We are given:
Step 1: Use Newton’s Second Law to find acceleration:
\[ \vec{a} = \frac{\vec{F}}{m} = 2t \hat{i} + 3t^2 \hat{j} \]
Step 2: Integrate to find velocity:
\[ \vec{v} = \int \vec{a} \, dt = \int (2t \hat{i} + 3t^2 \hat{j}) \, dt = t^2 \hat{i} + t^3 \hat{j} \]
Step 3: Power is given by dot product \( \vec{F} \cdot \vec{v} \):
\[ P = (2t \hat{i} + 3t^2 \hat{j}) \cdot (t^2 \hat{i} + t^3 \hat{j}) = 2t^3 + 3t^5 \] \[ \Rightarrow P = 2t^3 + 3t^5 \, \text{W} \]
Given: \[ \vec{F} = (2t \hat{i} + 3t \hat{j}) \, \text{N} \] The mass of the object is \( m = 1000 \, \text{gm} = 1 \, \text{kg} \). Using Newton's second law: \[ \vec{F} = m \vec{a} \quad \Rightarrow \quad \vec{a} = 2t \hat{i} + 3t^2 \hat{j} \] The velocity is the integral of acceleration: \[ \frac{d\vec{v}}{dt} = 2t \hat{i} + 3t^2 \hat{j} \] Integrating with respect to time: \[ \vec{v} = t^2 \hat{i} + t^3 \hat{j} \] Now, the power \( P \) is given by the dot product of force and velocity: \[ P = \vec{F} \cdot \vec{v} \] Substitute the expressions for \( \vec{F} \) and \( \vec{v} \): \[ P = (2t \hat{i} + 3t \hat{j}) \cdot (t^2 \hat{i} + t^3 \hat{j}) \] Simplifying: \[ P = (2t^3 + 3t^5) \, \text{W} \] \[ \boxed{P = 2t^3 + 3t^5 \, \text{W}} \]
A force \( \vec{f} = x^2 \hat{i} + y \hat{j} + y^2 \hat{k} \) acts on a particle in a plane \( x + y = 10 \). The work done by this force during a displacement from \( (0,0) \) to \( (4m, 2m) \) is Joules (round off to the nearest integer).


In the first configuration (1) as shown in the figure, four identical charges \( q_0 \) are kept at the corners A, B, C and D of square of side length \( a \). In the second configuration (2), the same charges are shifted to mid points C, E, H, and F of the square. If \( K = \frac{1}{4\pi \epsilon_0} \), the difference between the potential energies of configuration (2) and (1) is given by: