Isometrics of Liquid Matter. 



351 



v is nearly linear, trie gauge-reading for p = is of secondary 

 importance within the limits of the present paper. It was 

 not noted carefully. 



Table V. — Isometrics of Ether Observations. 



V 



t. 



n e . 



*V 



e. 



Np. 



p. 



Series 



No. 



Time. 



o 



7-147 

 7-132 



20-080 

 20-071 



4 V 144 

 4147 



13-177 

 13-194 



°0. 



21 : 2 

 21-3 



21*7 



21-8 



22 : 2 

 223 



22 : 3 



22-3 



o 



■ibi 



•112 



: l46t 



•155 



192 



•200 



•206 



•200 



o 



7-251 

 7-241 



20-266 

 20-226 



4-336 

 4-347 



13-377 

 13-394 



°0. 



17-8 



98-2 



98-0 



180 



218-8 



218-8 



18-1 



67-8 



68-0 



(181) 



157-8 



157-9 



17-9 



centim. 



3-80 

 29-79 

 29-86 



4-29 

 64-30 

 64-30 



5-19 

 21-14 

 21-14 

 (5-20) 

 49-04 

 49-06 



5-39 



atm. 



104 



816 



819 



118 



1761 



1761 



142 



579 



579 



(142) 



1344 



1344 



148 



XIV. 



h m 



50 



1 25 

 1 30 



1 55 



2 45 



2 50 



3 20 



4 



4 5 



5 

 5 5 

 5 30 



20-371 

 20-353 



7-212 



7-265 



4-397 

 4-415 



13-306 

 13-330 



20 : 

 200 



20 : 8 

 20-8 



210 



21-0 



21 : 2 

 21-3 



•000 

 •000 



•068* 

 •068 



•087 

 •087 



•ioi" 



•112 



20-371 

 20-353 



7-380 

 7-333 



4-484 

 4-502 



13-410 



13-442 



17-4 



220-2 



2200 



17-4 



99-1 



98-8 



17-4 



69-1 



69-4 



174 



158-0 



158-3 



17-4 



4-18 

 64-17 

 64-16 



423 

 30-83 

 30-84 



4-45 

 21-37 

 21-35 



4-43 

 48-93 

 48-98 



4-86 



114 



1758 



1758 



116 



845 



845 



122 



586 



585 



121 



1341 



1342 



133 



XV. 



52 



1 43 



1 50 



2 20 



3 

 3 5 

 3 20 

 3 50 



3 56 



4 30 



5 45 



5 50 



6 10 



The change of p during the course of a series is notice- 

 able, and it is due to the fact that the gauge, which had on a 

 former occasion been compelled to do violent work, has not 

 yet quite viscously recovered from the strain. The series 

 XV. is better than series XIV. in this respect, and- the im- 

 provement continues in all the other data, § 37. Of the two 

 values of fiducial p which comprehend any high pressure p, 

 the second is very probably correct and will be used below. 



35. An inspection of all my data shows that the tempera- 

 ture datum needs correction. The cause of discrepancy is 

 the temperature-coefficient and perhaps also the time-coefficient 

 of the magnetic system of the torsion-galvanometer. This 

 correction is easily applied, since whatever magnetic state ob- 

 tains affects the twists corresponding to all temperatures of a 

 given series, uniformly. If N ' be the twist for 100° on any 



2B2 



