357
325-328] The Spiral Arms
Actually this formula can only be valid up to about e = 0’6, all higher
values being represented by the spiral nebulae. The fact that the spirals far out
number the elliptical nebulae shews that k must be quite small, so that up to
e = 0-6 the effect of the factor e~ kt is probably inappreciable. If we neglect
the factor e -*• altogether, the law of distribution reduces to e^de. The. following
table shews the numbers of actually observed nebulae as given by Hubble
after allowing for foreshortening on the supposition that the nebulae are
oriented at random in space, together with a calculated distribution which
obeys the law e^de.
Ellipticity
Observed
(Hubble)
Calc.
0 to 0-05
99
1-27
0 05 to 0’15
5-6
5-3
0-15 to 0-25
7-6
7-6
0 25 to 0 35
9-3
9-2
0 35 to 0'45
100
10-7
0'45 to 0’55
12-1
12-1
0-55 to 0-65
10-8
13-2
0'65 to 0-75
21-7
14-2
There is good enough agreement except at the two ends of the curve. The
large observed preponderance of nearly spherical nebulae may arise from the
outer layers rotating less rapidly than the inner layers, and so not having the
elongation appropriate to the angular momentum of the nebula, while the
less marked excess of nebulae of high ellipticity could be easily explained in
the not improbable event of a few Sa nebulae having been classified as E 7.
The Spiral Arms.
328. Laplace, discussing the sequence of configurations assumed by his
rotating nebula, supposed that it had a universe to itself, and so was acted
on by no forces beyond its own gravitation. In this case symmetry required
that the matter shed in the equatorial plane should form perfect circles.
An actual nebula must be acted on by tidal forces arising from the general
gravitational field of the universe as well as from other nebulae. When first
it assumes the lenticular form, the forces of gravitation and centrifugal force
do not suddenly become equal at all points of the equator simultaneously.
Two opposite points of the equator will be distinguished from the others as
the points at which the tidal forces give the greatest height of tide, and the
ejection of matter will first commence at these two points. The two points
are points fixed in space, determined by the tidal field in space, and not
points rotating with the nebula, although of course their position may gradually
change as the gravitational forces of the ejected matter modify the general
tidal field.