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A particle moves in the x-y plane under ...

A particle moves in the x-y plane under the action of a force `vecF` such that the value of its linear momentum `vecP` at any time t is `P_(x)=2` cost and `p_(y)=2sint`. What is the angle `theta` between `vecF` and P at a given time t?

A

`90^(@)`

B

`0^(@)`

C

`180^(@)`

D

`30^(@)`

Text Solution

AI Generated Solution

The correct Answer is:
To solve the problem, we need to find the angle \( \theta \) between the force vector \( \vec{F} \) and the momentum vector \( \vec{P} \) at any time \( t \). ### Step-by-Step Solution: 1. **Define the momentum vector \( \vec{P} \)**: - Given: \[ P_x = 2 \cos t, \quad P_y = 2 \sin t \] - Therefore, the momentum vector can be expressed as: \[ \vec{P} = 2 \cos t \, \hat{i} + 2 \sin t \, \hat{j} \] 2. **Calculate the force vector \( \vec{F} \)**: - The force is defined as the rate of change of momentum: \[ \vec{F} = \frac{d\vec{P}}{dt} \] - Differentiate \( \vec{P} \): \[ \frac{dP_x}{dt} = \frac{d}{dt}(2 \cos t) = -2 \sin t \] \[ \frac{dP_y}{dt} = \frac{d}{dt}(2 \sin t) = 2 \cos t \] - Thus, the force vector is: \[ \vec{F} = -2 \sin t \, \hat{i} + 2 \cos t \, \hat{j} \] 3. **Use the dot product to find the angle \( \theta \)**: - The dot product \( \vec{F} \cdot \vec{P} \) is given by: \[ \vec{F} \cdot \vec{P} = (-2 \sin t)(2 \cos t) + (2 \cos t)(2 \sin t) \] - Simplifying this: \[ \vec{F} \cdot \vec{P} = -4 \sin t \cos t + 4 \sin t \cos t = 0 \] 4. **Relate the dot product to the angle**: - The formula for the dot product in terms of the angle is: \[ \vec{F} \cdot \vec{P} = |\vec{F}| |\vec{P}| \cos \theta \] - Since \( \vec{F} \cdot \vec{P} = 0 \), we have: \[ |\vec{F}| |\vec{P}| \cos \theta = 0 \] - This implies: \[ \cos \theta = 0 \] 5. **Determine the angle \( \theta \)**: - The angle \( \theta \) for which \( \cos \theta = 0 \) is: \[ \theta = \frac{\pi}{2} \text{ radians} = 90^\circ \] ### Conclusion: The angle \( \theta \) between the force \( \vec{F} \) and the momentum \( \vec{P} \) at any time \( t \) is \( 90^\circ \).
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