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A particle is moving in xy-plane in a ci...

A particle is moving in xy-plane in a circular path with centre at origin. If at an instant the position of particle is given by `(1)/(sqrt(2)) ( hat(i) + hat(j))`, then velocity of particle is along

A

`(1)/(sqrt(2)) (hat(i) - hat(j))`

B

`(1)/(sqrt(2))( hat(j) - hat(i))`

C

`(1)/(sqrt(2))( hat(i) + hat(j))`

D

Either (1) or (2)

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem step by step, we need to find the direction of the velocity of a particle moving in a circular path in the xy-plane, given its position vector. ### Step 1: Identify the position vector The position vector of the particle is given as: \[ \mathbf{r} = \frac{1}{\sqrt{2}} \hat{i} + \hat{j} \] ### Step 2: Determine the angular velocity vector Since the particle is moving in a circular path in the xy-plane, the angular velocity vector \(\mathbf{\omega}\) will be along the z-axis. It can be either in the positive z-direction (\(\hat{k}\)) or negative z-direction (\(-\hat{k}\)). ### Step 3: Calculate the velocity vector using the cross product The velocity \(\mathbf{v}\) of the particle can be calculated using the formula: \[ \mathbf{v} = \mathbf{r} \times \mathbf{\omega} \] Substituting the position vector and the angular velocity vector, we have: \[ \mathbf{v} = \left(\frac{1}{\sqrt{2}} \hat{i} + \hat{j}\right) \times \mathbf{\omega} \] ### Step 4: Consider both cases for \(\mathbf{\omega}\) 1. **Case 1**: If \(\mathbf{\omega} = \hat{k}\): \[ \mathbf{v} = \left(\frac{1}{\sqrt{2}} \hat{i} + \hat{j}\right) \times \hat{k} \] Using the right-hand rule for the cross product: \[ \hat{i} \times \hat{k} = -\hat{j}, \quad \hat{j} \times \hat{k} = \hat{i} \] Therefore, \[ \mathbf{v} = \frac{1}{\sqrt{2}}(-\hat{j}) + \hat{i} = \frac{1}{\sqrt{2}} \hat{i} - \hat{j} \] 2. **Case 2**: If \(\mathbf{\omega} = -\hat{k}\): \[ \mathbf{v} = \left(\frac{1}{\sqrt{2}} \hat{i} + \hat{j}\right) \times (-\hat{k}) \] This gives: \[ \mathbf{v} = -\left(\frac{1}{\sqrt{2}}(-\hat{j}) + \hat{i}\right) = \frac{1}{\sqrt{2}} \hat{j} - \hat{i} \] ### Step 5: Conclusion Thus, the velocity of the particle can either be: \[ \mathbf{v} = \frac{1}{\sqrt{2}} \hat{i} - \hat{j} \quad \text{or} \quad \mathbf{v} = \frac{1}{\sqrt{2}} \hat{j} - \hat{i} \] This indicates that the velocity vector is along the directions of these two vectors. ### Final Answer The velocity of the particle is along either: 1. \(\frac{1}{\sqrt{2}} \hat{i} - \hat{j}\) 2. \(\frac{1}{\sqrt{2}} \hat{j} - \hat{i}\)
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