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<p>the density increases), must vary in their absolute velocities according to their distances from the axis; and each portion cannot have its distance
from the axis changed by circulating currents, which it must continually be, without loss or gain in its quantity of motion: through the medium of
fluid friction, force must be expended, now in increasing its motion and now in retarding its motion. Hence, when the larger spheroid has also a
higher velocity of rotation, the relative slowness of the circulating<U>currents, and</U>the consequent retardation of cooling, must be much greater </p>
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<p align="right">than is implied by the extra distances to be travelled. And now observe the correspondence between inference and fact. In the first
place, if we compare the group of the great planets, Jupiter, Saturn, and Uranus, with the group of the small planets, Mars, Earth, Venus, and
Mercury, we see that low density goes along with great size and great velocity of rotation, and that high density goes along with small size and
small velocity of rotation. In the second place, we are shown this relation still more clearly if we compare the extreme instances—Saturn and Mercury.
The special contrast of these two, like the general contrast of the groups, points to the truth that low density, like the satellite-forming tendency,
is hiociated with the ratio borne by centrifugal force to gravity; for in the case of Saturn with his many satellites and least density, centrifugal
force at the equator is nearly of gravity, whereas in Mercury with no satellite and greatest density centrifugal force is but of gravity. </p>
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<p align="center" style="font: 9px;">There are, however, certain factors which, working in an opposite way, qualify and complicate these effects. Other things equal, mutual
gravitation among the parts of a large mhi will cause a<I>greater evolution of heat than is similarly caused in a small mhi; and the resulting</I>
difference of temperature will tend to produce more rapid dissipation of heat. To this must be added the greater velocity of the circulating
currents which the intenser forces at work in larger spheroids will produce—a contrast made still greater by the relatively smaller retardation
by friction to which the more voluminous currents are exposed. In these causes, joined with causes previously indicated, we may recognize a
probable explanation of the otherwise anomalous fact that the Sun, though having a thousand times the mhi of jupiter, has yet reached as advanced a
stage of concentration. For the force of gravity in the Sun, which at his surface is some ten times that at the surface of Jupiter, must expose his
central<B>parts to a pressure relatively very intense; producing, during contraction, a relatively rapid genesis of heat. And it is further to</B>be
remarked that, though the circulating currents in the Sun<I>have far greater distances to travel,</I>yet since his rotation is relatively so slow that the
angular velocity of his substance is but about one-sixtieth of that of Jupiter’s substance, the resulting obstacle to circulating currents is
relatively small, and the escape of heat far less retarded. Here, too, we may note that in the co-operation of these factors, there seems a reason
for the greater concentration reached by Jupiter than by Saturn, though Saturn is the<b>elder as well as the smaller of the two;</b>for at the same time
that the gravitative force in Jupiter is more than twice as great as in Saturn, his velocity of rotation is very little greater, so that the </p>
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<p align="left">opposition of the centrifugal force to the centripetal is not much more than half. But now, not judging more than roughly of the effects of these several .</p>
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