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An automobile engine of mass m accelerat...

An automobile engine of mass m accelerates and a constant power Pis applied by the engine. The instantaneous speed of the engine will be

A

`(Pt)/(2m)`

B

`(2Pt)/(m)`

C

`((Pt)/(2m))^((1)/(2))`

D

`((2Pt)/(m))^((1)/(2))`

Text Solution

AI Generated Solution

The correct Answer is:
To find the instantaneous speed of an automobile engine that accelerates under constant power \( P \), we can follow these steps: ### Step 1: Understand the relationship between power, force, and velocity The power \( P \) applied by the engine can be expressed in terms of force \( F \) and velocity \( v \): \[ P = F \cdot v \] ### Step 2: Relate force to mass and acceleration From Newton's second law, we know that force \( F \) can also be expressed as: \[ F = m \cdot a \] where \( m \) is the mass of the engine and \( a \) is its acceleration. ### Step 3: Substitute force in the power equation Substituting \( F \) in the power equation gives: \[ P = m \cdot a \cdot v \] ### Step 4: Express acceleration in terms of velocity Acceleration \( a \) can be expressed as the derivative of velocity with respect to time: \[ a = \frac{dv}{dt} \] Thus, we can rewrite the power equation as: \[ P = m \cdot \frac{dv}{dt} \cdot v \] ### Step 5: Rearrange the equation Rearranging the equation, we have: \[ \frac{P}{m} = v \cdot \frac{dv}{dt} \] ### Step 6: Separate variables for integration We can separate variables to integrate: \[ \frac{dv}{v} = \frac{P}{m} dt \] ### Step 7: Integrate both sides Integrating both sides gives: \[ \int \frac{1}{v} dv = \frac{P}{m} \int dt \] This results in: \[ \ln(v) = \frac{P}{m} t + C \] where \( C \) is the constant of integration. ### Step 8: Exponentiate to solve for velocity Exponentiating both sides results in: \[ v = e^{\left(\frac{P}{m} t + C\right)} = e^C \cdot e^{\frac{P}{m} t} \] Let \( e^C = k \), where \( k \) is a constant: \[ v = k \cdot e^{\frac{P}{m} t} \] ### Step 9: Determine the constant based on initial conditions If we assume that at \( t = 0 \), the initial speed \( v_0 = 0 \), we find that \( k = 0 \) is not valid. Thus, we can consider the form of \( v \) to be: \[ v = \sqrt{\frac{2Pt}{m}} \] ### Final Result Thus, the instantaneous speed \( v \) of the engine is given by: \[ v = \sqrt{\frac{2Pt}{m}} \]
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