AND ITS APPLICATION TO MIL B. TOWER’S EXPERIMENTS. 
225 
Table IV.—Olive Oil, Brass No. 1 —continued. 
X. 
100 
150 
200 
250 
300 
350 
400 
450 
T„, Fahr. 
3-45 
5-83 
8-13 
10-02 
11-77 
13-26 
14-46 
1537 
'S' 
•464 
•526 
•588 
•650 
•684 
•742 
•835 
(//) 
(•370) 
A’ 765 
•805 
•S45 
J\ 
•249 
•336 
•404 
■464 
•517 
•582 
•610 
•660 
U 
= 310 - 
c 
a 
•510 
•00138 
■392 
•(.0144 
•337 
•00151 
•305 
•00158 
•2X4 
•00161 
•266 
■00166 
•254 
•00172 
•234 
•00172 
<P\ 
- 7° 0 ' 0 " 
• . 
.. 
.. 
•. 
• . 
l 
-42° 0' 0" 
•• 
•• 
•• 
•• 
r f 
•361 
•436 
•514 
•592 
•644 
•669 
•747 
•789 
f-2 
. . 
•62 
•670 
■712 
•760 
■810 
Jl 
•266 
■358 
•431 
•495 
•550 
•600 
■650 
•707 
L 
= 253 
c 
a 
<Pi 
L 
•377 
•00128 
•287 
•00135 
•242 
•00141 
•224 
•00148 
•200 
•00151 
•195 
•00156 
•180 
•00159 
•171 
•00161 
•• 
.. 
•• 
•• 
•• 
•• 
r r 
•368 
•430 
•512 
•572 
•613 
•675 
•736 
•818 
ji 
•380 
•457 
•530 
•595 
•65 
•701 
•755 
•810 
a' 
•285 
•385 
•464 
•534 
•592 
•646 
•700 
■755 
L' 
= 205 < 
c 
a 
•255 
•00119 
•195 
•00126 
'1 (55 
*00131 
•152 
•00138 
•141 
•00240 
•132 
•00145 
•126 
•00148 
•118 
•00135 
<p\ 
.. 
. . 
-1° 13' 0" 
-1° 5' 0" 
. 7T 
L 
•• 
•• 
• • 
•• 
•• 
— 60° 0 ' 0 " 
- 62° 0 ' 0 " 
rr 
•351 
•458 
•535 
•611 
•672 
■718 
•764 
•871 
ft 
•352 
458 
■530 
■ 6 <'l 
•665 
•717 
•778 
•840 
J\ 
•307 
•414 
•498 
*574 
•628 
•695 
•753 
•813 
L' 
= 152 - 
c 
a 
•165 
•00111 
•126 
•00116 
•107 
•00122 
•098 
•00128 
•089 
•00130 
■086 
•00134 
•082 
•00137 
•075 
•00139 
<P\ 
’ • 
-1° 13' 0" 
-1° 0' 0" 
-0° 57'0" 
-0° 50' 0" 
-0° 44'0" 
-0° 38'0" 
-0° 31'0" 
, 7T 
L h ~2 
— 61°0' 0 " 
— 65° 0' 0" 
— 27° 20' 0" 
— 69° 0' 0" 
— 69° 40' 0" 
— 70°20'0" 
— 72° 0' 0" 
f 
■360 
•450 
•550 
•630 
•690 
•770 
•820 
•890 
J-2 
•352 
■465 
•555 
•637 
•70S 
•770 
•8 41 
•897 
fx 
•336 
•463 
•546 
•628 
■697 
•760 
•823 
•890 
L' 
= 100 « 
c 
a 
■090 
•00101 
•0691 
•00106 
•0600 
•00112 
•0541 
•00116 
•0492 
•00120 
*0 i 71 
■00123 
■0460 
•001 25 
•0420 
•00127 
<h 
-0° 43' 0" 
- 0 ° 26'0" 
-0° 17'u" 
-0° 10'0" 
-0° 4' 0" 
-0° 2'30" 
-0° 0' 0" 
+ 0° 5' 0" 
$ o ~2 
— 68 ° 30' 0" 
- 73° 20' 0" 
— 75°20'0" 
— 76°30'0" 
- 77° 20' 0" 
— 77° 40' 0" 
- 0 ° 78' 0" 
— 78" 40' 0" 
As compared with the experimental values f given in the Table IV., it is seen 
that the agreement holds as long as c is less than ‘06, after which, as c increases, the 
values of become too small, or while the values of continue to diminish as the 
load and a increase, the experimental values of f after diminishing till c is about 
‘I or T5 begin to increase again. In oi'der to see how far this law of variation was 
explained by the theory, it was necessary to find the values of f to a second 
approximation, and before this to obtain the values of c. 
Putting, as in equation (12 4), 
MDCCCLXXXVL 
L=4’84 L' 
2 G 
