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 \( -7j \).
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: