Sigma Percentile
JEE Main 2019
LEVELJEE Main

Animated Solution for Physics - Electrostatics: Four equal point charges each are placed in the xy-plane at , , and . The work required to put a fifth charge at the origin of the coordinate system (in joule) will be

Select Answer:

Visualized Solution

Visualizing the Setup

  • Four charges are placed at , , , and .

Work Done and Potential

  • Work done to bring a charge to the origin:
  • Net potential at origin:

Calculating Distances

Net Potential Equation

Simplifying Potential

Calculating Work Done

Final Answer

  • Final Answer:

The Way Forward

  • Consider: What if the charges at and were ?
  • How would the net potential change?

The Sigma Insight: Electric Potential and Potential Difference

Solution Diagram

The Geometry of Charges

Imagine a blank canvas, the -plane, where we are about to place four identical point charges, each carrying a charge . We pin them down at specific coordinates: , , , and . These charges create an invisible landscape of electric potential around them.
Our mission is to find out how much work it takes to bring a fifth charge, also , from infinitely far away and place it exactly at the origin .

The Master Equation

Work and Potential
In electrostatics, the work done by an external agent to bring a charge from infinity to a point is directly proportional to the electric potential at that point. The relationship is beautifully simple:
Here, our test charge is . So, our entire problem boils down to finding the net electric potential at the origin due to the four existing charges.

Superposition

Adding it All Up
The principle of superposition tells us that the net potential at any point is simply the algebraic sum of the potentials due to each individual charge. Unlike electric fields, potential is a scalar quantity, which means we don't have to worry about vector components or angles—we just add the numbers!
The potential due to a single point charge at a distance is given by:
where .
Let's find the distance of each of our four charges from the origin : 1. For the charge at , the distance is . 2. For the charge at , the distance is . 3. For the charge at , the distance is . 4. For the charge at , the distance is .

The Final Calculation

Now, we plug these distances into our superposition equation:
Let's factor out to make the algebra cleaner:
We know that . Also, can be simplified to .
Finally, we calculate the work done by multiplying this net potential by our fifth charge :
Substituting , we arrive at our final, elegant result:
This matches option (d) perfectly. The beauty of this problem lies in recognizing that scalar addition makes complex geometric arrangements surprisingly easy to handle!

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