hole has a like failing, which is often the case, it 
is very evident that this want of truth in both the pivot and hole is very 
detrimental to the good going of a watch. 
[Illustration: Fig. 4.] 
[Illustration: Fig. 5.] 
There are two kinds of pivots, known respectively as straight and 
conical pivots, but for the balance staff there is but one kind and that is 
the conical, which is illustrated in Fig. 4. The conical pivot has at least 
one advantage over the straight one, i. e., it can be made much smaller 
than a straight pivot, as it is much stronger in proportion, owing to its 
shape. All pivots have a tendency to draw the oil away from the jewels, 
and particularly the conically formed variety, which develops a strong 
capillary attraction. To prevent this capillary attraction of the oil, the 
back-slope is formed next to the shoulder, although many persons seem 
to think that this back-slope is merely added by way of ornament, to 
make the pivot more graceful in appearance. It is very essential, 
however, for if too much oil is applied the staff would certainly draw it 
away if its thickness were not reduced, by means of the back-slope. 
Before leaving the subject of capillarity let us examine the enlarged 
jewel in Fig. 5; c is an enlarged pivot, b is the hole jewel and a is the 
end stone. We observe that the hole jewel on the side towards the end
stone is convex. It is so made that through capillarity the oil is retained 
at the end of the pivot where it is most wanted. It is, in my opinion, 
very necessary that the young watchmaker should have at least a fair 
understanding of capillarity, and should understand why the end stone 
is made convex and the pivot with a back slope. For this reason I will 
try and make clear this point before proceeding further. We all know 
that it is essential to apply oil to all surfaces coming in contact, in order 
to reduce the friction as much as possible, and if the application of oil 
is necessary to any part of the mechanism of a watch, that part is the 
pivot. Saunier very aptly puts it thus: "A liquid is subject to the action 
of three forces: gravity, adhesion (the mutual attraction between the 
liquid and the substance of the vessel containing it), and cohesion (the 
attractive force existing among the molecules of the liquid and 
opposing the subdivision of the mass.)" 
We all know that if we place a small drop of oil upon a piece of flat 
glass or steel and then invert the same the oil will cling to the glass, 
owing to the adhesion of the particles; if we then add a little more to 
the drop and again invert, it will still cling, although the drop may be 
elongated to a certain degree. This is owing to the cohesion of the 
molecules of the oil, which refuse to be separated from one another. If, 
however, we again add to the drop of oil and invert the plate the drop 
will elongate and finally part, one portion dropping while the other 
portion clings to the main body of the liquid. The fall of the drop is 
occasioned by gravity overcoming the cohesion of the molecules. Now 
take a perfectly clean and polished needle and place a drop of oil upon 
its point and we will see that the oil very rapidly ascends towards the 
thicker portion of the needle. Now if we heat and hammer out the point 
of the needle into the form of a small drill and repeat the operation we 
find that the oil no longer ascends. It rises from the point to the extreme 
width of the drill portion, but refuses to go beyond. It clings to that 
portion of the needle which would correspond to the ridge just back of 
the slope in a conical pivot. Water, oil, etc., when placed in a clean 
wine glass, do not exhibit a perfectly level surface, but raise at the 
edges as shown at a in Fig. 6. If a tube is now inserted, we find that the 
liquid not only rises around the outside of the tube and the edges of the 
vessel, but also rises in the tube far beyond its mean level, as shown at
b. These various effects are caused by one of the forces above 
described, i. e., the adhesion, or mutual attraction existing between the 
liquid and the substance of the vessel and rod. The word capillarity is 
of Latin derivation, and signifies hair-like slenderness. The smaller the 
tube, or the nearer the edges of a vessel are brought together, the higher 
in proportion will the liquid rise above    
    
		
	
	
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