Galilei, Galileo
,
The systems of the world
,
1661
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121 - 130
131 - 140
141 - 150
151 - 160
161 - 170
171 - 180
181 - 190
191 - 200
201 - 210
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065/01/293.jpg
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283
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<
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<
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<
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<
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gr.
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</
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<
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<
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m.
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</
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<
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<
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<
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type
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gr.
<
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type
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</
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<
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<
emph
type
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m.
<
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type
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</
cell
>
</
row
>
<
row
>
<
cell
>
<
emph
type
="
italics
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Reinhold.
<
emph.end
type
="
italics
"/>
</
cell
>
<
cell
>Polar altit.</
cell
>
<
cell
>51</
cell
>
<
cell
>18</
cell
>
<
cell
>Altit. of the Star</
cell
>
<
cell
>79</
cell
>
<
cell
>30</
cell
>
</
row
>
<
row
>
<
cell
>
<
emph
type
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Hainzel.
<
emph.end
type
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</
cell
>
<
cell
/>
<
cell
>48</
cell
>
<
cell
>22</
cell
>
<
cell
/>
<
cell
>36</
cell
>
<
cell
>34</
cell
>
</
row
>
<
row
>
<
cell
/>
<
cell
/>
<
cell
>2</
cell
>
<
cell
>56</
cell
>
<
cell
/>
<
cell
>2</
cell
>
<
cell
>56</
cell
>
</
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>
<
row
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<
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/>
<
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<
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>
<
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type
="
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"/>
gr.
<
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type
="
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"/>
</
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>
<
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>
<
emph
type
="
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"/>
m.
<
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type
="
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</
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<
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/>
<
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>
<
emph
type
="
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"/>
gr.
<
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type
="
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"/>
</
cell
>
<
cell
>
<
emph
type
="
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"/>
m.
<
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type
="
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"/>
</
cell
>
</
row
>
<
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>
<
cell
>
<
emph
type
="
italics
"/>
Camerar.
<
emph.end
type
="
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"/>
</
cell
>
<
cell
>Polar altit.</
cell
>
<
cell
>52</
cell
>
<
cell
>24</
cell
>
<
cell
>Altit. of the Star</
cell
>
<
cell
>24</
cell
>
<
cell
>17</
cell
>
</
row
>
<
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>
<
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>
<
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type
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Hagecius
<
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type
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</
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>
<
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/>
<
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>48</
cell
>
<
cell
>22</
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>
<
cell
/>
<
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>20</
cell
>
<
cell
>15</
cell
>
</
row
>
<
row
>
<
cell
/>
<
cell
/>
<
cell
>4</
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>
<
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>2</
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>
<
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/>
<
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>4</
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>
<
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>2</
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>
</
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>
</
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>
<
p
type
="
main
">
<
s
>Of the remaining combinations that might be made of the
<
lb
/>
ſervations of all theſe Aſtronomers, thoſe that make the Stars
<
lb
/>
lime to an infinite diſtance, are many in number, namely, about
<
lb
/>
30. more than thoſe who give the Star, by calculation, to be
<
lb
/>
low the Moon; and becauſe (as it was agreed npon between us) it
<
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/>
is to be believed that the Obſervators have erred rather little than
<
lb
/>
much, it is a manifeſt thing that the corrections to be applied to
<
lb
/>
the Obſervaations, which make the ſtar of an infinite altitude, to
<
lb
/>
reduce it lower, do ſooner, and with leſſer amendment place it in
<
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/>
the Firmament, than beneath the Moon; ſo that all theſe applaud
<
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/>
the opinion of thoſe who put it amongſt the fixed Stars. </
s
>
<
s
>You may
<
lb
/>
adde, that the corrections required for thoſe emendations, are
<
lb
/>
much leſſer than thoſe, by which the Star from an unlikely
<
lb
/>
mity may be removed to the height more favourable for this
<
lb
/>
thour, as by the foregoing examples hath been ſeen; amongſt
<
lb
/>
which impoſſible proximities, there are three that ſeem to remove
<
lb
/>
the Star from the Earths centre, a leſſe diſtance than one
<
lb
/>
ameter, making it, as it were, to turn round under ground, and
<
lb
/>
theſe are thoſe combinations, wherein the Polar altitude of one
<
lb
/>
of the Obſervators being greater than the Polar altitude of the
<
lb
/>
other, the elevation of the Star taken by the firſt, is leſſer than the
<
lb
/>
elation of the Star taken by the latter.</
s
>
</
p
>
<
p
type
="
main
">
<
s
>The firſt of theſe is this of the
<
emph
type
="
italics
"/>
Landgrave
<
emph.end
type
="
italics
"/>
with
<
emph
type
="
italics
"/>
Gemma,
<
emph.end
type
="
italics
"/>
<
lb
/>
where the Polar altitude of the
<
emph
type
="
italics
"/>
Landgrave 51 gr. </
s
>
<
s
>18 min.
<
emph.end
type
="
italics
"/>
is
<
lb
/>
greater than the Polar altitude of
<
emph
type
="
italics
"/>
Gemma,
<
emph.end
type
="
italics
"/>
which is 50
<
emph
type
="
italics
"/>
gr. </
s
>
<
s
>50 m.
<
emph.end
type
="
italics
"/>
<
lb
/>
But the altitude of the Star of the
<
emph
type
="
italics
"/>
Landgrave 79 gr. </
s
>
<
s
>30 min.
<
emph.end
type
="
italics
"/>
<
lb
/>
is leſſer than that of the Star, of
<
emph
type
="
italics
"/>
Gemma 79 gr. </
s
>
<
s
>45 min.
<
emph.end
type
="
italics
"/>
<
lb
/>
<
arrow.to.target
n
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table57
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</
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</
p
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</
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>
</
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</
text
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</
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>