Proving Elliptical Trajectory Acceleration Vector Passes Through Focus

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The discussion centers on proving that the acceleration vector of a particle following an elliptical trajectory passes through the focus of the ellipse. The position vector is defined by the equations x=acos[pt] and y=bsin[pt], leading to an acceleration vector of a=-p²r, which points towards the center of the coordinate system rather than the focus. Participants express confusion about whether the provided equations accurately represent the motion of a planet, suggesting they may not align with Kepler's first law. Clarification is sought on the correct equations needed to demonstrate the desired proof. The conversation emphasizes the need for accurate representations of elliptical motion to validate the claim.
aim1732
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If a particle's trajectory is defined by the law x=acos[pt] and y=bsin[pt] where t is parameter of time then we have to prove that it's acceleration vector passes through the focus of the conic----ellipse in this case as can be clearly seen.
If we write out the position vector in the vector notation and differentiate twice we get a=-p2r and this clearly is directed towards the centre of the axes system and not the focus.Any ideas?
 
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aim1732 said:
If we write out the position vector in the vector notation and differentiate twice we get a=-p2r and this clearly is directed towards the centre of the axes system and not the focus.
Correct.

Any ideas?
Ideas regarding what? I assume you are trying to prove Kepler's first law. The given equation does not describe a planet's motion. You need to find the right equation.
 
have to prove that it's acceleration vector passes through the focus of the conic----ellipse in this case as can be clearly seen.

I meant this.
 

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