Question:

An electric dipole is formed by two charges +q and -q located in the x-y plane at (0,2) mm and (0,-2) mm as shown in the figure. The electric potential at point P(100, 100) mm due to dipole is V0. Now the charges +q and -q are moved to (-1,2)mm and (1,-2)mm respectively. What is the value of the electric potential at point P due to this new dipole?
An electric dipole is formed by two charges +q and -q located in the x-y plane at (0,2) mm and (0,-2) mm

Updated On: June 02, 2025
  • \(\frac{V_0}{2}\)
  • \(\frac{V_0}{4}\)
  • \(\frac{V_0}{8}\)
  • \(2V_0\)
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The Correct Option is A

Solution and Explanation

Electrostatic Potential Calculation

The correct option is: (A):

\(\vec{p_1} = q \times 4 \times 10^{-3} \hat{j}\)

Step 1: Calculate \(V_0\) at \((100,100) \, \text{mm}\)

The potential \(V_0\) is given by:

\(V_0 = \frac{K \vec{p_1} \cdot \vec{r_1}}{|\vec{r_1}|^3}\)

Substituting the known values:

\(V_0 = \frac{9 \times 10^9 \times q \times [4 \times 10^{-3} \hat{j}] \cdot (0.1 \hat{i} + 0.1 \hat{j})}{\left(\sqrt{(0.1)^2 + (0.1)^2}\right)^3}\)

Simplifying the dot product:

\(V_0 = \frac{9 \times 10^9 \times q \times [0.4 \times 10^{-3}]}{(0.1)^2 \times 2 \sqrt{2}}\)

Step 2: Moving Charges to New Positions

Now, +q and -q are moved to the points (-1,2) mm and (1,-2) mm, respectively. The new position vector is:

\(\vec{p} = q[-2 \hat{i} + 4 \hat{j}] \times 10^{-3}\)

The position vector \(\vec{r_1}\) remains:

\(\vec{r_1} = 0.1 \hat{i} + 0.1 \hat{j}\)

Step 3: Calculate the New Potential \(V\)

The new potential \(V\) is calculated as:

\(V = \frac{9 \times 10^9 (\vec{p}, \vec{r_1})}{|\vec{r_1}|^3}\)

Substituting the values:

\(V = \frac{9 \times 10^9 \times q \times [0.4 \times 10^{-3}]}{\left(\sqrt{(0.1)^2 + (0.1)^2}\right)^3}\)

Simplifying:

\(V = \frac{V_0}{2}\)

Thus, the new potential \(V\) is half of the original potential \(V_0\), confirming the relationship between the initial and final potentials.

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Concepts Used:

Electromagnetic waves

The waves that are produced when an electric field comes into contact with a magnetic field are known as Electromagnetic Waves or EM waves. The constitution of an oscillating magnetic field and electric fields gives rise to electromagnetic waves.

Types of Electromagnetic Waves:

Electromagnetic waves can be grouped according to the direction of disturbance in them and according to the range of their frequency. Recall that a wave transfers energy from one point to another point in space. That means there are two things going on: the disturbance that defines a wave, and the propagation of wave. In this context the waves are grouped into the following two categories:

  • Longitudinal waves: A wave is called a longitudinal wave when the disturbances in the wave are parallel to the direction of propagation of the wave. For example, sound waves are longitudinal waves because the change of pressure occurs parallel to the direction of wave propagation.
  • Transverse waves: A wave is called a transverse wave when the disturbances in the wave are perpendicular (at right angles) to the direction of propagation of the wave.