FREE BOOKS

Author's List




PREV.   NEXT  
|<   239   240   241   242   243   244   245   246   247   248   249   250   251   252   253   254   255   256   257   258   259   260   261   262   263  
264   265   266   267   268   269   270   271   272   273   274   275   276   277   278   279   280   281   282   283   284   285   286   287   288   >>   >|  
ces of Jupiter's satellites. Calculation does not yield in precision to direct observation. In this group of satellites, considered as an independent system of bodies, Laplace found a series of perturbations analogous to those which the planets experience. The rapidity of the revolutions unfolds, in a sufficiently short space of time, changes in this system which require centuries for their complete development in the solar system. Although the satellites exhibit hardly an appreciable diameter even when viewed in the best telescopes, our illustrious countryman was enabled to determine their masses. Finally, he discovered certain simple relations of an extremely remarkable character between the movements of those bodies, which have been called _the laws of Laplace_. Posterity will not obliterate this designation; it will acknowledge the propriety of inscribing in the heavens the name of so great an astronomer beside that of Kepler. Let us cite two or three of the laws of Laplace:-- If we add to the mean longitude of the first satellite twice that of the third, and subtract from the sum three times the mean longitude of the second, the result will be exactly equal to 180 deg.. Would it not be very extraordinary if the three satellites had been placed originally at the distances from Jupiter, and in the positions, with respect to each other, adapted for constantly and rigorously maintaining the foregoing relation? Laplace has replied to this question by showing that it is not necessary that this relation should have been rigorously true at the origin. The mutual action of the satellites would necessarily have reduced it to its present mathematical condition, if once the distances and the positions satisfied the law approximately. This first law is equally true when we employ the synodical elements. It hence plainly results, that the first three satellites of Jupiter can never be all eclipsed at the same time. Bearing this in mind, we shall have no difficulty in apprehending the import of a celebrated observation of recent times, during which certain astronomers perceived the planet for a short time without any of his four satellites. This would not by any means authorize us in supposing the satellites to be eclipsed. A satellite disappears when it is projected upon the central part of the luminous disk of Jupiter, and also when it passes behind the opaque body of the planet. The following is another very simpl
PREV.   NEXT  
|<   239   240   241   242   243   244   245   246   247   248   249   250   251   252   253   254   255   256   257   258   259   260   261   262   263  
264   265   266   267   268   269   270   271   272   273   274   275   276   277   278   279   280   281   282   283   284   285   286   287   288   >>   >|  



Top keywords:
satellites
 

Laplace

 

Jupiter

 

system

 

eclipsed

 

longitude

 

planet

 

distances

 

relation

 
positions

rigorously

 

satellite

 

observation

 

bodies

 

condition

 

satisfied

 

mathematical

 
reduced
 
present
 
approximately

elements

 

synodical

 

equally

 

employ

 

necessarily

 

precision

 

replied

 

question

 
considered
 

maintaining


foregoing
 
showing
 

adapted

 
mutual
 
plainly
 
action
 

origin

 

direct

 
constantly
 
disappears

projected
 

central

 

supposing

 
authorize
 
luminous
 

opaque

 

passes

 

Bearing

 

Calculation

 

respect