In celestial mechanics, the Stumpff functions
ck(x) ,
ck(x)~\equiv~
1 | |
k! |
-
x | |
~\left(k+2\right)! |
+
x2 | |
~\left(k+4\right)! |
- … ~=~
| ||||
\sum | ||||
n=0 |
~~
~~k=0,1,2,3, \ldots~~.
x~.
Stumpf functions are useful for working with surface launch trajectories, and boosts from closed orbits to escape trajectories, since formulas for spacecraft trajectories using them smoothly meld from conventional closed orbits (circles and ellipses, eccentricity to open orbits (parabolas and hyperbolas, with no singularities and no imaginary numbers arising in the expressions as the launch vehicle gains speed to escape velocity and beyond. (The same advantage occurs in reverse, as a spacecraft decelerates from an arrival trajectory to go into a closed orbit around its destination, or descends to a planet's surface from a stable orbit.)
By comparing the Taylor series expansion of the trigonometric functions sin and cos with
c0(x)
c0(x) ,
~x>0 :
\begin{align} c0(x)~&=~~\cos\sqrt{x } ,\\[1ex] c1(x)~&=~
\sin\sqrt{x | |
}{ |
\sqrt{x }}~. \end{align}
Similarly, by comparing with the expansion of the hyperbolic functions sinh and cosh we find for
~x<0 :
\begin{align} c0(x)~&=~~\cosh\sqrt{-x } ,\\[1ex] c1(x)~&=~
\sinh\sqrt{-x | |
}{ |
\sqrt{-x }}~.\end{align}
Circular orbits and elliptical orbits use sine and cosine relations, and hyperbolic orbits use the sinh and cosh relations. Parabolic orbits (marginal escape orbits) formulas are a special in-between case.
For higher-order Stumpff functions needed for both ordinary trajectories and for perturbation theory, one can use the recurrence relation:
x ck+2(x)=
1 | |
k! |
-ck(x)~
~k=0,1,2, \ldots ~,
or when
x\ne0
ck+2(x)~=~
1 | \left( | |
x |
1 | |
k! |
-ck(x) \right)~
~k=0,1,2, \ldots~~.
Using this recursion, the two further Stumpf functions needed for the universal variable formulation are, for
~x>0 :
\begin{align} c2(x)~&=~~~
1-\cos\sqrt{x | |
}{ |
\sqrt{x }} ,\\ \\ c3(x)~&=~
\sqrt{x | |
- |
\sin\sqrt{x } }{x} ; \end{align}
and for
~x<0 :
\begin{align} c2(x)~&=~
1-\cosh\sqrt{-x | |
}{ |
\sqrt{-x }} ,\\ \\ c3(x)~&=~
\sqrt{-x | |
- \sinh |
\sqrt{-x } }{-x}~~. \end{align}
The Stumpff functions can be expressed in terms of the Mittag-Leffler function:
ck(x)~=~E2,k+1(-x)~~.