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| Demonstration
touchant le mouvement de la lumiere trouvé
par M. Römer de l’Academie Royale des Sciences - [anonymous
author 7-December-1676]
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[selected
passages by Giampiero Barbieri – founding
member]
... in some passages the author uses a cryptic
kind of language, trying to hide his non complete understanding of the
problem ... these passages have been cancelled ...
following, a particular calculation has also been worked out by "Pighin",
giving back to Römer all his merits and greatness .... |
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« Since long,
Philosophers were trying to put up some kind of experiment, [to decide]
whether the light moved [straight away] from one point to another, whatever
the distance was or if such motion, instead, required a certain time.
i
Römer, a member
of the Royal Academy of Sciences, when carrying out observations on the
first satellite of Jupiter noticed an average delay …
» (*)
| (*) |
Cassini
discovered this delay well before
Römer and
ascribed it to the limited velocity of the light ...
... anyway he did
not pursue this intuition further as, with the other three Medicean satellites,
he was not able to measure this type of delay...
the problem was not of logic nature, as he assumed. It was simply a matter
of measurements... actually, measurement becomes
unforeseeable when satellites are slower... least, but not last, trying
to fix the moment when a satellite enters or outcomes from the shaded zone
is a problem and computation becomes uncertain ....
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«…
Let A be the
Sun, B Jupiter,
C the first satellite
eclipsed by Jupiter and out-coming in D,
and let the Earth, positioned at different distances from Jupiter, be EFGHLK.
i
Assuming the Earth to be in L,
near to the second Quadrature with Jupiter, just when the first satellite
emerges from the shade in D; if 42 hours and a half are needed to observe
a revolution of the said satellite, the Earth
will find itself in K the next time the satellite outcomes from D.
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It is obvious that if the light takes its time
to cross the distance from L to K, the
satellite shall be seen some time later at D.
This would not happen if the Earth could stand stationary in L.
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The revolution of this satellite, observed at
its out-coming from the shade, will be delayed
that much time that light will take to go from L to K.
i
On the contrary, in the other Quadrature FG,
where the Earth is becoming nearer, it meets the light and the
revolutions of the eclipses will also be shorter, while the emersions will
be longer... »
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From theory to facts ... |
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«…
The theory that light does not require time
is not tenable. After examining facts in detail, it has been found out
that what is not noticeable during two revolutions, becomes remarkably
relevant in the case of numerous revolutions, i.e.
40. If such revolutions are observed from
F, they will be considerably shorter than those at the opposite side of
the Zodiac. Difference is 22 minutes between
H and E (**)
double the distance Earth-Sun ...
»
i
«…
The necessity for this new Equation, regarding
the delay of the light, was a routine followed
up during all the observations carried out at the Observatory of the Royal
Academy since the last 8 years. It was confirmed
further by the Emersion of the first Satellite
observed in Paris on 9 November last at 5h 35’ 45’’ in the evening [
this observation was not recorded correctly...
"Io’s" emersion actually took place at 17h 11' 15'' on 9 November 1676
- Universal Time – when the Sun was about to set, but still above the horizon
... ], 10
minutes later than expected, compared to the
observation carried out in August, when the Earth was much nearer to Jupiter.
An event Römer
anticipated to the Academy at the beginning of September ...
»
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| From
facts to a clever analysis of the same ... |
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«… “in
toto” to make sure these inequalities
were caused by a delay of the light, it is
necessary to prove this delay did not derive from any type of eccentricity
or from other causes, as those generally taken into consideration to explain
the anomalies of the Moon and of the other Planets.
i
For certain it has been confirmed Jupiter’s
first satellite is eccentric and
its revolutions are anticipated or delayed
in accordance to how much Jupiter moves near or far away from the Sun.
The revolutions of the first Satellite are
unequal ... [a
point of view of the anonymous author]
... without these three last causes of inequality
preventing the first [the
light’s finite velocity] to
become manifest ... »
i |
| i
Note |
| (**) |
This value should correspond to the true value
of light’s velocity equal to 227,000 km/sec. ... but this is against what
affirmed in "Companion to the Cosmos by
John Gribbin – Phoenix Edition"- see: Römer, Ole (1644 – 1710) - at
page 417:
i
«… The
figure he came up with was equivalent, in modern units, to 225,000 km per
second. The difference from the true value was given by the value of the
mean distance Earth-Sun, accepted at the time. Using the same calculation
with the modern value, for the size of the Earth’s orbit, gives 298,000
km/sec; the modern value for the speed of light is 299,792 km/sec
... »
i
This last result is in accordance, in order of
size, with the error of "Pighin’s"
particular computation ... |
|
ii
selected passages from an article written
by an anonymous author... in some passages the author uses a cryptic kind
of language, trying to hide his non complete understanding of the problem
... these passages have been cancelled ... following, a particular calculation
has been worked out by "Pighin",
giving back to Römer
all his merits and greatness ....
i |
z |
| i |
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| Let us reckon
... the matter is not exactly trite ... |
| i |
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As suggested by the anonymous author,
who wrote of Römer,
it is better to be near to a quadrature and
to carry out evaluations on 40 satellite periods
.... in this instance, the second quadrature has been chosen, where Earth
is moving away ... and where the satellite is out-coming from the eclipse...
the graph shows the variation of the distance Earth-Jupiter as days pass
by... if the orbits were perfect circles the
graph would simply show a sine-curve, but
as the orbits are elliptical a slight modulation
may be seen, the period being similar to the
synodic period of Jupiter... only 35 orbits
were selected, as orbit no. 40th was below Leivi’s horizon,
working seat of the Association ...
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Description of the used methodology
....
With the use of a spreadsheet
let’s now compute:
results are on the left...
on the right is a detailed explanation of the
different steps...
"Io’s" out-comings from shade have been measured
with the precision of a second, using Perseus
... an extremely difficult operation for both Cassini
and Römer,
who instead, based their calculations on definite measures...
The problem also showed a certain chaotic aspect
in the value of "Io’s"
synodic period where significant errors are due to the variations of the
fifth decimal number ... trying to exactly measure the synodic period of
"Io"
is quite difficult, because of its delays and of its advances...
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The above shows the mathematical difficulties
and the true greatness of Cassini
and of Römer
who, both were able to carry out such accurate measurements and to use
statistical methods which, at the time, were just at their starting stage.
They also used a good deal of "common sense" to reduce the variance ...
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"Io"
takes 3.8 minutes to transit from shade to
light. Its vision,
when it outcomes from the eclipse, is conditioned both by the atmospheric
changes and by the eye sight of the observer...
an additional risk when taking measures...
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We are about the second Quadrature
with Jupiter ... the satellite fully
emerges on 24 Nov. 1678 at 21h 20m 51s [Orbit
no 01] and
again it is seen on 25 Jan. 1679 at 20h 9m 29s [Orbit
no 35] ...
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Starting data are the synodic period of "Io",
the two Julian dates [first
three lines in green]
and the distance Earth-Jupiter measured at the two dates a.m.[second
two lines in green]...
i
The Perseus time, equal to the difference between
the two dates JD, is computed and divided
by the synodic period of "Io".
The number of orbits
is obtained by rounding to the nearest whole
number [first line in blue]
....
The synodic period is multiplied by the number
of orbits to obtain the nominal time
.... difference between the two times is computed
and expressed in days, hours , minutes and seconds ...
The difference between the two distances from
Jupiter divided by the difference in seconds gives the
light’s velocity in Km/sec. [last
line in blue]
... |
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(**)
(*) |
Values in Julian Days were computed with the
aid of Perseus
Values of the distances Earth-Jupiter were
computed with the aid of Solex91 of Prof. Aldo Vitagliano |
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