Friction, Lubrication and the Lubricants in HorologyLewis, W. T. (William T.)
Science
Friction, Lubrication and the Lubricants in Horology
Lewis, W. T. (William T.)
Clock and watch making; Friction; Lubrication and lubricants
3. Thrust vertically two plates of glass into water, and gradually bring
the surfaces near to each other. Soon the water rises between the
plates, and rises higher as the plates are brought nearer. If their
surfaces be mutually parallel and vertical, the water rises to the same
height at all points between the plates, as shown at A (Fig. 9.)
[Illustration: Fig. 9.]
4. If the plates be united by a hinge, and form an angle, the height to
which the water ascends increases as the _distance_ between the plates
decreases up to their line of junction, where it attains a maximum, as
shown at B (Fig. 9.)
5. Decrease the _angle_ between the plates, and the water ascends
higher, as shown at C (Fig. 9.) Thus it is seen that _the ascension
varies inversely with the angle between the plates_; i. e., the smaller
the angle, the higher the water ascends.
6. When a drop of oil is placed between two glass plates arranged as
shown at A (Fig. 10), if the surfaces are not too far distant, and if
the oil touches both surfaces, it will be seen to work its way to the
junction of the plates; showing that _oil between surfaces has a
tendency to flow towards the apex of the angle_.
[Illustration: Fig. 10.]
7. Place a drop of oil on a taper piece of metal, as shown at B (Fig.
10). The oil will gradually recede from the point to a place where there
is more metal, showing that _oil on surfaces has a tendency to flow
towards the largest part_.
[Illustration: Fig. 11.]
8. When a drop of oil is placed between two watch glasses arranged with
flat and convex sides adjacent, as at A (Fig. 11), or with convex sides
adjacent, as at B (Fig. 11), if the glasses are rigidly fixed in their
relative positions the drop of oil can be shaken from its location only
with great difficulty; the oil at C holding its place with greater
tenacity than the oil at D.
The foregoing phenomena are called _capillary action_, or _capillarity_.
Capillary action is due to the forces of cohesion (20), and to the
forces of adhesion (21.)
~23. Centrifugal Force.~--_The tendency of a body rotating round a point
to escape from that point is called centrifugal force._
Place a small quantity of oil on the arm of a balance, near the arbor.
Rotate the wheel rapidly. The oil is seen to flow towards the rim of the
wheel.
~24. Absorption of Gases by Liquids~ depends on molecular attraction and
motion. Water at a temperature of 0° cen. (32° f.), is capable of
condensing in its _pores_ (17) six hundred times its own bulk of ammonia
gas. The absorption of oxygen from the air causes some oils to become
more viscous, to eventually become solid, without losing in weight, in
fact sometimes gaining. Other oils dry up, or _evaporate_, leaving
little or no residue.
~25. Force.~--_Force is that which can produce, change or destroy motion._
Public-domain text, read in full here on John Shaqi.
Reviews
Reviews
No reviews yet
Be the first to share your thoughts on this work.
Join the Discussion
Join the discussion
Sign in to leave a comment or review.
Sign InorCreate an account