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An object of mass 2 kg at rest at origin...

An object of mass 2 kg at rest at origin starts moving under the action of a force
`vec(F)=(3t^(2)hat(i)+4that(j))N` The velocity of the object at t = 2 s will be -

A

`(3hat(i)+2hat(j))m//s`

B

`(2hat(i)+4hat(j))m//s`

C

`(4hat(i)+4hat(j))m//s`

D

`(3hat(i)-4hat(j))m//s`

Text Solution

AI Generated Solution

The correct Answer is:
To find the velocity of the object at \( t = 2 \) seconds, we will follow these steps: ### Step 1: Identify the given information - Mass of the object, \( m = 2 \, \text{kg} \) - Force acting on the object, \( \vec{F} = (3t^2 \hat{i} + 4t \hat{j}) \, \text{N} \) ### Step 2: Calculate the acceleration Using Newton's second law, \( \vec{F} = m \vec{a} \), we can find the acceleration \( \vec{a} \): \[ \vec{a} = \frac{\vec{F}}{m} = \frac{(3t^2 \hat{i} + 4t \hat{j})}{2} \] This gives us: \[ \vec{a} = \left(\frac{3t^2}{2} \hat{i} + 2t \hat{j}\right) \, \text{m/s}^2 \] ### Step 3: Determine the velocity components To find the velocity, we need to integrate the acceleration with respect to time. #### For the x-component of velocity (\( v_x \)): \[ \frac{dv_x}{dt} = \frac{3t^2}{2} \] Integrating with respect to \( t \): \[ dv_x = \frac{3t^2}{2} dt \] Integrating from \( t = 0 \) to \( t = 2 \): \[ v_x = \int_0^2 \frac{3t^2}{2} dt = \frac{3}{2} \cdot \left[\frac{t^3}{3}\right]_0^2 = \frac{3}{2} \cdot \left(\frac{2^3}{3} - 0\right) = \frac{3}{2} \cdot \frac{8}{3} = 4 \, \text{m/s} \] #### For the y-component of velocity (\( v_y \)): \[ \frac{dv_y}{dt} = 2t \] Integrating with respect to \( t \): \[ dv_y = 2t dt \] Integrating from \( t = 0 \) to \( t = 2 \): \[ v_y = \int_0^2 2t dt = \left[t^2\right]_0^2 = 2^2 - 0 = 4 \, \text{m/s} \] ### Step 4: Combine the velocity components Now we can write the total velocity vector at \( t = 2 \) seconds: \[ \vec{v} = v_x \hat{i} + v_y \hat{j} = 4 \hat{i} + 4 \hat{j} \, \text{m/s} \] ### Final Answer The velocity of the object at \( t = 2 \) seconds is: \[ \vec{v} = 4 \hat{i} + 4 \hat{j} \, \text{m/s} \] ---
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