[M2.18backL] [M2.18back] 18
[diagrams] increased when they become large; The reader will at once
understand this differentiation of strength in the masses,
by considering that a small stone may project from over a
wall as at a 1 opposite, without smallest chance of the portions
a a breaking off. but a great rock cannot overhang in
the same proportion, as at 2,without considerable danger
of portions of the overhanging mass giving way: much
more if superincumbent weight be added; whose pressure
shall be confined to the overhanging portion; Now not only does this
principle applies directly to the capitals of shafts, even
when they are considered as crowning masses without any
superimposed weight, so that for instance the capital b of
the shaft 3, might with perfect safety project ½ a foot
if the shaft were only a foot in diameter and five feet
high but might not with safety project six feet from a
shaft 12 feet in diameter and sixty feet high; But the
diminution of security is, in [?] still greater, when the increase of superincum
-bent weight is considered, and not
only its increase; but its less perfect diffusion;
for when the capital is small, in all probability the
weights will be laid on it as at c or c2 and the lines of
pressure thrown through it to the shaft, but if the
capital be very large the weight will in all probability
be thrown on it as at d, or d2, and some of the
lines of resistance
[Version 0.05: May 2008]