Skip to main content

Saturn’s Missing Helium



Like Jupiter, Saturn is thought to have a large rocky core. But unlike
Jupiter, data from Earth-based telescopes and spacecraft show
that the atmosphere of Saturn has a serious helium deficiency: Its
chemical composition is 96.3% hydrogen molecules, 3.3% helium,
and 0.4% other substances (by mass, 92% hydrogen, 6%
helium, and 2% other substances). This is a puzzle because Jupiter
and Saturn are thought to have formed in similar ways from the
gases of the solar nebula (see Section 8-4), and so both planets
(and the Sun) should have essentially the same abundances of hydrogen
and helium. So where did Saturn’s helium go?
The explanation may be simply that Saturn is smaller than
Jupiter, and as a result Saturn probably cooled more rapidly. (We
saw in Section 7-6 why a small world cools down faster than a
large one.) This cooling would have triggered a process analogous
to the way rain develops here on Earth. When the air is cool
enough, humidity in the Earth’s atmosphere condenses into raindrops
that fall to the ground. On Saturn, however, it is droplets
of liquid helium that condense within the planet’s cold, hydrogenrich
outer layers. In this scenario, helium is deficient in Saturn’s
upper atmosphere simply because it has fallen farther down into
the planet. By contrast, Jupiter’s helium has not rained out because
its upper atmosphere is warmer and the helium does not
form droplets.

In this scenario, Jupiter and Saturn both have about the same
overall chemical composition. But Saturn’s smaller mass, less than
a third that of Jupiter, means that there is less gravitational force
tending to compress its hydrogen and helium. This explains why
Saturn’s density is only about half that of Jupiter, and is in fact
the lowest of any planet in the solar system.


Comments

Popular posts from this blog

The Ptolemaic System

Explaining the nonuniform motions of the five planets was one of the main challenges facing the astronomers of antiquity. The Greeks developed many theories to account for retrograde motion and the loops that the planets trace out against the background stars. One of the most successful and enduring models was originated by Apollonius of Perga and by Hipparchus in the second century B.C. and expanded upon by Ptolemy, the last of the great Greek astronomers, during the second century A.D.  sketches the basic concept, usually called the Ptolemaic system. Each planet is assumed to move in a small circle called an epicycle, whose center in turn moves in a larger circle, called a deferent, which is centered approximately on the Earth. Both the epicycle and deferent rotate in the same direction As viewed from Earth, the epicycle moves eastward along the deferent. Most of the time the eastward motion of the planet on its epicycle adds to th...

Lorentz transformation

Lorentz transformation and its inverse : Define an event to have spacetime coordinates  ( t , x , y , z )  in system  S  and  ( t ′, x ′, y ′, z ′)  in a reference frame moving at a velocity v with respect to that frame,  S ′. Then the Lorentz transformation specifies that these coordinates are related in the following way: {\displaystyle {\begin{aligned}t'&=\gamma \ (t-vx/c^{2})\\x'&=\gamma \ (x-vt)\\y'&=y\\z'&=z,\end{aligned}}} where {\displaystyle \gamma ={\frac {1}{\sqrt {1-{\frac {v^{2}}{c^{2}}}}}}} is the Lorentz factor and  c  is the speed of light in vacuum, and the velocity  v  of  S ′, relative to  S , is parallel to the  x -axis. For simplicity, the  y  and  z  coordinates are unaffected; only the  x  and  t  coordinates are transformed. These Lorentz transformations form a one-param...

Elliptically Polarized Light

When light is passed through a polarizer, it gets polarized according to the  properties of the polarizer. Considering an extremely Efficient polarizer, The light that emerges out is said to be plane polarized light. The vibration of electric and magnetic vectors is confined to one plane. When Two Such Plane Polarized Lights Waves, Having Unequal Magnitude And Moving Perpendicular To Each Other, Interfere, They Result Into An Elliptically Polarized Light.  The equation of resultant wave represents that of ellipse.                                                                                                {\displaystyle B=|\mathbf {E} |{\sqrt {\frac {1-{\sqrt {1-\sin ^{2}(2\theta )\sin ^{2}\beta }}}{2}}}} ...