[Folder Location]
When Light Slowed Down for Olaf R/omer
______________________________________
Timothy Paul Smith
University of New Hampshire
tim.smith@unh.edu
(received: October 25, 1995)
(first printed - Vol. 2, No. 4 - November 1995)
One of the major revolutions of physics in the twentieth century
has been the introduction of special relativity. It arises from the
counter-intuitive premise that the speed of light is constant in all
references frames. Three hundred thousand kilometers each second, no
matter if I am at rest, or flying by on the tail of a comet, or
piggy-backed on a TeV proton. It upsets and angers us. When solids are
contracted, time dilated and nothing is simultaneous. That the speed of
light is constant in all references frames is not obvious to me in my
everyday life. In fact that light has a finite speed is not obvious
either.
Hero of Alexandria (1st-century) tells us that of course the
speed of light is infinite. To prove this he tells us to go outside on
a clear and starry night with our eyes closed. Turn our face towards
the sky and open our eyes. We instantly see stars.
Now this may seem like an absurd `proof' to us until we realize
that most of the theories of light at that time were really more
interested in explaining sight. Hero subscribed essentially to the
theory of Pythagoras (c 580- c 500 bc). We see things by `touching' them
with our `eye-ray' (my word). Sight originates at our eyes, propagates
to the object, and returns to our eyes. Thus sight, and therefore
light, is modeled on the sense of touch.
This was not the only theory of light in antiquity. The Atomist
described light as motes which started out at the object and propagated
to the observe;
The images must cross tremendous space
In time almost dimensionless. This happens
Because they need only the slightest push,
...
In the first shine of starlight, see the stars
Respond that very instant, radiant
- Lucretius [1]
Perhaps I should not put too much emphasis on the writings of
antiquity. What could they say when such concepts as infinity and
infinitesimal were not developed into the Calculus concepts we presently
use?
The theory of eye-rays was put to rest by an Arabic physicist
and mathematician named Alhazen, about the year 10000, but the speed of
light, finite or infinite, remained veiled in its rapidity.
Galileo Galilei (1564-1642) considered it but a simple problem
to solve, in principle. In his book "Dialogues Concerning Two New
Sciences" (1638) he proposed:
SIMPLICIO: Everyday experience shows that the propagation
of light is instantaneous; for when we see a piece of
artillery fired, at great distance, the flash reaches
our eyes without lapse of time; but the sound reaches
the ear only after a noticeable interval.
SAGREDO: Well, Simplicio, the only thing I am to infer
from this familiar bit of experience is that sound, in
reaching our ear, travels more slowly than light; it
does not inform me whether the coming of the light is
instantaneous or whether, although extremely rapid, it
still occupies time. An observation of this kind tells
us nothing more than one in which it is claimed that
"As soon as the sun reaches the horizon its light
reaches our eyes"; but who will assure me that these
rays had not reached this limit earlier than they
reached our vision?
SALVIATI: The small conclusiveness of these and other
similar observations once led me to devise a method by
which one might accurately ascertain whether illumination,
i.e., the propagation of light, is really instantaneous.
The fact that the speed of sound is as high as it is,
assures us that the motion of light cannot fail to be
extraordinarily swift. The experiment which I devised
was as follows:
Let each of two persons take a light contained in a
lantern, or other receptacle, such that by the
interposition of the hand, the one can shut off or admit
the light to the vision of the other. Next let them stand
opposite each other at a distance of a few cubits and
practice until they acquire such skill in uncovering and
occulting their lights that the instant one sees the light
of his companion he will uncover his own. After a few trials
the response will be so prompt that without sensible error
the uncovering of one light is immediately followed by the
uncovering of the other, so as soon as one exposes his light
he will instantly see that of the other. Having acquired skill
at this short distance let the two experimenters, equipped as
before, take up positions separated by a distance of two or
three miles and let them perform the same experiment at night,
noting carefully whether the exposures and occultations occur
in the same manner as at short distances; if they do, we may
safely conclude that the propagation of light is instantaneous;
but if time is required at a distance of three miles which,
considering the going of one light and the coming of the other,
really amounts to six, then the delay ought to be easily
observable. If the experiment is to be made at still greater
distances, say eight or ten miles, telescopes may be employed,
each observer adjusting one for himself at the place where he
is to make the experiment at night; then although the lights
are not large and are therefore invisible to the naked eye at
so great a distance, they can readily be covered and uncovered
since by aid of the telescopes, once adjusted and fixed, they
will become easily visible.
SAGREDO: This experiment strikes me as a clever and reliable
invention. But tell us what you conclude from the results.
SALVIATI: In fact I have tried the experiment only at a short
distance, less than a mile, from which I have not been able
to ascertain with certainty whether the appearance of the
opposite light was instantaneous or not; but if not
instantaneous it is extraordinarily rapid - I should call
it momentary; and for the present I should compare it to
motion which we see in the lightning flash between clouds
eight or ten miles distant from us.
- Galileo Galilei [2]
Whereas Galileo thought that the only aspect of the speed of
light which needed to be addressed was measuring, at the same Descartes
(1596-1650) tells us "I confess that I know nothing of Philosophy, if
the Light of the Sun is not transmitted to our Eyes in an instant" [3]
------====+++====------
In all introductory astronomy textbooks we are told that the
speed of light was measured in 1676. But I want to stay with Galileo for
the present.
On the night of January 7, 1610 Galileo turned his telescope to
Jupiter and noted the planet in front of three fixed stars. He sketched
in his notebook;
* * O * (Jan. 7, 1610)
Coincidentally, the next night he trained his telescope once again on
Jupiter, and this time saw;
O * * * (Jan. 8, 1610)
He concluded that Jupiter had moved to the left (east), which he knew
it should not be doing. He also thought that the "fixed stars" appeared
to be a bit closer to each other then on the previous night. January
9-th was cloudy. On the 10-th he observed;
* * O (Jan. 10, 1610)
and concluded that Jupiter blocked one of the "stars". He was now truly
intrigued. In his sketches he tried to indicate the magnitude of the
"stars"
X * O (Jan. 11, 1610)
* . O * (Jan. 12, 1610)
The third "star" appeared out from behind Jupiter at about 3 o'clock in
the morning. Finally he spotted four;
* O * * * (Jan. 13, 1610)
That same year Galileo realized not only where the "stars"
really moons of Jupiter, but also here was a clock in the heavens which
everyone one earth could see. He knew that this meant you could measure
longitude!
------====+++====------
The whole idea of using eclipses to measure longitude is an old
one, usually attributed to Hero of Alexandria [4] (again!). If an
observer in Alexandria and Rome where to both note the instant they
observed a lunar eclipse in local time, then later compared notes they
would find that their observations varied by over an hour (1h 10m),
which would mean about 17-degrees of longitude. Hero already knew how
to measure latitude, and the distance around the earth, thus he could
calculate the distance between Alexandria and Rome.
I will note that (depending on the latitude) on error of ten
minutes leads to an error of about 150 miles. So how good are the
clocks of antiquity?
------====+++====------
Galileo's moons of Jupiter were being eclipsed every day or so.
If he could construct a table predicting the times of eclipses as viewed
from his observatory, a navigator anywhere in the world could calculate
their longitude accurately and frequently. So for several years Galileo
took data on Jupiter's moons, but was never able to construct his table
with any great predictive power, and finally gave up the project.
In 1668 Giovanni Domenico Cassini (1625-1712) published his
tables of the eclipses of the moons of Jupiter, and on the strength of
that opus he was invited by Louis XIV to continue his observations at
the observatory in Paris. A few years later the Danish astronomer Olaus
R/omer joined him, and in 1675 R/omer proposed that the discrepancy in
time were due to the finite velocity of the speed of light. In fact he
calculated that it took fourteen minutes for light to cross the diameter
of the earths orbit.
The observation sounds so straight forward. First measure the
period of orbit of one of the moons of Jupiter. To do that just count
the number of orbits in an extended period of time, say ten years,
then divide the time by the number of orbits. Now on a day when the
earth is close to Jupiter predict the time of an eclipse six months
later. If you then measure the time of the eclipse six months later you
will observe a sixteen and a half minute delay (R/omer originally
reported fourteen minutes).
(Io) (Jupiter) (Earth) (Sun) [at time 0]
| <-- light 0 --> |
(Io) (Jupiter) (Sun) (Earth) [at time 6]
| <--------------- light+6 -------------> |
| <-- light 0 --> | <--- light across --->|
the earths orbit
R/omer went on to calculate the speed of light as 140,000
miles/sec. = 225,000 km/s. Modern measurements yield 186,000 miles/sec
= 300,000 km/s. The problem in R/omer's day was not the timing (the 14
minutes was soon corrected), but the distance. The distance to the Sun
was not well known.
------====+++====------
The data seems so clear, the signature so evident, but that is
from our 300+ year vantage point. Newton wrote in the first edition
(1686) of Principia:
Namq; Lucem successive propagari & spatio quasi
decem minutorum primorum a Sole as Terram venire,
jam constat per Phaenomena Satellitum *Jovis*,
Observationibus diversorum Astronomorum confirmata.
- Newton (1686) [5]
[ For it is now certain from the phenomena of Jupiter's
satellites, confirmed by the observations of different
astronomers, that light is propagated in succession, and
requires about seven or eight minutes to travel from the
sun to the earth]
- Newton (1725) [6]
Yet when Cassini published his tables of eclipses in 1693 he refused to
use the "equation of light". Instead there was a stream of `classical'
corrections; the eccentricities of the orbits, the incline of the
planes of the orbits, and so forth. The problem was that the equation
of light did not explain all of the data:
It appears then, that we must renounce, though perhaps
with regret, the ingenious and seductive hypothesis of
the successive propagation of light . . . . . How little
prevents us from falling into great errors! If Jupiter
had but one satellite, or if the eccentricity had been
less, and these two things are very possible, we should
have concluded with the the utmost confidence that light
traversed the annual orbit of the earth in 14 minutes.
- Fontenelle [7]
The problem for the equation of light correction is that it did
not explain all the data. It only explained the deviation in the
"principle moon" (Io), the other moons were not periodic with a simple
speed of light correction factor.
Farther observations seemed to be filled with all types of
problematic details. In 1693 Cassini measured the inclination of the
orbits of all the moons at 2-deg 55-min. In 1707 Maraldi found that the
incline of the second moon was 3-deg 33-min! This is one of those
things which are not suppose to change. The times of the eclipses of
some of the moons varied by as much as an hour! It appeared as if
predictability in the orbits had broken down.
In retrospect we quickly realize that the problem was that this
is a few-but-not-two body problem, which can not really be calculated
with circles and close orbits. This too was becoming apparent in the
first half of the eighteenth century. Bradley recognized that the
discrepancies might be due to the mutual attraction of the moon,
While we carefully attend to future observations, by
means of which the theory of the satellites may be
established,*'a posteriori*, let us hope that some
rival of the great Newton, relying upon sure and tried
principle of gravitation, will achieve the noble task
of investigating *'a priori* the effects of their
mutual attraction
- Bradley [8]
Still, the theory of R/omer did eventually prevail, and this
first measurement of the speed of light became part of our textbooks.
------====+++====------
When I started this study I expected to find a great resistance
to Olaus R/omer on the grounds that a finite velocity of light might
have been unthinkable. But instead I found it was resisted on the
perfectly valid point that it didn't explain the discrepancies in *all*
of the data. To paraphrase Fontenelle; If there had been but one moon,
they would have accepted the speed of light much sooner.
The other thing which struck me is the practical application of
science which drove this study, the search for a tool to measure
longitude. Hero, Galileo, Cassini and even R/omer were trying to
calibrate this time piece in the sky. The speed of light seems like
such an abstract or at least esoteric measurement, it is had to imagine
a sea-captain relying upon its measurement to steer clear of Scylla and
Charybdis!
------====+++====------
[1] Lucretius, "On The Nature Of Things".
[2] Galileo Galilei, "Dialogues Concerning Two New Sciences" (1638).
[3] Rene Descartes, "XVII Letter of the III Volume ", quoted by
Francois-Marie Voltaire, "The Elements of Newton's Philosophy ", p 9-10 (1738).
[4] Hero of Alexandria, "Dioptra".
[5] Isaac Newton, "Principia" (1686).
[6] Isaac Newton, "Principia" third edition (1725).
[7] Bernard Le Bovier Fontenelle (1657-1757),
"M'em. Acad. des Sciences, Hist." p. 80
[8] James Bradley (1693-1762).
[Follow-ups] |
||||||||||||||||||
Replying here is disabled according to your current identity.
Hosted by VivBoard
| Evaluation:
|
|||||||||||
| Feel:
|
|||||||||||
| Clear | |||||||||||
| People's view: | |||||||||||