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If M is mass of rocket, r is rate of eje...

If M is mass of rocket, r is rate of ejection of gases and u is velocity of gases with respect to rocket then acceleration of the rocket dv/dt is equal to

A

`(ru)/(M -rt)`

B

`(M-rt)/(ru)`

C

`(ru)/(M+rt)`

D

`(ru)/(M)`

Text Solution

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The correct Answer is:
To find the acceleration of the rocket, we can use the concept of thrust force and the relationship between mass, velocity, and acceleration. Let's break down the solution step by step. ### Step-by-Step Solution: 1. **Understanding the Variables**: - Let \( M \) be the initial mass of the rocket. - Let \( r \) be the rate of ejection of gases (mass flow rate). - Let \( u \) be the velocity of the gases with respect to the rocket. 2. **Thrust Force**: - The thrust force (\( F \)) generated by the rocket can be expressed as: \[ F = u \cdot \frac{dm}{dt} \] - Here, \( \frac{dm}{dt} \) is the rate of change of mass, which is equal to \(-r\) (since the mass is decreasing). 3. **Applying Newton's Second Law**: - According to Newton's second law, the acceleration (\( a \)) of the rocket can be expressed as: \[ a = \frac{F}{m} \] - Substituting the expression for thrust force into this equation gives: \[ a = \frac{u \cdot (-r)}{M - rt} \] - Here, \( M - rt \) represents the mass of the rocket at time \( t \) after \( rt \) mass has been expelled. 4. **Final Expression for Acceleration**: - Therefore, the acceleration of the rocket can be expressed as: \[ \frac{dv}{dt} = \frac{-ur}{M - rt} \] ### Final Answer: The acceleration of the rocket is given by: \[ \frac{dv}{dt} = \frac{-ur}{M - rt} \]

To find the acceleration of the rocket, we can use the concept of thrust force and the relationship between mass, velocity, and acceleration. Let's break down the solution step by step. ### Step-by-Step Solution: 1. **Understanding the Variables**: - Let \( M \) be the initial mass of the rocket. - Let \( r \) be the rate of ejection of gases (mass flow rate). - Let \( u \) be the velocity of the gases with respect to the rocket. ...
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