The Trouvelot astronomical drawings manualTrouvelot, E. L. (Etienne Leopold)
Science
The Trouvelot astronomical drawings manual
Trouvelot, E. L. (Etienne Leopold)
Astronomy -- Pictorial works
When a comet is first discovered with the telescope at a great distance
from the Sun, it is difficult to predict whether it will become visible
to the naked eye, or will remain a telescopic object, as it is only in
approaching the Sun that these singular bodies acquire their full
development. Thus, Donati's comet, whose tail became so conspicuous an
object at its full appearance in 1858, remained two months after its
discovery by the telescope without any indication of a tail. The comet
of Halley, which before and after its return in 1759, remained five
years inside of the orbit of Saturn, showed not the least trace of its
presence during the greater part of this time. Nothing but calculation
could then indicate the position in the sky of this invisible object,
which was so prominent when it approached the Sun.
Another curious phenomenon exhibited by comets, and first noticed by
Valz, is that in approaching the Sun the nebulosity composing these
bodies contracts, instead of dilating, as would be naturally supposed
from the greater amount of solar heat which they must then receive. In
receding from the Sun, on the contrary, they expand gradually. As comets
approach the Sun, the tail and nucleus are developed, while the
nebulosity originally constituting these comets contracts, as if its
material had been partly consumed in this development. In a certain
sense it may be said that the comets are partly created by the Sun; in
more exact terms, the changes of form which they undergo are induced by
the Sun's action upon them at different distances and under varying
conditions. Moreover, they are rendered visible by its influence,
without which they would pass unperceived in our sky. When a comet
disappears from view, it is not because its apparent diameter is so much
reduced by the distance that it vanishes, but rather on account of the
diminution of its light, both that which it receives from the Sun, and
its own light; these bodies being in some degree self-luminous, as will
be shown below.
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