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A particle of mass 'm' is moving along a...

A particle of mass 'm' is moving along a circle of radius 'r'. At some instant, its speed is 'v' and it is gaining speed at a uniform rate'a', then, at the given instant, acceleration of the particle is :

A

along the radius

B

inclined to radius at `theta="sin"^(-1)(1)/([1+(v^(4))/(a^(2)r^(2))]^(1//2))`

C

inclined to radius at `theta=cos^(-1)(ar)/(v^(2))`

D

inclined to radius at `theta=tan^(-1)(v^(2))/(ar)`

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The correct Answer is:
To find the acceleration of a particle moving in a circular path with a given speed and a uniform rate of acceleration, we can break down the problem into steps. ### Step-by-Step Solution: 1. **Identify the Components of Acceleration**: - The particle has two components of acceleration: - **Centripetal Acceleration (a_c)**: This is due to the circular motion and is directed towards the center of the circle. It can be calculated using the formula: \[ a_c = \frac{v^2}{r} \] where \( v \) is the speed of the particle and \( r \) is the radius of the circle. 2. **Determine Tangential Acceleration (a_t)**: - The particle is gaining speed at a uniform rate \( a \). This tangential acceleration is given as: \[ a_t = a \] where \( a \) is the uniform rate of acceleration. 3. **Calculate the Net Acceleration (a_net)**: - The total or net acceleration of the particle can be found using the Pythagorean theorem, since the tangential and centripetal accelerations are perpendicular to each other: \[ a_{net} = \sqrt{a_t^2 + a_c^2} \] - Substituting the values of \( a_t \) and \( a_c \): \[ a_{net} = \sqrt{a^2 + \left(\frac{v^2}{r}\right)^2} \] 4. **Final Expression**: - Therefore, the expression for the acceleration of the particle at the given instant is: \[ a_{net} = \sqrt{a^2 + \frac{v^4}{r^2}} \] ### Final Answer: The acceleration of the particle is: \[ a_{net} = \sqrt{a^2 + \frac{v^4}{r^2}} \]
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