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a particle is moving in x-y-plane at 2 m...

a particle is moving in x-y-plane at `2 m//s` along x-axis. `2` seconds later, its velocity is `4 m//s` in a direction making `60^(@)` with positive x-axis. Its average acceleration for the period of motion is:-

A

`sqrt(5) m//s^(2)`, along y-axis

B

`sqrt(3) m//s^(2)`, along y-axis

C

`sqrt(5) m//s^(2)`, along at `60^(@)` with positive x-axis

D

`3m//s^(2)` at `60^(@)` with positive x-axis.

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The correct Answer is:
To solve the problem, we will follow these steps: ### Step 1: Identify the initial and final velocities - The initial velocity \( \mathbf{V_i} \) is given as \( 2 \, \text{m/s} \) along the x-axis. In vector form, this can be represented as: \[ \mathbf{V_i} = 2 \hat{i} \] - The final velocity \( \mathbf{V_f} \) is given as \( 4 \, \text{m/s} \) at an angle of \( 60^\circ \) with the positive x-axis. We can break this into its x and y components: \[ V_{fx} = 4 \cos(60^\circ) = 4 \times \frac{1}{2} = 2 \, \text{m/s} \] \[ V_{fy} = 4 \sin(60^\circ) = 4 \times \frac{\sqrt{3}}{2} = 2\sqrt{3} \, \text{m/s} \] Thus, the final velocity in vector form is: \[ \mathbf{V_f} = 2 \hat{i} + 2\sqrt{3} \hat{j} \] ### Step 2: Calculate the change in velocity The change in velocity \( \Delta \mathbf{V} \) is given by: \[ \Delta \mathbf{V} = \mathbf{V_f} - \mathbf{V_i} \] Substituting the values: \[ \Delta \mathbf{V} = (2 \hat{i} + 2\sqrt{3} \hat{j}) - (2 \hat{i}) = 2\sqrt{3} \hat{j} \] ### Step 3: Calculate the average acceleration The average acceleration \( \mathbf{a_{avg}} \) is given by the change in velocity divided by the time interval. The time interval is \( 2 \, \text{s} \): \[ \mathbf{a_{avg}} = \frac{\Delta \mathbf{V}}{\Delta t} = \frac{2\sqrt{3} \hat{j}}{2} = \sqrt{3} \hat{j} \, \text{m/s}^2 \] ### Step 4: Final Result Thus, the average acceleration of the particle is: \[ \mathbf{a_{avg}} = \sqrt{3} \hat{j} \, \text{m/s}^2 \]

To solve the problem, we will follow these steps: ### Step 1: Identify the initial and final velocities - The initial velocity \( \mathbf{V_i} \) is given as \( 2 \, \text{m/s} \) along the x-axis. In vector form, this can be represented as: \[ \mathbf{V_i} = 2 \hat{i} \] ...
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