These are parametric equations for the Keplerian orbit of a planet: tan(phi/2) =
ID: 2117922 • Letter: T
Question
These are parametric equations for the Keplerian orbit of a planet:
tan(phi/2) = sqrt{(1+e)/(1-e)} tan(psi/2)
r = a ( 1 -e cos(psi)) and t = ( T/ 2pi) (psi- e sin(psi))
Here (r,phi) are plane polar coordinates, t is time, and psi is an independent variable parameter. Also, T = period of revolution, a = semimajor axis, and e= eccentricity.
(A) Determine the Cartesian coordinates (x,y) and time t for the point P shown on the figure. (Express the answers in terms of a, e, T.)
(B) Determine the Cartesian coordinates (x,y) and time t for the point R shown on the figure. (Express the answers in terms of a, e, T.)
(C) Determine L/m where L is the angular momentum of the planet, and m is its mass. (Express the answer in terms of a, e, T.)
Explanation / Answer
tan(q/2) = sqrt{(1+e)/(1-e)}tan(k/2)
r = a(1-e cosk)
t = (T/2pi) (k-e sink).
We restrict our attention to just one revolution through the orbit, starting from P, so k varies in between [0,2pi].
(A)
Point P is on the positive x-axis and a is semi-major axis.
So P = (a(1-e),0). (distance from center of ellipse to endpoint on major axis is a and the distance from center of ellipse to focus is ae, so distance between endpoint and nearest focus is a-ae = a(1-e)
=> a(1-e) = r = a(1-e cosk)
=> cos k = 1.
Also q = 0 => 0 = tan(q/2) = sqrt{(1+e)/(1-e)}tan(k/2)
=> tan(k/2) = 0.
The two equations above imply k = 0.
So time t = 0 s. (agreeing with our assumption that revolution starts at P).
Also note that when the planet returns to P, we have k = 2pi....(Observation).This is because for P k = 0, 2pi, 4pi,...
(B)
From the figure and the details of the ellipse
R = (0,ae.sqrt{1-e^2}) (for an ellipse with semimajor axis a, eccentricity e,
Thus r = ae.sqrt{1-e^2}
=> ae.sqrt{1-e^2} = r = a(1-e cosk)
=> cos k = (1/e) - sqrt{1-e^2}.
Also q = pi/2
=> 1 = tan q/2 = sqrt{(1+e)/(1-e)}tan(k/2)
From the above two we get k is in [0,pi),
k = 2 arctan(sqrt{(1-e)/(1+e)}).
So time t = (T/2pi) (k-e sink).
= (T/2pi) (2 arctan(sqrt{(1-e)/(1+e)}) - e sin(2 arctan(sqrt{(1-e)/(1+e)})).
(C)
We have from our physics that angular momentum is conserved for a planetory motion.
so To find angular velocity we need to divide 2pi, the total revolution angle by its time period T.
So L = m.(2pi/T).
=> L/m = 2pi/T.
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