The Bennington evening banner. (Bennington, Vt.) 19??-1961, 1911-08-09
A ROPE OF WATER.
BertheIOt's Test That Showed Its
Tensile Strength.
THE COHESION OF MATTER.

Perfect Planes Of Metal or Glass When
Brought into Contact viii Adhere to
One Another as Though They Were
Glued Together.
II is we'll known that liquids are
among the least compressible Of sub
stances; this in spite Of the fact that
they have the property Of conforming
to any shape Of vessel or OF yielding
to any forces, no matter how small.
which tend to change only their shape
Thus. to squeeze water into nine
tenths Of its volume under ordinary
conditions would require pressure
Of no less than 1900 atmospheres, or
$4,000 pounds, to the square inch.
This property of being almost incom-
pressible is best illustrated perhaps
by an experiment tried centuries ago,
wherein an attempt was made to com
press water by filling a leaden shell
with 1t and then, after closing, ham
mering and squeezing the shell. The
only effect of the tremendous pres
sures produced In this way was to
cause the water to penetrate the mi
mute pores of the lead and exude in
drops like perspiration on the outer
surface Of the shell. The same effect
was found for silver shell.
But, while 1t is familiar fact that
liquids will resist an enormous force Of
compression, the companion fact that
they are also capable of withstandng
tension Is not 30 generally known. At
first sight this statement may appear
ridiculous. When water may be so
readily dipped from pail or poured
from one vessel to another, how can
1t be capable of withstanding tension?
II, however, we prevent change Of
form we find that pure water is capa'
BILE of bearing fifty atmospheres Of ten
sion. or $50 pounds to the square inch
II It was possible, then. to utilize this
property by making a rope" OF water
we should find 1t capable OF sustaining
good fraction OF the weight that
could be borne by an ordinary rope OF
the same size. But 1t must be admit.
ted that the task Of making a rope out
Of such material would be rather DIFF.
6cult, to say the least. Notwithstanding
the fact that 1t possesses this desirable
property Of tensile strength. Because
OF It's inability to resist a reforming
force II would have to be inclosed In
tube; but, while It would here be In
condition to Withstand compression, as
from a piston in the tube, any attempt
at stretching the liquid In this way
would simply result In pulling away
the piston from the water surface.
However, this tensile strength was
actually found by Berthelot In the fol
lowing way: A strong glass tube sealed
at one end and drawn out very fine at
the other was filed nearly full OF wa
ter and then closed The tube was then
cautiously heated until the water had
expanded and completely filed It II
was then slowly and carefully cooled
back TO Its original temperature, when
II was found that the water had not
contracted, but still filled the tube.
1t Is almost a universal law that a
small extension In volume Of a body
requires the same magnitude Of force
to produce II as to cause similar
amount OF compression. the forces, how
ever, being tension in one case and
compression In the other. With this
law In mind II is readily seen that the
water that now fills the tube must be
under tension. since previously at the
same temperature It did not quite all
the tube-that is, II has actually been
stretched or expanded beyond Its nor
NAL volume for this temperature, and
from our knowledge Of the forces that
would be required to produce the cor
responding compression We can figure
out what this tension must be.
The ultimate particles OF molecules
Of matter we believe 10 be held to-
gether by powerful forces. known va
riously as cohesion or adhesion, but
being In any case forces Of attraction,
and these forces tend 10 prevent any
expansion OF the matter. be II solid or
liquid. II might be thought that these
forces would cause two bodies In con.
tact TO adhere 10 each other. but par.
ticles have 20 be so near together 10
DO acted upon by them that II Is diff
hcult TO bring bodies into such close
contact that an appreciate area OF
one Is within this distance Of the other
However. two clean pieces OF lead
can readily be pressed so closely TO
gether that they will adhere. and a
set OF copper cubes was once made
with such true faces that when q doz
en- OF them were piled one on top OF
the other the series adhered together
so well that the whole could be lifted
from the top one. But the best ex
ample is furnished by pieces OF op
tical glass whose surfaces have beer
worked so plane that when pressed to
gether they viii as readily break al
some other spot as at this plane.
Perhaps II Is unfortunate that these
useful forces. which hold all mattel
together and keep II from collapslnf
into impalpable dust, are confined II
their action TO such limited range
n this were not so, break OF any
sort could be fixed by merely bring
Ing together the broken ends. Glu'
Of any kind would be unnecessary.
But even this state OF Affairs woulI