Published online by Cambridge University Press: 24 October 2008
The derivation given by Hoyle and Lyttleton for an accretion formula proposed by them is examined. A number of arguments against its validity are put forward, especially that on the one hand their capture radius depends on the theorem that if the velocity of certain masses of gas after collision is less than the velocity of escape at the point, they will not in fact escape, while on the other hand it is clear (and is now admitted) that the gas cannot in fact move with this velocity at all. It is also shown that since, ex hypothesi, the individual molecules will all, on the average, retain their hyperbolic velocities, there is not the compelling reason for their capture that there appeared to be in Hoyle and Lyttleton's argument, where only the mean radial velocity of the centre of gravity of the mass was considered. Further, it seems improbable that the temperature of the interstellar matter can be low enough for the initial assumptions of their theory to hold.
* Proc. Cambridge Phil. Soc. 35 (1939), 405 and 592.Google Scholar
† The question forms part of a wider discussion appearing in the Mon. Not. R. Astr. Soc. 100 (May, 1940).Google Scholar
* Loc. cit. p. 409.
† Loc. cit. P. 597.
* Loc. cit. p. 411.
* Ant (x) (i.e. “antilogarithm of x”) is written here for 10x, in the same way as exp (x) is commonly written for e x. The notation was first proposed in Astrophysical J. 73 (1931), 292Google Scholar (see also Nature, 124 (1929), 94).Google Scholar
† Hoyle and Lyttleton, loc. cit. p. 412 or p. 598.
* Loc. cit. p. 598.
† These figures should be roughly halved if we assume that the hydrogen is all ionized. However, they should also be approximately doubled if there is, as there well may be, one Ca+ atom to every 40 of hydrogen.
* Loc. cit. p. 599.
* Internal constitution of the stars, p. 377.