Pressure, Resistance, and Stability of Earth: American Society of Civil Engineers: Transactions, Paper No. 1174, Volume LXX, December 1910Meem, J. C.
Science
Pressure, Resistance, and Stability of Earth: American Society of Civil Engineers: Transactions, Paper No. 1174, Volume LXX, December 1910
Meem, J. C.
Civil engineering -- Periodicals; Soil mechanics
As soon as the blocking was removed the bottom settled nearly 2 in., as
noted in Fig. 1, Plate XXIV, due to the initial compacting of the sand
under the arching stresses. A measurement was taken from the bottom of
the washers to the top of the false bottom, and it was noted as 41 in.
(Fig. 1). After some three or four hours, as the arch had not been
broken, it was decided to test it under greater loading, and four men
were placed on it, four others standing on the haunches, as shown in
Fig. 2, Plate XXIV. Under this additional loading of about 600 lb. the
bottom settled 2 in. more, or nearly 4 in. in all, due to the further
compression of the sand arch. About an hour after the superimposed load
had been removed, the writer jostled the box with his foot sufficiently
to dislodge some of the exposed sand, when the arch at once collapsed
and the bottom fell to the ground.
Referring to Fig. 2, if, instead of being ordinary sand, the block
comprised within the area, _A U J V X_, had been frozen sand, there can
be no reason to suppose that it would not have sustained itself, forming
a perfect arch, with all material removed below the line, _V E J_, in
fact, the freezing process of tunneling in soft ground is based on this
well-known principle.
[Illustration: FIG. 2.]
[Illustration: FIG. 3.]
If, then, instead of removing the mass, _J E V_, it is allowed to remain
and is supported from the mass above, one must concede to this mass in
its normal state the same arching properties it would have had if
frozen, excepting, of course, that a greater thickness of key should be
allowed, to offset a greater tendency to compression in moist and dry as
against frozen sand, where both are measured in a confined area.
If, in Fig. 2, _E V J_ = [phi] = the angle of repose, and it be assumed
that _A J_, the line bisecting the angle between that of repose and the
perpendicular, measures at its intersection with the middle vertical
(_A_, Fig. 2) the height which is necessary to give a sufficient
thickness of key, it may be concluded that this sand arch will be
self-sustaining. That is, it is assumed that the arching effect is taken
up virtually within the limits of the area, _A N_{1} V E J N A_, thus
relieving the structure below of the stresses due to the weight or
thrust of any of the material above; and that the portion of the
material below _V E J_ is probably dead weight on any structure
underneath, and when sustained from below forms a natural "centering"
for the natural arch above. It is also probably true that the material
in the areas, _X N_{1} A_ and _A N U_, does not add to the arching
strength, more especially in those materials where cohesion may not be
counted on as a factor. This is borne out by the fact that, in the
experiment noted, a well-defined crack developed on the surface of the
sand at about the point _U_{1}_, and extended apparently a considerable
depth, assumed to be at _N_, where the haunch line is intersected by the
slope line from _A_.
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