( *8 ) 
whereas for v = b -f- (*>— b) — (b 1 -J- pLb) -f- 
@, = 1, — A6 = V.): 
. (c) 
which for values of 0 in the neighbourhood of 1 passes into v = 1 /* + “> 
So we calculated the following values for p,v, and p for T= 9. 
To gain a better survey of the course of the values mentioned, some 
more values of <p have been inserted in the table. 
We notice that for all the values of T, when viz. A b is negative, 
i.e. positive , p has a minimum value at tp = 1. The amount of 
this minimum value will, of course, depend on the temperature. 
Thus pnin = 1,5.10- 38 or practically =0 at T= 9. (For v — b — 0, 
P ~~ Q®, P i 8 always == 1, when Lb is negative, while for v .= oo, 
p = 0, p is also = 1). 
When <p = 1, v is evidently =1’/, according to (c). In general 
v will be determined by v = b, — Lb for u> — 1. (Comp, also 
p. 771 of I). 
It is self-evident that for the accurate calculation of p, v and p 
more figures have been reckoned with than are indicated here. The 
values of p and v have mostly been shortened to 2 figures, whereas 
those of p have been indicated in 2 or 3 figures. So between <p = 187 
and ip = 0,25 the values of p have been reduced to round numbers 
to tens of units. 
With regard to the different maxima and minima e.g. for 9> 
we observe once more, that in the equation: 
r „ (l+flflr fl _ T_ ^ _ a 
in which a decrease of <p is always attended with an increase of 
V " prep are p first decreases rapidly from oo to — 3840, when 
>) For from r = 6, _ (_Ah) ^ M]om . 
