be a point at a distance <math>s</math> from the negative charge (<math>q_2</math>). Since <math>q_1</math> is positive and <math>q_2</math> is negative, the point of zero potential must be closer to the charge with the smaller magnitude, which is <math>q_2</math>. Thus, P will be on the side of <math>q_2</math> away from <math>q_1</math>. The distance of P from <math>q_1</math> will be <math>(s+d)</math>.

The net potential at P is:

<math display="block">V = \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_1}{(s+d)} + \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_2}{s}</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+d)} + \frac{1}{4\pi\varepsilon_0} \cdot \frac{q_2}{s} = 0</math>

This implies:

<math display="block">\frac{q_1}{(s+d)} = -\frac{q_2}{s}</math>

Substituting the values:

<math display="block">\frac{5 \times 10^{-8}}{(s+0.16)} = -\frac{(-3 \times 10^{-8})}{s}</math>

Simplifying the equation:

<math>5s = 3(s+0.16)</math>

<math>5s = 3s + 0.48</math>

<math>2s = 0.48</math>

<math>s = \frac{0.48}{2} = 0.24 \text{ m} = 24 \text{ cm}</math>

This distance <math>s</math> is measured from <math>q_2</math>. The distance from <math>q_1</math> would be <math>s+d = 24 + 16 = 40 \text{ cm}</math>.

Therefore, the electric potential is zero at two points: 10 cm from the positive charge between the charges, and 40 cm from the positive charge (or 24 cm from the negative charge) outside the system of charges.

Question 2.2

A regular hexagon of side 10 cm has a charge 5 µC at each of its vertices. Calculate the potential at the centre of the hexagon.
Solution:

We have a regular hexagon with side length <math>l = 10 \text{ cm} = 0.1 \text{ m}</math>. There are six charges, each of magnitude <math>q = 5 \mu C = 5 \times 10^{-6} C</math>, placed at each vertex.

In a regular hexagon, the distance from the center to each vertex is equal to the side length of the hexagon. Therefore, the distance of each vertex from the center (let's call it O) is <math>d = l = 0.1 \text{ m}</math>.

The electric potential at the center O is the sum of the potentials due to each of the six charges. Since all charges are identical and equidistant from the center, we can use the principle of superposition.

The potential due to a single charge <math>q</math> at a distance <math>d</math> is given by <math>V_{single} = \frac{1}{4\pi\varepsilon_0} \cdot \frac{q}{d}</math>.

Since there are six such charges, the total potential at the center is:

<math display="block">V_{total} = 6 \times V_{single} = 6 \times \frac{1}{4\pi\varepsilon_0} \cdot \frac{q}{d}</math>

We know that the electrostatic constant <math>\frac{1}{4\pi\varepsilon_0} = 9 \times 10^9 \text{ Nm}^2\text{C}^{-2}</math>.

Substituting the given values:

<math display="block">V_{total} = 6 \times (9 \times 10^9 \text{ Nm}^2\text{C}^{-2}) \times \frac{5 \times 10^{-6} \text{ C}}{0.1 \text{ m}}</math>

Calculating the value:

<math>V_{total} = 6 \times 9 \times 10^9 \times 5 \times 10^{-5} \text{ V}</math>

<math>V_{total} = 270 \times 10^4 \text{ V} = 2.7 \times 10^6 \text{ V}</math>

Therefore, the potential at the centre of the hexagon is <math>2.7 \times 10^6 \text{ V}</math>.

Common mistakes

  • Incorrectly setting up the distance variable for points outside the charge system.
  • Errors in algebraic manipulation when solving for the position of zero potential.
  • Forgetting to convert units (e.g., cm to m) before calculation.
  • Misapplying the superposition principle for potential.

Revision tips

  • Review the formula for electric potential due to a point charge and the superposition principle.
  • Practice setting up equations for points between and outside charges carefully.
  • Ensure all units are consistent (SI units) before performing calculations.
  • Visualize the geometry of the problem, especially for regular polygons.

Practice MCQs

Q1. For two charges q1 and q2 separated by distance d, at what point on the line joining them is the electric potential zero?

Q2. If a regular hexagon has identical charges at each vertex, where is the net electric potential zero?

Q3. What is the unit of electric potential?

Q4. If the distance between two charges is halved, how does the electric potential at a point midway between them change (assuming charges remain the same)?

Frequently asked questions

What is electric potential?

Electric potential at a point in an electric field is the amount of work done per unit positive charge in bringing the charge from infinity to that point. Its SI unit is the Volt (V).

How do you find the point where electric potential is zero for two charges?

You set up an equation where the sum of potentials from each charge is zero. This often involves considering points between the charges and points outside the charges, solving algebraically for the distance.

What is the significance of a regular hexagon in these problems?

A regular hexagon has symmetry where all vertices are equidistant from the center. This simplifies calculations for potential at the center, as the distance term in the potential formula is the same for all charges.

Why is it important to convert units in these calculations?

The electrostatic constant (1/(4πε₀)) uses SI units. To get the correct potential in Volts, all distances must be in meters and charges in Coulombs.

How do these solutions help in exam preparation?

These solutions provide clear, step-by-step methods to solve typical problems from the NCERT textbook, reinforcing understanding of concepts and improving problem-solving skills for exams.

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