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author | Joe Hunkeler <jhunkeler@gmail.com> | 2015-08-11 16:51:37 -0400 |
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committer | Joe Hunkeler <jhunkeler@gmail.com> | 2015-08-11 16:51:37 -0400 |
commit | 40e5a5811c6ffce9b0974e93cdd927cbcf60c157 (patch) | |
tree | 4464880c571602d54f6ae114729bf62a89518057 /math/slalib/doc/m2av.hlp | |
download | iraf-osx-40e5a5811c6ffce9b0974e93cdd927cbcf60c157.tar.gz |
Repatch (from linux) of OSX IRAF
Diffstat (limited to 'math/slalib/doc/m2av.hlp')
-rw-r--r-- | math/slalib/doc/m2av.hlp | 38 |
1 files changed, 38 insertions, 0 deletions
diff --git a/math/slalib/doc/m2av.hlp b/math/slalib/doc/m2av.hlp new file mode 100644 index 00000000..51d04343 --- /dev/null +++ b/math/slalib/doc/m2av.hlp @@ -0,0 +1,38 @@ +.help m2av Jun99 "Slalib Package" +.nf + + SUBROUTINE slM2AV (RMAT, AXVEC) + + - - - - - + M 2 A V + - - - - - + + From a rotation matrix, determine the corresponding axial vector + (single precision) + + A rotation matrix describes a rotation about some arbitrary axis. + The axis is called the Euler axis, and the angle through which the + reference frame rotates is called the Euler angle. The axial + vector returned by this routine has the same direction as the + Euler axis, and its magnitude is the Euler angle in radians. (The + magnitude and direction can be separated by means of the routine + slVN.) + + Given: + RMAT r(3,3) rotation matrix + + Returned: + AXVEC r(3) axial vector (radians) + + The reference frame rotates clockwise as seen looking along + the axial vector from the origin. + + If RMAT is null, so is the result. + + P.T.Wallace Starlink 11 April 1990 + + Copyright (C) 1995 Rutherford Appleton Laboratory + Copyright (C) 1995 Association of Universities for Research in Astronomy Inc. + +.fi +.endhelp |