|
|
double3 | axis |
| |
|
double | j2 = 1.0 |
| |
|
double | radius = 10.0 |
| |
|
| static int | status |
| | Apply the addition force change due to oblate gravity modeled by a J2 dipole term.
|
| |
◆ AddToGE()
◆ status
| int GravityEngine2.GravityJ2.status |
|
static |
Apply the addition force change due to oblate gravity modeled by a J2 dipole term.
The equation for the perturbing force is taken from Gravity (Poisson) (3.90) p166
This routine is called for each massive (i,j) pair. Those that have a "from body" with a non-zero J2 will apply the non-spherical perturbing force to the other.
There really should be an equal and opposite force on the source of the J2 force but since this is most often used for a planet force on a satellite, this is neglected since it's so small.
- Parameters
-
| fromIndex | |
| toIndex | |
| rsq | |
| rvmu_from | |
| rvmu_to | |
| parmFrom | |
| t | |
| afrom_out | |
| a | |
The documentation for this class was generated from the following file:
- ge2/GE2/Assets/GravityEngine2/Runtime/Core/ExternalAcceleration/GravityJ2.cs