Problem 113
Question
A Multistage Rocket. Suppose the first stage of a two-stage rocket has total mass \(12,000 \mathrm{kg},\) of which 9000 \(\mathrm{kg}\) is fuel. The total mass of the second stage is \(1000 \mathrm{kg},\) of which 700 \(\mathrm{kg}\) is fuel. Assume that the relative speed \(v_{\text { cx }}\) of ejected material is constant, and ignore any effect of gravity. The effect of gravity is small during the firing period if the rate of fuel consumption is large.) (a) Suppose the entire fuel supply carried by the two-stage rocket is utilized in a single-stage rocket with the same total mass of \(13,000 \mathrm{kg} .\) In terms of \(v_{\mathrm{cx}},\) what is the speed of the rocket, starting from rest, when its fuel is exhausted? (b) For the two-stage rocket, what is the speed when the fuel of the first stage is exhausted if the first stage carries the second stage with it to this point? This speed then becomes the initial speed of the second stage. At this point, the second stage separates from the first stage. (c) What is the final speed of the second stage? (d) What value of \(v_{\mathrm{ex}}\) is required to give the second stage of the rocket a speed of 7.00 \(\mathrm{km} / \mathrm{s} ?\)
Step-by-Step Solution
VerifiedKey Concepts
Rocket Equation
\[ v = v_{\text{ex}} \ln \left( \frac{M_i}{M_f} \right) \]where:
- \( v \) is the final velocity of the rocket,
- \( v_{\text{ex}} \) is the exhaust velocity of the ejected material,
- \( M_i \) is the initial total mass (rocket plus fuel), and
- \( M_f \) is the final mass (rocket without fuel).
Understanding this helps predict how fast the rocket will travel when the fuel is depleted. It emphasizes the importance of the mass ratio (\( \frac{M_i}{M_f} \)) and the exhaust velocity in achieving high speeds.
Fuel Consumption Calculation
The fuel mass is the main factor reducing the rocket's mass over time as it is consumed. For the entire rocket in this case:
- Stage One Fuel: \( 9,000 \text{ kg} \)
- Stage Two Fuel: \( 700 \text{ kg} \)
- Total Fuel Mass: \( 9,700 \text{ kg} \)
Exhaust Velocity
In our scenario, this velocity remains constant and is essential in calculating the rocket's final speeds. Using the rocket equation:\[ v = v_{\text{ex}} \ln \left( \frac{M_i}{M_f} \right) \]we see that higher \( v_{\text{ex}} \) leads to a greater velocity change for a given fuel mass ratio.By comparing scenarios (single-stage and two-stage), exhaust velocity helps us understand how best to utilize fuel: reducing the amount needed for the desired speed or increasing the final speed possible with a given fuel mass. The required exhaust velocity to achieve a specific speed is an essential calculation when designing a rocket’s propulsion system.
Two-Stage Rocket Dynamics
For our example, the first stage carries both stages initially, consuming its 9,000 kg of fuel, leaving a remaining mass of 4,000 kg:\[ v = v_{\text{ex}} \ln \left( \frac{13,000}{4,000} \right) \]The separation of stages means less mass for the second stage to accelerate, which is beneficial for reaching higher velocities with the remaining fuel. Next, the final speed of the second stage is calculated using its initial speed plus the additional speed gained by burning its own fuel.
Designing rockets using multiple stages is a strategic way to reduce weight as each part has finished its role, adapting to the changing mass by recalculating velocities specific to each stage. This staging allows rockets to achieve speeds and altitudes that a single-stage configuration could not match with the same fuel.