Title: Conic sections
1Conic sections
V
m
r
?
M
2- µ Keplers constant GM (m3 s-2)
- h angular momentum constant
- E total energy constant
- e eccentricity
3Semi major axis a
semi minor axis b
ra
rp
4Solution
1
5- Location of perigee (closest approach) can be
found from 1 by setting ? to zero
6- Location of apogee (furthest departure) can be
found from 1by setting ? to p (note that ra only
has real values for e lt 1, circles and ellipses)
7- Combining perigee and apogee give a useful means
of finding eccentricity
8Semi major axis, a
9Semi minor axis, b
10family of solutions
- The value of eccentricity determines the category
of orbit obtained - e 1gives captive orbits
- e 1creates escape trajectories
e gt 0 lt1 elliptical
e 0 circular
e gt 1 hyperbola
e 1 parabola
11Example 1 circular Earth orbit
- e 0, r 6500 km and 40,000 km
12example 2 Connect with elliptical transfer orbit
13(No Transcript)
14(No Transcript)
15(No Transcript)
16Fuel requirement for manouver
- For LH2/LOX rocket with c 4500m/s
17- This was an example of a Hohmann transfer
- It was believed to have the minimum energy
requirement for moving between co-planar circular
orbits, as no fuel is wasted on velocity vector
rotation - Disproved by US student who postulated the
gravity assist manoeuvre for an assignment
18Example 3 hyperbolic capture into circular orbit
- Arrival at mars with a relative approach velocity
(V8) of 3km/sec, with capture into a circular
orbit at an altitude of 4000km - Find ?v required
19V8
?v
V2
Vcirc
20Adjust hyperbolic approach so that its perigee is
at the altitude of the required circular orbit.
The required velocity change will then be along
the line of flight and at maximum velocity,
giving the greatest change in E for a given ?v
21(No Transcript)
22(No Transcript)
23- Combinations of these manoeuvres enable all
bodies in the plane of the ecliptic to be
visited. - Some moons rotate out of plane, and require 3D
calculations of a more complex nature
24Example 4 transfer of a satellite left in LEO
inclined at 30 degrees to the equator to GEO
- This requires the same operations as in example
2, plus an orbital plane change of 30 - the plane change is best done at a point where
the orbit crosses the equator, where a simple
velocity rotation will suffice - It may be done at LEO, before or after perigee
burn - or GEO, before or after apogee kick burn
- or it may be combined with either of the 2 burns
- Choose whichever gives the smallest ?v
25LEO options
10130
7834 m/s
26GEO options
3158
Minimum ?v
1650
27(No Transcript)
28Fuel requirement for manouver
- For LH2/LOX rocket with c 4500m/s