Animated Solution for Physics - Electrostatics: Four equal point charges Q each are placed in the xy-plane at (0,2), (4,2), (4,−2) and (0,−2). The work required to put a fifth charge Q at the origin of the coordinate system (in joule) will be
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Visualized Solution
Visualizing the Setup
Four charges Q are placed at (0,2), (0,−2), (4,2), and (4,−2).
Work Done and Potential
Work done to bring a charge Q to the origin:
W=Q⋅Vorigin
Net potential at origin:
Vorigin=V1+V2+V3+V4
Calculating Distances
r1=02+22=2
r2=02+(−2)2=2
r3=42+22=20
r4=42+(−2)2=20
Net Potential Equation
V=r1KQ+r2KQ+r3KQ+r4KQ
V=2KQ+2KQ+20KQ+20KQ
Simplifying Potential
V=KQ[21+21+202]
V=KQ[1+252]
V=KQ(1+51)
Calculating Work Done
W=Q⋅V
W=Q⋅KQ(1+51)
W=4πε0Q2(1+51)
Final Answer
Final Answer: 4πε0Q2(1+51)
The Way Forward
Consider: What if the charges at (4,2) and (4,−2) were −Q?
How would the net potential change?
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The Sigma Insight: Electric Potential and Potential Difference
Solution Diagram
The Geometry of Charges
Imagine a blank canvas, the xy-plane, where we are about to place four identical point charges, each carrying a charge Q. We pin them down at specific coordinates: (0,2), (0,−2), (4,2), and (4,−2). 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 Q, from infinitely far away and place it exactly at the origin (0,0).
The Master Equation
Work and Potential
In electrostatics, the work done W by an external agent to bring a charge q from infinity to a point is directly proportional to the electric potential V at that point. The relationship is beautifully simple:
W=qV
Here, our test charge q is Q. So, our entire problem boils down to finding the net electric potential V 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 V due to a single point charge Q at a distance r is given by:
V=rKQ
where K=4πε01.
Let's find the distance of each of our four charges from the origin (0,0):
1. For the charge at (0,2), the distance is r1=02+22=2.
2. For the charge at (0,−2), the distance is r2=02+(−2)2=2.
3. For the charge at (4,2), the distance is r3=42+22=16+4=20.
4. For the charge at (4,−2), the distance is r4=42+(−2)2=16+4=20.
The Final Calculation
Now, we plug these distances into our superposition equation:
V=r1KQ+r2KQ+r3KQ+r4KQ
V=2KQ+2KQ+20KQ+20KQ
Let's factor out KQ to make the algebra cleaner:
V=KQ[21+21+202]
We know that 21+21=1. Also, 20 can be simplified to 4×5=25.
V=KQ[1+252]
V=KQ(1+51)
Finally, we calculate the work done by multiplying this net potential by our fifth charge Q:
W=Q⋅V=Q⋅KQ(1+51)
Substituting K=4πε01, we arrive at our final, elegant result:
W=4πε0Q2(1+51)
This matches option (d) perfectly. The beauty of this problem lies in recognizing that scalar addition makes complex geometric arrangements surprisingly easy to handle!