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<title>DIO, The International Journal of Scientific History</title>
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  <hr /><h2>&ddagger;<a name="tth_sEc4">
4</a>&nbsp;&nbsp;The instruments used by Hipparchos</h2><a name="sec-4">
</a><a name="4">
</a>


<center>
 by KEITH A.PICKERING
</center>

<p /><div class="p"><!----></div>
     <h3><a name="tth_sEc4.1">
A</a>&nbsp;&nbsp;A revealing gap</h3><a name="sec-4A">
</a><a name="4A">
</a>

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.1.1">
A1</a>&nbsp;&nbsp;</h4>More than 2000 years after its compilation, it is now possible to 
determine with some confidence the kinds of instruments that were used 
to observe the stars of the Ancient Star Catalog, and in which parts of 
the sky the various instruments were employed. The fact that there were 
multiple instruments, and that the ASC was not, 
as stated by Ptolemy, observed with a single ecliptical astrolabe, does 
more than provide yet-another proof that the catalog was observed by 
Hipparchos (for we have more than enough of those already); it also 
allows us a glimpse into the hitherto unknown workings of astronomy and 
instrument manufacture as they were practiced at a critical point of 
ancient Greek science.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.1.2">
A2</a>&nbsp;&nbsp;</h4>The <i>Almagest</i> divides the ASC into three sections, for the northern, 
zodiacal, and southern parts of the sky. Looking at the northern sky, 
figure 1 plots the absolute errors in longitude for each northern star 
in the ASC, according to its actual longitude at the epoch of the 
catalog (which we will take to be -128.0). In looking at 
the plot, note particularly that there is an odd gap in the plotted 
stars at about 70
&deg; ecliptic longitude. Note also that there is a 
similar gap at about 250
&deg; ecliptic longitude, exactly 180
&deg; 
away.  This 
gap can be more easily seen if we overlay the second half of the 
longitudes (180-360) on top of the first half, as we have done in 
figure 2. Note particularly that the longitude errors increase in 
absolute magnitude as we get close to the gap. For purposes of 
comparison, figure 3 plots the absolute errors in right ascension by 
right ascension: the gap disappears.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.1.3">
A3</a>&nbsp;&nbsp;</h4>This gap is significant because it shows us, first, that the northern 
sky was observed primarily with a single instrument; second, that the 
instrument was an ecliptic astrolabe; and third, that the astrolabe was 
of a somewhat different design from the description given by Ptolemy, 
and indeed different from any previously known to have existed.

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
<a name="tth_fIg1">
</a> <img src="inst1.png" alt="inst1.png" />

<p /><div class="p"><!----></div>
<center>Figure 1: <a name="fg5">
</a> Errors in longitude by longitude, for northern 
stars in the ASC. Note vertical gaps in the data.</center>

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
<a name="tth_fIg2">
</a> <img src="inst2.png" alt="inst2.png" />

<p /><div class="p"><!----></div>
<center>Figure 2: <a name="fg6">
</a> Errors in longitude by longitude, with longitudes overlain.
Note vertical gap in the data.</center>

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
<a name="tth_fIg3">
</a> 
<p /><div class="p"><!----></div>
<img src="inst3.png" alt="inst3.png" />

<p /><div class="p"><!----></div>
<center>Figure 3: <a name="fg7">
</a> Errors in right ascension by right ascension, for northern stars in the ASC.
Note lack of vertical gaps in the data.</center>

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
     <h3><a name="tth_sEc4.2">
B</a>&nbsp;&nbsp;The astrolabe</h3><a name="sec-4B">
</a><a name="4B">
</a>

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.1">
B1</a>&nbsp;&nbsp;</h4>The armillary astrolabe used in ancient Greek astronomy is, at first 
glance, a bewildering maze of nested rings, fitted closely inside each 
other, that rotate in complex ways. Let's look at the way an armillary 
astrolabe is contructed, from the inside out. The innermost ring (Ring 
1) contains a pair of sighting holes or pinnules, diametrically 
opposite each other, through which the star is sighted. Immediately 
surrounding Ring&nbsp;1 is Ring&nbsp;2, whose inside diameter is fractionally 
larger than the outside diameter of Ring&nbsp;1. Ring&nbsp;1 is constrained so 
that it rotates inside Ring&nbsp;2, in the same plane, their edges just 
touching. Ring&nbsp;2 has a scale of degrees on its edge, indicating the 
rotational position of the pinnules on Ring&nbsp;1. (See figure 4.) If we 
wished, we could mount Ring&nbsp;2 on the meridian, and then use the Ring 
1&amp;2 assembly as a transit instrument. To do this, we would have to 
orient Ring&nbsp;2 so that it points north-south, and so that its 
zero-degree points on the scale were horizontal, and 90-degree points were 
vertical.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.2">
B2</a>&nbsp;&nbsp;</h4>But to make the Ring&nbsp;1&amp;2 assembly more useful, we will mount it 
differently. We construct an outer ring, Ring&nbsp;3, set vertically 
so that the whole Ring&nbsp;1&amp;2 assembly can pivot within it, around a 
vertical axis. We run axle pins from the 90-degree poles of Ring 
2 into the inner edge of Ring&nbsp;3; so now Ring&nbsp;1&amp;2 can rotate to any 
azimuth. To determine the azimuth at which Ring&nbsp;1&amp;2 is pointing, we 
add Ring&nbsp;4, which is fixed horizontally and at right angles to Ring&nbsp;3. 
Ring&nbsp;4 carries another scale of degrees, indicating the rotational 
position of Ring&nbsp;2. Rings 3&amp;4 now form a cage, within which Ring&nbsp;2 
rotates freely in azimuth, while Ring&nbsp;1 rotates freely in altitude 
within Ring&nbsp;2. (See figure&nbsp;<a href="#fg8">4</a>). The instrument can now be used as a 
theodolite, since we can determine the altitude and azimuth of any 
star with it. We will call this arrangement the 4-ring instrument.

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
<a name="tth_fIg4">
</a> <img src="astrol1.png" alt="astrol1.png" />

<p /><div class="p"><!----></div>
<center>Figure 4: <a name="fg8">
</a> The four-ring instrument. Ring&nbsp;1 (innermost white) carries 
pinnules through which the star is sighted. Ring&nbsp;2 (dark gray) has a scale of 
degrees. Ring&nbsp;3 (outer white) holds the polar axis. Ring&nbsp;4 (light gray) contains
the second scale of degrees. When Ring&nbsp;4 is horizontal, the instrument can be
used as a theodolite; when mounted to rotate with the sky, it is an astrolabe.
</center>

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.3">
B3</a>&nbsp;&nbsp;</h4>The 4-ring instrument is capable of pointing to almost any point in 
the celestial sphere, making it quite useful. In fact, there is only one 
fly in the ointment to this whole arrangement: at certain rotational 
positions, Ring&nbsp;2 becomes so closely aligned with Ring&nbsp;3 that a star 
cannot be seen through the pinnules, because Ring&nbsp;3 gets in the way. 
There are two such rotational positions, exactly 180
&deg; apart. For the 
same reason, it is impossible to observe very near to the horizon, 
because Ring&nbsp;4 gets in the 
way.<a href="#tthFtNtAAB" name="tthFrefAAB">
<math xmlns="http://www.w3.org/1998/Math/MathML">
<mrow><msup><mi></mi><mrow><mn>1</mn></mrow></msup>
</mrow></math></a>

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.4">
B4</a>&nbsp;&nbsp;</h4>A larger issue with the 4-ring instrument is one of orientation. With 
Ring&nbsp;4 oriented horizontally, it makes a fine theodolite, but 
horizon-based coordinates are of limited utility in astronomy, because the sky 
moves as the earth rotates. It is much better to mount 
the 4-ring instrument so that it rotates too, following the sky. 

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.5">
B5</a>&nbsp;&nbsp;</h4>Recall that the purpose of Ring&nbsp;3 is entirely structural: it holds the 
axis around which Rings 1&amp;2 rotate. So the most obvious 
arrangement is to simply extend that axis, and orient the axis toward 
the celestial pole. Then the entire 4-ring instrument could be rotated 
along with the sky. The astrolabe, if mounted this way, would read 
equatorial coordinates directly, because Ring&nbsp;4 would be permanently 
aligned with the celestial equator. All that would be needed would be 
a way to align the instrument in right ascension.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.6">
B6</a>&nbsp;&nbsp;</h4>Although equatorial coordinates are used extensively today, in ancient 
times ecliptical coordinates were more widely used. So in practice, 
what was really needed was a way to mount the 4-ring instrument so 
that: (a) it could rotate with the sky; and (b) Ring&nbsp;4 would be 
aligned with the ecliptic instead of the celestial equator. And in the 
<i>Almagest</i> V.1, Ptolemy describes how this was done: a second axis was 
drilled in Ring&nbsp;3 (this would have been 23
<math xmlns="http://www.w3.org/1998/Math/MathML">
<mrow><msup><mi></mi><mrow><mo>&SmallCircle;</mo></mrow></msup>
<mn>51</mn><mo>'</mo></mrow></math> from the first). 
Then the 4-ring instrument was mounted so that the second axis was pointed 
to the celestial pole. The entire instrument could then rotate (around the 
polar axis) to follow the sky; while the coordinate readings from Ring&nbsp;2 and 
Ring&nbsp;4 are stuck in a different coordinate frame, tilted in exactly the 
same manner as the ecliptic is tilted to the equator. And there we 
have it: the ecliptic armillary astrobale, nearly the same as 
described by Ptolemy in the <i>Almagest</i>.<a href="#tthFtNtAAC" name="tthFrefAAC">
<math xmlns="http://www.w3.org/1998/Math/MathML">
<mrow><msup><mi></mi><mrow><mn>2</mn></mrow></msup>
</mrow></math></a>

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.7">
B7</a>&nbsp;&nbsp;</h4>Except for one big thing. When we drilled the polar axis in Ring&nbsp;3, at 
that moment we permanently fixed the ecliptic longitude of Ring&nbsp;3 
along the 90
&deg;-270
&deg; solstitial colure. This 
is the great circle in the 
sky through which both the ecliptic poles and celestial poles run, and 
now this colure must also run through Ring&nbsp;3 too, since both 
instrumental axes run through Ring&nbsp;3. Now we know that Ring&nbsp;3 will get 
in the way of some observations, so if we build an astrolabe this way - as 
described by Ptolemy - we should expect there to be a gap in observed 
stars at 90
&deg; and 270
&deg; ecliptic longitude. As we have 
seen, there is a longitudinal gap, but it is not at 90-270; it is at 
70-250. This means that the astrolabe which Hipparchos actually used 
to observe the ASC was built in a somewhat different manner than the 
one described by Ptolemy in the <i>Almagest</i>.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.8">
B8</a>&nbsp;&nbsp;</h4>Instead of drilling a second set of axis holes in Ring&nbsp;3, Hipparchos 
(or his instrument maker) must have used separate bearing journals  to 
hold the polar axis. There would be two such journals clamped or affixed 
to opposite sides of Ring&nbsp;3 at the celestial poles (see fig.&nbsp;<a href="#fg9">5</a>). 
Since the solstitial colure (which defines 90-270 ecliptic longitude) must 
contain both axes, the colure no longer contains Ring&nbsp;3; rather, it is 
offset by some amount. In the instrument actually used by Hipparchos, 
this amount was about 20 degrees. This arrangement has a structural advantage, 
because it avoids putting 
another set of holes in Ring&nbsp;3, which has already been weakened by the 
holes for the ecliptic axis.

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
<a name="tth_fIg5">
</a> 
<table align="center" border="0"><tr><td>
<img src="astrol2.png" alt="astrol2.png" /></td></tr></table><!--hboxt-->

<p /><div class="p"><!----></div>
<center>Figure 5: <a name="fg9">
</a> The four-ring instrument viewed from above the poles.
Ring&nbsp;2 (dark gray) pivots around the North Ecliptic Pole (NEP), while the entire 
4-ring instrument rotates around the North Celestial Pole (NCP) to follow the sky.
(The NCP axis is affixed to an outer Ring&nbsp;6, which is not shown in the diagram.)
According to the <i>Almagest</i>, the NCP axis is drilled in Ring&nbsp;3 (top); in the 
astrolabe used by Hipparchos, the NCP axis is carried on a separate bearing 
journal (bottom). The 90-270 solsticial colure is the great circle joining the 
two axes - along Ring&nbsp;3 (top) or offset from it (bottom).</center>

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.9">
B9</a>&nbsp;&nbsp;</h4>If he had used more than one astrolabe for observing the Northern sky, 
Hipparchos could have arranged to have the journals on astrolabe&nbsp;#2 
mounted on the opposite sides of Ring&nbsp;3 than the arrangement on 
astrolabe&nbsp;#1; so the blind spot of astrolabe&nbsp;#2 would be at 110-290, 
and the blind spot of one instrument could be covered by the other. 
Therefore it is apparent that large parts of the northern sky were 
observed with a single instrument - or nearly so.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.10">
B10</a>&nbsp;&nbsp;</h4>You recall that there is another blind spot, along Ring&nbsp;4. This ring 
falls right on the ecliptic, so we might expect to see a gap in the 
data here, too, just as we found in the longitudes. In the northern 
sky, only one constellation (Ophiuchus) dips all the way down to the 
ecliptic; but there is no such gap along the ecliptic in Ophiuchus. In 
fact, there is no such gap among the stars of the zodiacal 
constellations, either.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.11">
B11</a>&nbsp;&nbsp;</h4>So there must have been a different instrument or a different 
technique (or both) for observing right at the ecliptic. One 
possibility is a second set of 
pinnules.<a href="#tthFtNtAAD" name="tthFrefAAD">
<math xmlns="http://www.w3.org/1998/Math/MathML">
<mrow><msup><mi></mi><mrow><mn>3</mn></mrow></msup>
</mrow></math></a>
The primary pinnules would be mounted on Ring&nbsp;1 at diametrically 
opposite positions, as already described; while the second set would 
be mounted above these, a little more than one ring-width away. Thus, 
the sightline through the first set would be exactly parallel to the 
sightline through the second set. When the first set was too close to 
the ecliptic to observe, the second set would still be able to see 
over the top of Ring&nbsp;4.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.2.12">
B12</a>&nbsp;&nbsp;</h4>I have been unable to find similar gaps in either the Zodiac or the South 
sections of the ASC. This implies that the instrument used in the North 
was different than the one(s) used in other parts of the sky.

<p /><div class="p"><!----></div>
     <h3><a name="tth_sEc4.3">
C</a>&nbsp;&nbsp;Gap Characteristics</h3><a name="sec-4C">
</a><a name="4C">
</a>

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.3.1">
C1</a>&nbsp;&nbsp;</h4>Are there bright stars in the gap that Hipparchos usually would have taken,
or is the reason for the lack of cataloged stars simply that there are no
bright stars in this region of the sky? In other words, is the gap real?
As it turns out, there are only five stars in the Northern sky brighter 
than magnitude 3.9 that Hipparchos left out of the catalog: 
&chi; UMa, 

&alpha; Lac, 46 LMi, 109 Her, and 
&alpha; Sct. Two of these five (109 
Her and 
&alpha; Sct) are in the gap. Since the gap represents only about 
5% of the sky, this is clearly a significant number.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.3.2">
C2</a>&nbsp;&nbsp;</h4>The gap is caused by the physical presence of Ring&nbsp;3, which has a constant
physical width. But the longitudinal width of Ring&nbsp;3 increases toward the ecliptic
pole, because the lines of longitude converge there. We can determine
the relative thickness of Ring&nbsp;3 by close examination of the edges of the gap.
In figure <a href="#gap2">6</a>, I have plotted the region near the gap in latitude and
"folded" longitude, along with lines indicating the position that the gap 
would have if Ring&nbsp;3 was centered at 69.5 - 249.5 and had a width of 3.7 degrees.
These parameters fit the actual gap quite well (although smaller widths cannot
be excluded).

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
<a name="tth_fIg6">
</a> 
<p /><div class="p"><!----></div>
<img src="gap2.png" alt="gap2.png" />

<p /><div class="p"><!----></div>
<center>Figure 6: <a name="gap2">
</a> Close view of the gap in cataloged stars. The lines show the 
limits of a gap 3.7 degrees wide centered at 69.5 - 249.5 degrees longitude.</center>

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
<a name="tth_fIg7">
</a> 
<p /><div class="p"><!----></div>
<img src="gap3.png" alt="gap3.png" />

<p /><div class="p"><!----></div>
<center>Figure 7: <a name="gap3">
</a> Stars brighter than magnitude 4.5 missing from the northern
part of the ASC. Note that none are missing above latitude 75, possibly indicating
that a different kind of instrument was used in this small region of the sky.</center>

<p /><div class="p"><!----></div>

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.3.3">
C3</a>&nbsp;&nbsp;</h4>Similarly, in figure <a href="#gap3">7</a>, I have plotted all stars of magnitude 4.5 or
brighter that are missing from the catalog, with the same gap limits. Note particularly
that there are no missing stars this bright above latitude 75. This is a
good indication of the polar limits of the astrolabe, and shows the region in
which a different instrument was probably used. This also explains why there are 
a couple of holdout stars present in the gap: the holdouts are both at very high latitudes.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.3.4">
C4</a>&nbsp;&nbsp;</h4>The edges of the gap are between 4 and 5 degrees apart at the ecliptic. The exact edges 
depend on how far north one chooses to assume was observed with this single instrument. 
The gap is actually two adjacent gaps: one in which the lower pinnule is blocked by Ring&nbsp;3, 
and one in which the upper pinnule is blocked. Therefore, the 5-degree width of the gap 
implies that the physical width of Ring&nbsp;3 was between 2 and 2
&deg;.5 degrees. The 
exact center of the gap is a bit tricky to pin down, but it seems to be very close to 
69
&deg;.5 of ecliptic longitude.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.3.5">
C5</a>&nbsp;&nbsp;</h4>Further, between these two adjacent gaps, at the very center, there is
a very narrow "gap within the gap," where a star lying at that precise longitude 
should be visible. This is because, when Ring&nbsp;2 is <i>exactly</i> aligned with 
Ring&nbsp;3, neither pinnule on Ring&nbsp;1 is blocked by Ring&nbsp;3: the line of sight passes 
along the edge of Ring&nbsp;3 just as if it were a wide extension of Ring&nbsp;2. As it 
turns out, there is in fact a cataloged star lying almost exactly at the center 
of the gap: 
&epsi; UMi. But since it also lies at a very high latitude, there 
is no guarantee that it was observed through the "gap within the gap," rather than 
in the same manner as other stars near the ecliptic pole.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.3.6">
C6</a>&nbsp;&nbsp;</h4>A ring about 2 degrees wide is rather narrow, structurally speaking, which in turn 
places limits on the material used to construct the astrolabe. For example, if 
Ring&nbsp;3 was 50 cm in diameter, it could be no more than about 1 cm (perhaps less) 
in width. I tend to doubt that a wooden instrument of this narrow aspect ratio could 
be stiff enough against the weight it must support to be very accurate; bronze seems 
a more likely material.

<p /><div class="p"><!----></div>
     <h3><a name="tth_sEc4.4">
D</a>&nbsp;&nbsp;Epoch of the Northern Catalog</h3><a name="sec-4D">
</a><a name="4D">
</a>

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.4.1">
D1</a>&nbsp;&nbsp;</h4>The single-instrument hypothesis implies that the northern sky 
was observed all at once, before the instrument had time to become 
worn or damaged; in other words, a matter of months or a few years, 
rather than decades. Careful analysis will allow us to determine the 
epoch of this northern observational effort.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.4.2">
D2</a>&nbsp;&nbsp;</h4>After subtracting Ptolemy's 2
<math xmlns="http://www.w3.org/1998/Math/MathML">
<mrow><msup><mi></mi><mrow><mo>&SmallCircle;</mo></mrow></msup>
<mi>&nbsp;</mi><msup><mi></mi><mrow><mn>2</mn></mrow></msup>

<msub><mo>/</mo><mrow><mn>3</mn></mrow>
</msub>
</mrow></math> false precessional constant, we 
can reconstruct the actual longitudes of these stars as observed by 
Hipparchos. Due to precession, stars advance from west to east 
parallel to the ecliptic, maintaining their same ecliptic latitudes, 
but increasing their ecliptic longitudes at a rate of about 83' per 
century. So, as a first cut, we can simply take these reconstructed 
Hipparchan longitudes and assume that they were (on average) correct 
as measured, then find the epoch at which such an assumption would be 
true. For the northern stars, this works out to -157,&nbsp;
&PlusMinus;59 years.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.4.3">
D3</a>&nbsp;&nbsp;</h4>There is a problem with this procedure, however, because the longitudes 
observed by Hipparchos were not actually correct, on average. There is a 
systematic error which we must account for. The longitude of the stars
is determined ultimately by reference to the Sun. The Sun is observed just
before sunset, on a day just after new Moon. The longitude of the Sun is
known from theory, and the difference between the Sun and Moon gives the
Moon's longitude; then, after sunset of the same day, the difference
between the Moon and a fundamental star is observed, to give the 
longitude of the fundamental star; and finally, the longitudes of
individual stars are observed by their difference from the fundamental 
star. But each of these steps requires the astrolabe to be briefly 
clamped in position while the measurements are being made; and these
successive clampings tend to push the longitudes lower than true, 
because the earth rotates during these brief intervals. In other words,
there is a systematic error in rotation of the astrolabe around the 
equatorial axis.

<p /><div class="p"><!----></div>
      <h4><a name="tth_sEc4.4.4">
D4</a>&nbsp;&nbsp;</h4>Rawlins 1982 has shown that misrotation of the astrolabe with respect 
to the real sky will make itself known by the presence of a cosine 
error wave in the observed latitudes. Further, the amplitude of this 
cosine error wave is proportional to the amount of astrolabe 
misrotation. And in fact there is just such an error in the latitudes 
of the northern stars. This error wave has an amplitude of 
10.6&nbsp;
&PlusMinus;1.8 arcmin, implying that 
the astrolabe was systematically misrotated by 24.2&nbsp;
&PlusMinus;4.2 arcmin. It takes 
precession 29.2 years to move a star that far in longitude, meaning 
that the actual epoch of observation for the northern stars was 
-128&nbsp;
&PlusMinus;59 years. This is very nearly the epoch implied by Ptolemy's
precessional constant.

<p /><div class="p"><!----></div>
<br /><br /> <b>References.</b><br />

<p /><div class="p"><!----></div>
 Rawlins, Dennis (1982).  An Examination of the Ancient Star 
Catalog. <i>PASP</i> 94, 359.<br />
Toomer, G.J. (1998).  <i>Ptolemy's Almagest</i>.  Princeton University Press.<br />

<p /><div class="p"><!----></div>
<hr /><h3>Footnotes:</h3>

<p /><div class="p"><!----></div>
<a name="tthFtNtAAB"></a><a href="#tthFrefAAB">
<math xmlns="http://www.w3.org/1998/Math/MathML">
<mrow><msup><mi></mi><mrow><mn>1</mn></mrow></msup>
</mrow></math></a>  Areas near the axis are also blocked by both Ring&nbsp;3 and Ring&nbsp;2.
<p /><div class="p"><!----></div>
<a name="tthFtNtAAC"></a><a href="#tthFrefAAC">
<math xmlns="http://www.w3.org/1998/Math/MathML">
<mrow><msup><mi></mi><mrow><mn>2</mn></mrow></msup>
</mrow></math></a>  For purposes of simplicity, we have left out Ring 5, which is used 
only as an aid to orientation. Ring 6, which is fixed to the earth 
as a strutctural support for the whole instrument, holds the second
axis, which points toward the North Celestial Pole.
<p /><div class="p"><!----></div>
<a name="tthFtNtAAD"></a><a href="#tthFrefAAD">
<math xmlns="http://www.w3.org/1998/Math/MathML">
<mrow><msup><mi></mi><mrow><mn>3</mn></mrow></msup>
</mrow></math></a>  Ptolemy does not mention a second set of pinnules in the <i>
Almagest</i>, but given the foregoing, he cannot be taken as a wholly 
reliable source on the construction of astrolabes.
<br /><br /><hr /><small>File translated from
T<sub>E</sub>X
by <a href="http://hutchinson.belmont.ma.us/tth/">
T<sub>T</sub>M</a>,
version 3.33.<br />On 19 Apr 2003, 12:12.</small>
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