4 
40 R. Clausius on the al pp lication of the 
= 1, has here another value, I will not enter upon the subject 
again, but will only state the final result. We find namely, 
ty = 137°-43. =: 
The equation (49) which serves to determine ¢, takes for this 
case the following form: 
(57) gg = 26604 + 51°515 log i 
a 
ig 
oF 
ico 
Det 
Pr 
Wey 
Miz, 
au 
3 
From this we obtain in succession the following approximate 
values, a 
¢ = os: 
1 “98. 
rr S101 74. 
2 pe 10176, 
The last of these values, from which the later a would only 
differ in the highest decimals, we consider as the correct value of 
ts and ap Pp'y it_ together with the known values “of t, and ¢, to 
e first of equations (xviI). Thence we have | 
W= 3108 
if we calculate the work according ti Pambour’s equation (XI1), 
attributing the same value to V, we find 
W = 82640, 
whereby however we must not take the values of Band b 
the machine without condenser from equation (290), but ‘ties 
equation (29a) determined for machines with condensers 
57. he same way, as is here indicated for the volume 1 5, 
T have also ee the work for Le volumes 1:2, 1-8, and 2° 1. 
to 
which gives the nontorng possi 
heat, if also —s ages of absorbing and giving out 
are co: 
