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A self-propelled vehicle of mass m, whos...

A self-propelled vehicle of mass m, whose engine delivers a constant power P, has an acceleration `a = (P//mv)`. (Assume that there is no friction). In order to increase its velocity from `v_(1)` to `v_(2)`, the distan~e it has to travel will be:

A

`(3P)/(m)(v_(2)^(2)-v_(1)^(2))`

B

`(m)/(3P)(v_(2)-v_(1))`

C

`(m)/(3P)(v_(2)^(3)-v_(1)^(3))`

D

`(m)/(3P)(v_(2)^(2)-v_(1)^(2))`

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The correct Answer is:
To solve the problem of finding the distance a self-propelled vehicle must travel to increase its velocity from \( v_1 \) to \( v_2 \), given that its engine delivers a constant power \( P \) and has an acceleration defined by \( a = \frac{P}{mv} \), we can follow these steps: ### Step-by-Step Solution: 1. **Understanding the Relationship**: The acceleration \( a \) can be expressed in terms of velocity \( v \) and time \( t \) as: \[ a = \frac{dv}{dt} \] Given that \( a = \frac{P}{mv} \), we can equate the two expressions for acceleration. 2. **Rearranging the Equation**: We can rearrange the equation: \[ \frac{dv}{dt} = \frac{P}{mv} \] Now, we can multiply both sides by \( dt \) and \( v \): \[ v \, dv = \frac{P}{m} \, dt \] 3. **Using the Chain Rule**: We can express \( dt \) in terms of \( dx \) (distance): \[ dt = \frac{dx}{v} \] Substituting this into our equation gives: \[ v \, dv = \frac{P}{m} \frac{dx}{v} \] Rearranging this leads to: \[ v^2 \, dv = \frac{P}{m} \, dx \] 4. **Integrating Both Sides**: Now we can integrate both sides. The left side will be integrated with respect to \( v \) from \( v_1 \) to \( v_2 \), and the right side will be integrated with respect to \( x \) from \( x_1 \) to \( x_2 \): \[ \int_{v_1}^{v_2} v^2 \, dv = \frac{P}{m} \int_{x_1}^{x_2} dx \] 5. **Calculating the Integrals**: The integral of \( v^2 \) is: \[ \frac{v^3}{3} \bigg|_{v_1}^{v_2} = \frac{v_2^3}{3} - \frac{v_1^3}{3} \] The integral of \( dx \) is simply: \[ x \bigg|_{x_1}^{x_2} = x_2 - x_1 \] 6. **Setting Up the Equation**: Now we can set up the equation: \[ \frac{v_2^3 - v_1^3}{3} = \frac{P}{m} (x_2 - x_1) \] 7. **Solving for Distance**: Rearranging gives us the distance traveled: \[ x_2 - x_1 = \frac{m}{3P} (v_2^3 - v_1^3) \] ### Final Result: Thus, the distance \( d \) that the vehicle must travel to increase its velocity from \( v_1 \) to \( v_2 \) is: \[ d = \frac{m}{3P} (v_2^3 - v_1^3) \]
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