Change orbit from circle to parabola

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SUMMARY

The discussion focuses on the mechanics of changing a spaceship's orbit from circular to parabolic by applying a thrust. The key factor, denoted as f, represents the increase in speed required for this transition when thrust is applied tangentially. The participants utilize Kepler's laws and equations related to energy and angular momentum to derive the necessary conditions for this orbital change. Additionally, they explore the implications of thrust direction on the distance of closest approach.

PREREQUISITES
  • Understanding of orbital mechanics, specifically circular and parabolic orbits.
  • Familiarity with Kepler’s laws of planetary motion.
  • Knowledge of kinetic energy and potential energy equations in gravitational fields.
  • Concepts of angular momentum and its role in orbital dynamics.
NEXT STEPS
  • Study the derivation of energy equations for circular and parabolic orbits.
  • Learn about the effects of thrust direction on orbital mechanics.
  • Investigate the relationship between angular momentum and orbital shape changes.
  • Explore numerical simulations of orbital transitions using software like MATLAB or Python.
USEFUL FOR

Aerospace engineers, physics students, and anyone interested in orbital mechanics and spacecraft trajectory optimization will benefit from this discussion.

athrun200
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1(a) Homework Statement

A spaceship travels in a circular orbit around a planet. It applies a sudden
thrust and increases its speed by a factor f . If the goal is to change the
orbit from a circle to a parabola, what should f be if the thrust points in the tangential direction?

1(b) Is your answer any different if the thrust points
in some other direction? What is the distance of closest approach if the
thrust points in the radial direction?


Homework Equations


Kepler’s laws


The Attempt at a Solution


We know that for circle, ε=0; for parabola ε=1
We also know that ε=\sqrt{1+\frac{2EL^{2}}{m\alpha^{2}}}
So E=-\frac{m\alpha^{2}}{2L^{2}} for ε=0
E=0 for ε=1

But I don't know what to do next in order to find the increased factor f
 
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Hello. Could you please define the symbols ##\alpha## and ##L##?

Can you express the kinetic energy of the ship in terms of ##m##, ##\alpha## and ##L## before and after the thrust?
 
Last edited:
TSny said:
Hello. Could you please define the symbols ##\alpha## and ##L##?

Can you express the kinetic energy of the ship in terms of ##m##, ##\alpha## and ##L## before and after the thrust?

V(r)=-\frac{\alpha}{r}
So \alpha=GMm

L is angular momentum.

I think it is possible to express KE in terms of m and L but not \alpha.
But what should I do next?
 
athrun200 said:
V(r)=-\frac{\alpha}{r}
So \alpha=GMm

L is angular momentum.

I think it is possible to express KE in terms of m and L but not \alpha.
But what should I do next?

ok. Express kinetic energy in terms of ##\alpha## and ##r## using E= KE + V
You can assume ##r## remains constant during the thrust. So you should be able to relate initial and final speeds since you know how E changes. Instead of expressing E in terms of L, try to express E in terms of r for a circular orbit.
 

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