38 R. Clausius on the Application of the 
= 133°01 ie 
t” = 134 43 d 
v” = 134 +32 3 
t'’” = 138 +38 
Still further Screen would differ only in the higher deci- : 
mal places, and we have accordingly, inasmuch as we will con- 
tent ourselves with two decimals, to consider the last number as 
the true value of ¢,. The pressure belonging to this is 
P.= 2308°30. 
If we apply these values of V and p2, at the same time with the 
other values closely determined in § 51, to the first. of equations 1 
(XVIII) we obtain 
W =11960. 
piserapl S equation (x11) gives for the same vital 0° 6, the 
work 
W= 12520. 
64. In order to show still more distinctly the dependence of 
the work upon the volume, and at the same time, the difference 
which prevails in this respect between Pambour’s and my theory, | 
T have executed the same calculation as for the volume 0°6 for a | 
series of volumes increasing at equal distances. The results are 
comprised in the following table. ‘The first horizontal series of | 
numbers, which is separated from the others by a line, contains | 
the values found for a machine without injurious space. For 
the rest the arrangement of the table is-easily understood. 
Vv te w ee 
Vv 
0°3637 52°:22 14990 03883 16000 
0°3690 52 22 14450 0:3883 15200 
4 49 °12 14100 15050 
40 *83 13020 06 13780 
06 84 °33 11960 0:6 12520 
0-7 29 -03 10910 0-7 11250 
0-8 124 ‘55 08 9980 
0-9 T2017 8860 09 8710 
1 117 ‘36 ] 4440 
bour’s pc in the expansion which takes . place singe Pu the 
— the oo ways remains in the form of saath 
‘was so in the beginning; according to our theory, on t 
— apart of the: mass whieh earried along in the fluid 
