Solving Kepler’s equation via Smale’s α-theory
We obtain an approximate solution E ~ = E ~ ( e , M ) of Kepler’s equation E - e sin ( E ) = M for any e ∈ [ 0 , 1 ) and M ∈ [ 0 , π ] . Our solution is guaranteed, via Smale’s α -theory, to converge to the actual solution E through Newton’s method at quadratic speed, i.e. the n -th iteration produc...
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Published in | Celestial mechanics and dynamical astronomy Vol. 119; no. 1; pp. 27 - 44 |
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Main Authors | , , |
Format | Journal Article |
Language | English |
Published |
Dordrecht
Springer Netherlands
01.05.2014
|
Subjects | |
Online Access | Get full text |
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Summary: | We obtain an approximate solution
E
~
=
E
~
(
e
,
M
)
of Kepler’s equation
E
-
e
sin
(
E
)
=
M
for any
e
∈
[
0
,
1
)
and
M
∈
[
0
,
π
]
. Our solution is guaranteed, via Smale’s
α
-theory, to converge to the actual solution
E
through Newton’s method at quadratic speed, i.e. the
n
-th iteration produces a value
E
n
such that
|
E
n
-
E
|
≤
(
1
2
)
2
n
-
1
|
E
~
-
E
|
. The formula provided for
E
~
is a piecewise rational function with conditions defined by polynomial inequalities, except for a small region near
e
=
1
and
M
=
0
, where a single cubic root is used. We also show that the root operation is unavoidable, by proving that no approximate solution can be computed in the entire region
[
0
,
1
)
×
[
0
,
π
]
if only rational functions are allowed in each branch. |
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Bibliography: | ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 0923-2958 1572-9478 |
DOI: | 10.1007/s10569-014-9545-8 |