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A particle moves in a plane such that it...

A particle moves in a plane such that its coordinates changes with time as `x = at` and `y = bt`, where a and b are constants. Find the position vector of the particle and its direction at any time t.

A

`(a) hati + (bt) hatj`

B

`(at) hati + (b) hatj`

C

`(at) hati + (bt) hatj`

D

`(a) hati + (b) hatj`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the position vector of the particle and its direction at any time \( t \). ### Step-by-Step Solution: 1. **Identify the given equations**: The coordinates of the particle are given as: \[ x = at \] \[ y = bt \] where \( a \) and \( b \) are constants. 2. **Write the position vector**: The position vector \( \mathbf{r} \) of the particle in a two-dimensional plane can be expressed in terms of its coordinates \( x \) and \( y \): \[ \mathbf{r} = x \hat{i} + y \hat{j} \] Substituting the expressions for \( x \) and \( y \): \[ \mathbf{r} = (at) \hat{i} + (bt) \hat{j} \] Thus, the position vector becomes: \[ \mathbf{r} = at \hat{i} + bt \hat{j} \] 3. **Determine the direction of the particle**: The direction of the particle can be described by the angle \( \theta \) it makes with the x-axis. This angle can be found using the tangent function: \[ \tan(\theta) = \frac{y}{x} \] Substituting the expressions for \( x \) and \( y \): \[ \tan(\theta) = \frac{bt}{at} = \frac{b}{a} \] 4. **Find the angle \( \theta \)**: To find \( \theta \), we take the inverse tangent: \[ \theta = \tan^{-1}\left(\frac{b}{a}\right) \] ### Final Answer: - The position vector of the particle at any time \( t \) is: \[ \mathbf{r} = at \hat{i} + bt \hat{j} \] - The direction of the particle at any time \( t \) is given by the angle: \[ \theta = \tan^{-1}\left(\frac{b}{a}\right) \]

To solve the problem, we need to find the position vector of the particle and its direction at any time \( t \). ### Step-by-Step Solution: 1. **Identify the given equations**: The coordinates of the particle are given as: \[ x = at ...
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