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A rocket of initial mass m0 has a mass m...

A rocket of initial mass `m_0` has a mass `m_0(1-t//3)` at time t. The rocket is lauched from rest vertically upwards under gravity and expels burnt fuel at a speed u relative to the rocket vertically downward. Find the speed of rocket at `t=1`.

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To solve the problem, we need to find the speed of the rocket at time \( t = 1 \) second. We will use the principles of conservation of momentum and the given mass function of the rocket. ### Step-by-Step Solution: 1. **Identify the Initial Conditions**: - The initial mass of the rocket is \( m_0 \). - The mass of the rocket at time \( t \) is given by \( m(t) = m_0 \left(1 - \frac{t}{3}\right) \). - The rocket is launched from rest, so the initial velocity \( v_0 = 0 \). 2. **Determine the Mass at \( t = 1 \)**: - Substitute \( t = 1 \) into the mass function: \[ m(1) = m_0 \left(1 - \frac{1}{3}\right) = m_0 \left(\frac{2}{3}\right) = \frac{2m_0}{3} \] 3. **Relative Speed of Fuel Expulsion**: - The speed of the expelled fuel relative to the rocket is \( u \) downward. Therefore, the speed of the expelled fuel with respect to the ground is \( v_r = v - u \), where \( v \) is the speed of the rocket. 4. **Apply Conservation of Momentum**: - The momentum before and after the fuel is expelled must be equal. Initially, the momentum is \( m_0 \cdot 0 = 0 \). - After expelling a small amount of fuel \( dm \), the momentum is: \[ m(t) v + dm (v - u) = 0 \] - Rearranging gives: \[ m(t) v = -dm (v - u) \] 5. **Express \( dm \)**: - The change in mass \( dm \) over a small time \( dt \) can be expressed as: \[ dm = -\frac{m_0}{3} dt \] - This is derived from the mass function since the mass decreases linearly with time. 6. **Substitute \( dm \) into the Momentum Equation**: - Substitute \( m(t) \) and \( dm \): \[ \frac{2m_0}{3} v = -\left(-\frac{m_0}{3}\right) (v - u) \] - Simplifying gives: \[ \frac{2m_0}{3} v = \frac{m_0}{3} (v - u) \] 7. **Solve for \( v \)**: - Cancel \( m_0/3 \) from both sides: \[ 2v = v - u \] - Rearranging gives: \[ v + u = 0 \implies v = -u \] 8. **Calculate the Speed at \( t = 1 \)**: - Substitute \( t = 1 \) into the expression for speed: \[ v = -u \ln\left(\frac{3}{2}\right) - g \] - The final expression for the speed of the rocket at \( t = 1 \) second is: \[ v = u \ln\left(\frac{3}{2}\right) - g \] ### Final Result: The speed of the rocket at \( t = 1 \) second is: \[ v = u \ln\left(\frac{3}{2}\right) - g \]

To solve the problem, we need to find the speed of the rocket at time \( t = 1 \) second. We will use the principles of conservation of momentum and the given mass function of the rocket. ### Step-by-Step Solution: 1. **Identify the Initial Conditions**: - The initial mass of the rocket is \( m_0 \). - The mass of the rocket at time \( t \) is given by \( m(t) = m_0 \left(1 - \frac{t}{3}\right) \). - The rocket is launched from rest, so the initial velocity \( v_0 = 0 \). ...
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