The electric field intensity at the center of the square due to each charge will be equal in magnitude but directed towards each charge. Since the charges are placed symmetrically, the directions of the electric field due to each charge are such that they cancel each other out. Therefore, the net electric field intensity E at the center of the square is zero.

The electric potential at a point due to a charge is a scalar quantity and it does not have any direction. The electric potential at the center of the square due to each charge will be the same since the distance from each charge to the center of the square is the same. Therefore, the net electric potential V at the center of the square is four times the electric potential due to one charge.

Let's denote each charge as q and the distance from each charge to the center of the square as a. The electric potential V due to one charge is given by the formula V = k*q/a, where k is Coulomb's constant. Therefore, the net electric potential at the center of the square is V_net = 4*k*q/a.

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The electric field intensity at the center of the square due to each charge will be equal in magnitude but directed towards each charge. Since the charges are placed symmetrically, the directions of the electric field due to each charge are such that they cancel each other out. Therefore, the net electric field intensity E at the center of the square is zero.

The electric potential at a point due to a charge is a scalar quantity and it does not have any direction. The electric potential at the center of the square due to each charge will be the same since the distance from each charge to the center of the square is the same. Therefore, the net electric potential V at the center of the square is four times the electric potential due to one charge.

Let's denote each charge as q and the distance from each charge to the center of the square as a. The electric potential V due to one charge is given by the formula V = k*q/a, where k is Coulomb's constant. Therefore, the net electric potential at the center of the square is V_net = 4*k*q/a.

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The electric field intensity at the center of the square due to each charge will be equal in magnitude but directed towards each charge. Since the charges are placed symmetrically, the directions of the electric field due to each charge are such that they cancel each other out. Therefore, the net electric field intensity E at the center of the square is zero.

The electric potential at a point due to a charge is a scalar quantity and it does not have any direction. The electric potential at the center of the square due to each charge will be the same since the distance from each charge to the center of the square is the same. Therefore, the net electric potential V at the center of the square is four times the electric potential due to one charge.

Let's denote each charge as q and the distance from each charge to the center of the square as a. The electric potential V due to one charge is given by the formula V = k*q/a, where k is Coulomb's constant. Therefore, the net electric potential at the center of the square is V_net = 4*k*q/a.

Four identical charges each of charge are placed at the corners of a square. Then at the centre of the square the resultant electric intensity E and the net electric potential V are

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