Problem : 
In Solving the Orbits we derived the 
equation:
From this, derive the expression we stated for 
1/r.  Hint: Define 
y = 1/r 
and use the fact that 
 = -
 = - 
.  
Making the 
y substitution, we have:
We can then complete the square on the right-hand side and we have:
Then we let 
p = y - 
 and we have:
where we have just defined 
C in terms of the constant 
E, G, M, m, L.  We can 
now separate variables:
|   =  dθ'âácos-1(p'/  )|pp1 = θ - θ1âáp =  cos  (θ - θ1) - cos-1(p1/  )  =  cos(θ - θ0) |  | 
 
Finally, recalling 
p = (1/r) - 
, and we can pick an axis such 
that 
θ0 = 0:
The quantity under the radical is defined a 
ε, the eccentricity. 
 
Problem : 
Using the expression we derived for (1/r), show that this reduces to x2 = y2 = k2 -2kεx + ε2x2, where k =  , 
ε =
, 
ε =  , and cosθ = x/r.
, and cosθ = x/r.
We have:
|  =  (1 + εcosθ)âá1 =  (1 + ε  )âák = r + εx |  | 
 
We can solve for 
r and then use 
r2 = x2 + y2:
which is the result we wanted.
 
Problem : 
For 0 < ε < 1, use the above equation to derive the equation for an 
elliptical orbit.  What are the semi-major and semi-minor axis lengths?  Where 
are the foci?
We can rearrange the equation to 
(1 - ε2)x2 +2kεx + y2 = k2.  We can divide through by 
(1 - ε2) and complete the square in x:
Rearranging this equation into the standard form for an ellipse we have:
|  +  = 1 |  | 
 
This is an ellipse with one foci at the origin, the other at 
( , 0)
, 0), semi-major axis length 
a = 
 and semi-minor axis length 
b = 
.  
 
Problem : 
What is the energy difference between a circular earth orbit of radius 7.0×103 kilometers and an elliptical earth orbit with apogee 5.8×103 kilometers and perigee 4.8×103 kilometers.  The mass 
of the satellite in question is 3500 kilograms and the mass of the earth is 
5.98×1024 kilograms.  
The energy of the circular orbit is given by 
E = -  = 9.97×1010
 = 9.97×1010 Joules.  The equation used here can also be applied to elliptical 
orbits with 
r replaced by the semimajor axis length 
a.  The semimajor axis 
length is found from 
a =  = 5.3×106
 = 5.3×106 meters.  Then 
E = -  = 1.32×1011
 = 1.32×1011 Joules.  
The energy of the elliptical orbit is higher.  
 
Problem : 
If a comet of mass 6.0×1022 kilograms has a hyperbolic orbit around 
the sun of eccentricity
ε = 1.5, what is its closest distance 
of approach to the sun in terms of its angular momentum (the mass of the sun is 
1.99×1030
kilograms)?
Its closest approach is just 
rmin, which is given by:
| rmin =  = (6.44×10-67)L2 |  |