Satellite Reentry: Examining Newtonian Gravity

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The discussion on satellite reentry emphasizes the dual influences of gravitational forces and atmospheric drag on a satellite's descent from high orbit. Newtonian gravity, described by the equation g = GM/r^2, plays a crucial role as both gravity and air resistance change with altitude and speed. The atmosphere provides variable resistance that opposes the satellite's velocity, complicating reentry dynamics. Additionally, factors like temperature may also affect air resistance. Overall, the complexities of reentry require practical equations to accurately model these interactions.
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The path of a satellite reentering the atmosphere from a very high orbit has two components, one gravitational and the other from the atmosphere. Could there be a discussion of the two separate components using Newtonian gravity with gravity as:

g = GM/r^2

that change with elevation as a function of time.
 
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There may also be a velocity component from the satellite's rotational velocity...anyway the atmosphere acts as a variable resistance (drag) in a direction opposite the velocity.

the complication is that air resistance and gravity vary with altitude and air resistance varies with speed...and likely with temperature as well...

Try wikipedia,
http://en.wikipedia.org/wiki/Orbital_spaceflight

and see "RE-ENTRY for a brief discussion of some practical considerations...it's not a simple theoretical situation underlying your question. For one thing, a satellite in free fall will burn up...

There are practical equations for computing air resistance...I researched some for wind force on a boat while anchored...it varied as the square of wind speed...people had computed/measured constants for different boat shapes...
 
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