Question
Question: Four charges are placed at the vertices of square with side of \(5cm\) . The charges are: \(1, - 1,2...
Four charges are placed at the vertices of square with side of 5cm . The charges are: 1,−1,2,−2×10−8C . What is the Electric field at the center of the square?
Solution
First let’s see the top left corner charge and right bottom corner charge i.e. q2 and q4 . since it’s a square both of them are at equal distance from the center. find the net field at the center, similar way for a charge at the top right corner and bottom left corner i.e. q1 and q3 . find the distance of separation, then find field magnitude, then calculate the electric field at the center of the square.
Complete answer:
At point, A due to charge q1 the electric field is away from the charge because it's positive so it will create repulsive force let it be E , due to charge q2 the electric field is towards the charge because it's negative let it be E.
Similarly, for charge q3 the electric field is away from the charge, the charge has doubled but the distance is same from the center let it be 2E, at last for charge q4 the electric field is towards the charge let it also be 2E
Now we see the charge q1 and q3 are linear and in the opposite direction so the net electric field will be ⇒2E−E=E
Similarly for q2 and q4 .
From the above diagram, both the electric field are perpendicular to each other so the net electric field will be in between
⇒Enet=E2+E2
Hence, Enet=E2
Now finding the value of E
⇒E=(halfofdiagonal)2kq
⇒E=(r)2kq
Now we will find the distance of separation r , diagonal is a2 so,
⇒r=2a2
Therefore, E=(2a2)29×109×10−8
⇒E=(25×10−22)29×109×10−8
⇒E=25×10−49×10×2
⇒E=7.2×104CN
Hence Enet=7.19×104×2
⇒Enet=1.02×105CN
Hence the electric field at the center of the square is Enet=1.02×105CN
Note:
The electric field in the square's center is the vector sum of the electric fields in the center caused by each of the charges separately. The algebraic total of the potentials at the center owing to each of the charges individually equals the potential at the center of the square.