If potential (in volt) in a region is expressed as $ V(x, y, z) = 6xy - y + 2yz $, the electric field (in} $ \text{N/C} $ at point (1, 0, 1) is:
The electric field is the negative gradient of the potential. The gradient of the potential function in three dimensions is: \[ \vec{E} = - \nabla V = - \left( \frac{\partial V}{\partial x} \hat{i} + \frac{\partial V}{\partial y} \hat{j} + \frac{\partial V}{\partial z} \hat{k} \right) \] We are given the potential: \[ V(x, y, z) = 6xy - y + 2yz \] Now, calculate the partial derivatives:
1. \( \frac{\partial V}{\partial x} = 6y \) 2. \( \frac{\partial V}{\partial y} = 6x - 1 + 2z \) 3. \( \frac{\partial V}{\partial z} = 2y \)
At the point \( (1, 0, 1) \): 1. \( \frac{\partial V}{\partial x} = 6(0) = 0 \)
2. \( \frac{\partial V}{\partial y} = 6(1) - 1 + 2(1) = 6 - 1 + 2 = 7 \)
3. \( \frac{\partial V}{\partial z} = 2(0) = 0 \)
Thus, the electric field is: \[ \vec{E} = - \left( 0 \hat{i} + 7 \hat{j} + 0 \hat{k} \right) = -7 \hat{j} \]
Therefore, the electric field at point \( (1, 0, 1) \) is \( -7j \).
Three point charges are located on a circular arc at A, B and C as shown in the figure below. The total electric field at the centre of the arc (C) is 
Five charges, 'q' each are placed at the corners of a regular pentagon of side 'a' as shown in figure. First, charge from 'A' is removed with other charges intact, then charge at 'A' is replaced with an equal opposite charge. The ratio of magnitudes of electric fields at O, without charge at A and that with equal and opposite charge at A is 