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+<!--Converted with LaTeX2HTML 97.1 (release) (July 13th, 1997)
+ by Nikos Drakos (nikos@cbl.leeds.ac.uk), CBLU, University of Leeds
+* revised and updated by: Marcus Hennecke, Ross Moore, Herb Swan
+* with significant contributions from:
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+<TITLE>SLA_AOPQK - Quick Appt-to-Observed</TITLE>
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+<H2><A NAME="SECTION000410000000000000000">SLA_AOPQK - Quick Appt-to-Observed</A>
+<A NAME="xref_SLA_AOPQK">&#160;</A><A NAME="SLA_AOPQK">&#160;</A>
+</H2>
+ <DL>
+<DT><STRONG>ACTION:</STRONG>
+<DD>Quick apparent to observed place (but see Note&nbsp;8, below).
+<DT><STRONG>CALL:</STRONG>
+<DD><TT>CALL sla_AOPQK (RAP, DAP, AOPRMS, AOB, ZOB, HOB, DOB, ROB)</TT>
+<P> </DL>
+<P> <DL>
+<DT><STRONG>GIVEN:</STRONG>
+<DD>
+<BR>
+<TABLE CELLPADDING=3>
+<TR VALIGN="TOP"><TD ALIGN="LEFT"><EM>RAP,DAP</EM></TD>
+<TH ALIGN="LEFT"><B>D</B></TH>
+<TD ALIGN="LEFT" NOWRAP>geocentric apparent <IMG WIDTH="42" HEIGHT="29" ALIGN="MIDDLE" BORDER="0"
+ SRC="img3.gif"
+ ALT="$[\,\alpha,\delta\,]$"> (radians)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="LEFT"><EM>AOPRMS</EM></TD>
+<TD ALIGN="LEFT"><B>D(14)</B></TD>
+<TD ALIGN="LEFT" NOWRAP>star-independent apparent-to-observed parameters:</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(1)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>geodetic latitude (radians)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(2,3)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>sine and cosine of geodetic latitude</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(4)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>magnitude of diurnal aberration vector</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(5)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>height (metres)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(6)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>ambient temperature (degrees K)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(7)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>pressure (mB)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(8)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>relative humidity (0-1)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(9)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>wavelength (<IMG WIDTH="26" HEIGHT="25" ALIGN="MIDDLE" BORDER="0"
+ SRC="img21.gif"
+ ALT="$\mu{\rm m}$">)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(10)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>lapse rate (degrees K per metre)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(11,12)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>refraction constants A and B (radians)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(13)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>longitude + eqn of equinoxes +
+``sidereal <IMG WIDTH="16" HEIGHT="13" ALIGN="BOTTOM" BORDER="0"
+ SRC="img19.gif"
+ ALT="$\Delta$">UT'' (radians)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="CENTER" NOWRAP COLSPAN=1>(14)</TD>
+<TD></TD>
+<TD ALIGN="LEFT" NOWRAP>local apparent sidereal time (radians)</TD>
+</TR>
+</TABLE></DL>
+<P> <DL>
+<DT><STRONG>RETURNED:</STRONG>
+<DD>
+<BR>
+<TABLE CELLPADDING=3>
+<TR VALIGN="TOP"><TD ALIGN="LEFT"><EM>AOB</EM></TD>
+<TH ALIGN="LEFT"><B>D</B></TH>
+<TD ALIGN="LEFT" NOWRAP>observed azimuth (radians: N=0, E=<IMG WIDTH="26" HEIGHT="14" ALIGN="BOTTOM" BORDER="0"
+ SRC="img22.gif"
+ ALT="$90^{\circ}$">)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="LEFT"><EM>ZOB</EM></TD>
+<TD ALIGN="LEFT"><B>D</B></TD>
+<TD ALIGN="LEFT" NOWRAP>observed zenith distance (radians)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="LEFT"><EM>HOB</EM></TD>
+<TD ALIGN="LEFT"><B>D</B></TD>
+<TD ALIGN="LEFT" NOWRAP>observed Hour Angle (radians)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="LEFT"><EM>DOB</EM></TD>
+<TD ALIGN="LEFT"><B>D</B></TD>
+<TD ALIGN="LEFT" NOWRAP>observed Declination (radians)</TD>
+</TR>
+<TR VALIGN="TOP"><TD ALIGN="LEFT"><EM>ROB</EM></TD>
+<TD ALIGN="LEFT"><B>D</B></TD>
+<TD ALIGN="LEFT" NOWRAP>observed Right Ascension (radians)</TD>
+</TR>
+</TABLE></DL>
+<P> <DL>
+<DT><STRONG>NOTES:</STRONG>
+<DD><DL COMPACT>
+<DT>1.
+<DD>This routine returns zenith distance rather than elevation
+in order to reflect the fact that no allowance is made for
+depression of the horizon.
+ <DT>2.
+<DD>The accuracy of the result is limited by the corrections for
+ refraction. Providing the meteorological parameters are
+ known accurately and there are no gross local effects, the
+ predicted azimuth and elevation should be within about
+<P> <IMG WIDTH="23" HEIGHT="18" ALIGN="BOTTOM" BORDER="0"
+ SRC="img25.gif"
+ ALT="$0\hspace{-0.05em}^{'\hspace{-0.1em}'}\hspace{-0.4em}.1$"> for <IMG WIDTH="56" HEIGHT="27" ALIGN="MIDDLE" BORDER="0"
+ SRC="img26.gif"
+ ALT="$\zeta<70^{\circ}$">. Even
+ at a topocentric zenith distance of
+ <IMG WIDTH="26" HEIGHT="14" ALIGN="BOTTOM" BORDER="0"
+ SRC="img22.gif"
+ ALT="$90^{\circ}$">, the accuracy in elevation should be better than
+ 1&nbsp;arcminute; useful results are available for a further
+ <IMG WIDTH="18" HEIGHT="14" ALIGN="BOTTOM" BORDER="0"
+ SRC="img27.gif"
+ ALT="$3^{\circ}$">, beyond which the sla_REFRO routine returns a
+ fixed value of the refraction. The complementary
+ routines sla_AOP (or sla_AOPQK) and sla_OAP (or sla_OAPQK)
+ are self-consistent to better than 1&nbsp;microarcsecond all over
+ the celestial sphere.
+ <DT>3.
+<DD>It is advisable to take great care with units, as even
+ unlikely values of the input parameters are accepted and
+ processed in accordance with the models used.
+ <DT>4.
+<DD><I>Apparent</I> <IMG WIDTH="42" HEIGHT="29" ALIGN="MIDDLE" BORDER="0"
+ SRC="img3.gif"
+ ALT="$[\,\alpha,\delta\,]$"> means the geocentric apparent right ascension
+ and declination, which is obtained from a catalogue mean place
+ by allowing for space motion, parallax, precession, nutation,
+ annual aberration, and the Sun's gravitational lens effect. For
+ star positions in the FK5 system (<I>i.e.</I> J2000), these effects can
+ be applied by means of the sla_MAP <I>etc.</I> routines. Starting from
+ other mean place systems, additional transformations will be
+ needed; for example, FK4 (<I>i.e.</I> B1950) mean places would first
+ have to be converted to FK5, which can be done with the
+ sla_FK425 <I>etc.</I> routines.
+ <DT>5.
+<DD><I>Observed</I> <IMG WIDTH="66" HEIGHT="29" ALIGN="MIDDLE" BORDER="0"
+ SRC="img28.gif"
+ ALT="$[\,Az,El~]$"> means the position that would be seen by a
+ perfect theodolite located at the observer. This is obtained
+ from the geocentric apparent <IMG WIDTH="42" HEIGHT="29" ALIGN="MIDDLE" BORDER="0"
+ SRC="img3.gif"
+ ALT="$[\,\alpha,\delta\,]$"> by allowing for Earth
+ orientation and diurnal aberration, rotating from equator
+ to horizon coordinates, and then adjusting for refraction.
+ The <IMG WIDTH="41" HEIGHT="29" ALIGN="MIDDLE" BORDER="0"
+ SRC="img29.gif"
+ ALT="$[\,h,\delta\,]$"> is obtained by rotating back into equatorial
+ coordinates, using the geodetic latitude corrected for polar
+ motion, and is the position that would be seen by a perfect
+ equatorial located at the observer and with its polar axis
+ aligned to the Earth's axis of rotation (<I>n.b.</I> not to the
+ refracted pole). Finally, the <IMG WIDTH="13" HEIGHT="14" ALIGN="BOTTOM" BORDER="0"
+ SRC="img24.gif"
+ ALT="$\alpha$"> is obtained by subtracting
+ the <I>h</I> from the local apparent ST.
+ <DT>6.
+<DD>To predict the required setting of a real telescope, the
+ observed place produced by this routine would have to be
+ adjusted for the tilt of the azimuth or polar axis of the
+ mounting (with appropriate corrections for mount flexures),
+ for non-perpendicularity between the mounting axes, for the
+ position of the rotator axis and the pointing axis relative
+ to it, for tube flexure, for gear and encoder errors, and
+ finally for encoder zero points. Some telescopes would, of
+ course, exhibit other properties which would need to be
+ accounted for at the appropriate point in the sequence.
+ <DT>7.
+<DD>The star-independent apparent-to-observed-place parameters
+ in AOPRMS may be computed by means of the sla_AOPPA routine.
+ If nothing has changed significantly except the time, the
+ sla_AOPPAT routine may be used to perform the requisite
+ partial recomputation of AOPRMS.
+ <DT>8.
+<DD>The ``sidereal <IMG WIDTH="16" HEIGHT="13" ALIGN="BOTTOM" BORDER="0"
+ SRC="img19.gif"
+ ALT="$\Delta$">UT'' which forms part of AOPRMS(13)
+ is UT1-UTC converted from solar to
+ sidereal seconds and expressed in radians.
+ <DT>9.
+<DD>At zenith distances beyond about <IMG WIDTH="26" HEIGHT="14" ALIGN="BOTTOM" BORDER="0"
+ SRC="img33.gif"
+ ALT="$76^\circ$">, the need for
+ special care with the corrections for refraction causes a
+ marked increase in execution time. Moreover, the effect
+ gets worse with increasing zenith distance. Adroit
+ programming in the calling application may allow the
+ problem to be reduced. Prepare an alternative AOPRMS array,
+ computed for zero air-pressure; this will disable the
+ refraction corrections and cause rapid execution. Using
+ this AOPRMS array, a preliminary call to the present routine
+ will, depending on the application, produce a rough position
+ which may be enough to establish whether the full, slow
+ calculation (using the real AOPRMS array) is worthwhile.
+ For example, there would be no need for the full calculation
+ if the preliminary call had already established that the
+ source was well below the elevation limits for a particular
+ telescope.
+ <DT>10.
+<DD>The azimuths <I>etc.</I> used by the present routine are with
+ respect to the celestial pole. Corrections to the terrestrial pole
+ can be computed using sla_POLMO.
+ </DL></DL>
+<BR> <HR>
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+<ADDRESS>
+<I>SLALIB --- Positional Astronomy Library<BR>Starlink User Note 67<BR>P. T. Wallace<BR>12 October 1999<BR>E-mail:ptw@star.rl.ac.uk</I>
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