Multistage continuous Rocket Eqn

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SUMMARY

The discussion focuses on the application of the Tsiolkovsky rocket equation to multistage rockets that discard structural and engine mass continuously at zero velocity relative to the rocket. Two primary assumptions are presented: one where mass is ejected in discrete chunks and another where mass is dropped continuously in proportion to burnt fuel. The effective exhaust velocity is calculated by multiplying the exhaust mass flow rate by the exhaust velocity and dividing by the combined ejection rate, allowing for precise modeling of the rocket's motion.

PREREQUISITES
  • Understanding of the Tsiolkovsky rocket equation
  • Knowledge of momentum conservation principles
  • Familiarity with mass flow rates in rocket propulsion
  • Basic concepts of multistage rocket design
NEXT STEPS
  • Study the derivation and applications of the Tsiolkovsky rocket equation
  • Explore momentum conservation in rocket propulsion systems
  • Research continuous mass ejection techniques in rocket design
  • Analyze case studies of multistage rockets and their performance metrics
USEFUL FOR

Aerospace engineers, rocket scientists, and students studying propulsion systems who are interested in advanced rocket motion modeling and multistage design principles.

syncphysics99
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So if you have a rocket let's say that discards all the structural and engine mass continuously at zero velocity that is relative to the rocket until only the payload is traveling at the final velocity - then what will the equation of motion will look like? we can neglect the drag and gravitational losses.
 
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syncphysics99 said:
So if you have a rocket let's say that discards all the structural and engine mass continuously at zero velocity that is relative to the rocket until only the payload is traveling at the final velocity - then what will the equation of motion will look like? we can neglect the drag and gravitational losses.
You could make either of two assumptions.

1. The structure and engine mass are ejected in discrete chunks. i.e. stage 1 is burned out over time then the useless structure and engine are discarded instantly. In this case you can apply the Tsiolkovsky rocket equation piecewise over each burn.

2. The structure and engine mass are dropped continuously and in proportion to the burnt fuel/ejected reaction mass. In this case you can multiply the exhaust mass flow rate by the exhaust velocity to get a momentum ejection rate. Then divide by the combined (and proportional!) engine+superstructure ejection rate to get an "effective exhaust velocity". Plug that into the Tsiolkovsky rocket equation applied over the total burn.
 

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