The determination of
longitude is a significant practical problem in
cartography and
navigation.
Philip III of Spain offered a prize for a method to determine the longitude of a ship out of sight of land, and
Galileo proposed a method of establishing the time of day, and thus longitude, based on the times of the eclipses of the moons of
Jupiter; this method was not significantly improved until accurate mechanical clocks were developed in the eighteenth century. Galileo proposed this method to the Spanish crown (1616–1617) but it proved to be impractical, because of the inaccuracies of Galileo's timetables and the difficulty of observing the eclipses on a ship. However, with refinements, the method could be made to work on land. After studies in Copenhagen, Rømer joined
Jean Picard in 1671 to observe about 140 eclipses of Jupiter's moon
Io on the island of
Hven at the former location of
Tycho Brahe's observatory of
Uraniborg, near Copenhagen, over a period of several months, while in Paris
Giovanni Domenico Cassini observed the same eclipses. By comparing the times of the eclipses, the difference in longitude of Paris to Uraniborg was calculated. Cassini had observed the moons of Jupiter between 1666 and 1668, and discovered discrepancies in his measurements that, at first, he attributed to light having a finite speed. In 1672 Rømer went to Paris and continued observing the satellites of Jupiter as Cassini's assistant. Rømer added his own observations to Cassini's and observed that times between eclipses (particularly those of Io) got shorter as Earth approached Jupiter, and longer as Earth moved farther away. Cassini made an announcement to the Academy of Sciences on 22 August 1676:
This second inequality appears to be due to light taking some time to reach us from the satellite; light seems to take about ten to eleven minutes [to cross] a distance equal to the half-diameter of the terrestrial orbit. . Rømer compared the duration of Io's orbits as Earth moved towards Jupiter (F to G) and as Earth moved away from Jupiter (L to K). Cassini did not pursue this reasoning, but Rømer adopted it and set about proving the idea, using a selected number of observations performed by Picard and himself between 1671 and 1677. Rømer presented his results to the
French Academy of Sciences, and it was summarised soon after by an anonymous reporter in a short paper, ''
, published 7 December 1676 in the Journal des sçavans''. The reporter used cryptic phrasing which obfuscated Rømer's reasoning in the process. Rømer himself never published his results. Rømer's reasoning was as follows. Referring to the illustration, assume the Earth is at point
L, and Io emerges from Jupiter's shadow at point
D. After several orbits of Io, at 42.5 hours per orbit, the Earth is at point
K. If light is not propagated instantaneously, the additional time it takes to reach
K, which he reckoned about 3½ minutes, would explain the observed delay. Rømer observed
immersions at point
C from positions
F and
G, to avoid confusion with
eclipses (Io shadowed by Jupiter from
C to
D) and
occultations (Io hidden behind Jupiter at various angles). In the table below, his observations in 1676, including the one on 7 August, believed to be at the opposition point
H, and the one observed at
Paris Observatory to be 10 minutes late, on 9 November. By
trial and error, during eight years of observations, Rømer worked out how to account for the finite speed of light when reckoning the
ephemeris of Io. He calculated the delay as a proportion of the angle corresponding to a given Earth's position with respect to Jupiter,
Δt = 22·()[minutes]. When the angle α is 180° the delay becomes 22 minutes, which is the time necessary for the light to cross a distance equal to the diameter of the
Earth's orbit,
H to
E. Rømer neither calculated this ratio, nor did he give a value for the speed of light. However, many others calculated a speed from his data, the first being
Christiaan Huygens; after corresponding with Rømer and eliciting more data, Huygens deduced that light travelled Earth diameters per second, which is approximately 212,000 km/s. Rømer's view that the velocity of light was finite was not fully accepted until measurements of the so-called
aberration of light were made by
James Bradley in 1727. In 1809, again making use of observations of Io, but this time with the benefit of more than a century of increasingly precise observations, the astronomer
Jean Baptiste Joseph Delambre reported the time for light to travel from the Sun to the Earth as 8 minutes and 12 seconds. Depending on the value assumed for the astronomical unit, this yields the speed of light as just a little more than 300,000 kilometres per second. The modern value is 8 minutes and 19 seconds, and a speed of 299,792,458 m/s. == Inventions ==