Elliptical Orbit (2)

Suppose we detected an object in the Solar System orbiting the Sun. It is following an elliptical orbit, but we don't know where its perihelion is, so when it was detected, we do not actually know the value of its true anomay. So we assign it a value \(\theta_1\).

Five Points of Ellipse

At intervals of \(15^{\circ}\) we measure its distance r from the Sun. The true anomaly is decreasing as it is moving closer, so we subtract 15, 30, 45 and 60 degrees from \(\theta_1\).

label distance r
(AU)
angle
(degrees)
$$r_1$$$$100$$$$\theta_1$$
$$r_2$$$$86.15$$$$\theta_1 - 15$$
$$r_3$$$$75$$$$\theta_1 - 30$$
$$r_4$$$$66.41$$$$\theta_1 - 45$$
$$r_5$$$$60$$$$\theta_1 - 60$$

The equation of ellipse

$$ r= \frac{a(1-e^2)}{1+e \cos \theta} $$ has four unknowns:

distance r

semimajor axis a,

eccentricity e,

true anomaly θ1.

To find the values, we need at least four simultaneous equations. Maybe even five. They are:

$$ r_1 = \frac{a(1-e^2)}{1+e \cos \theta_1 } = 100 $$ $$ r_2 = \frac{a(1-e^2)}{1+e \cos (\theta_1 - 15^\circ)} = 86.15 $$ $$ r_3 = \frac{a(1-e^2)}{1+e \cos (\theta_1 - 30^\circ)} =75 $$ $$ r_4 = \frac{a(1-e^2)}{1+e \cos (\theta_1 - 45^\circ)} = 66.41 $$ $$ r_5 = \frac{a(1-e^2)}{1+e \cos (\theta_1 - 60^\circ)} = 60 $$
The calculations. Click if you want to see them.

We can start by \(r_1 \div r_3\) $$ \frac{100}{75}= \frac{1 + e \cos (\theta_1 -30^o)}{1+ e \cos \theta_1} $$ with the use of $$ \cos(A-B) = \cos A \cos B + \sin A \sin B $$ we arrive with Eq A: $$ 1+ 1.4 e \cos \theta_1 = 1.5 e \sin \theta_1 $$

Similarly \(r_3 \div r_5 \), we get Eq B:

$$ 1+2.33 e \cos \theta_1 = 0.96 e \sin \theta_1 $$

Dividing Eq A with Eq B and rearranging, eventually we get:

$$ e \cos \theta_1 = -0.25 $$

Substituting back into r1:

$$ r_1 = \frac{a(1-e^2)}{1+e \cos \theta_1 } = 100 $$ $$ a(1 -e^2) = 75 $$

Substituting \(e \cos \theta_1= -0.25\) into r4 and combining them


We get $$ \tan \theta_1 = -\sqrt{3} $$

There are two possible values of θ1:

$$ \theta_1 = 120^{\circ}, 300^{\circ} $$.

The value that makes sense is $$ \theta_1 = 120^{\circ} $$

With θ1 known, everything else falls into place. We can use r1 and r3

$$ r_1 = \frac{a(1-e^2)}{1+e \cos 120^{\circ} } = 100 $$ $$ r_3 = \frac{a(1-e^2)}{1+e \cos 90^{\circ} } = 75 $$ and find that eccentricity is $$ e = 0.5$$ and semimajor axis is $$ a = 100 $$

With a and e known, we have described the elliptical orbit of the object. $$ r = \frac{75}{1+ 0.5 \cos \theta } $$

Periapsis/Perihelion is at θ= 0, giving us rper = 50 A.U.

Apoapsis/Aphelion is at θ = 180o, giving us rap = 150 A.U.

The semi-minor axis b is obtained $$ e^2 = 1 - \frac{b^2}{a^2} $$ $$ b =\sqrt{ 100^2( 1 - 0.5^2 )} $$ $$ b = 86.6 \mathrm{ A.U.} $$


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