Earthwork Slips and Subsidences upon Public Works: Their Causes, Prevention, and ReparationNewman, John
Science
Earthwork Slips and Subsidences upon Public Works: Their Causes, Prevention, and Reparation
Newman, John
Earthwork
A covering of stone pitching may be necessary, but in unsubmerged work
it has some disadvantages for, having joints, it allows unequal
penetration of water through them and impedes the equal discharge of
water from the earth, although its weight is a recommendation as it
opposes and may balance a pressure of water behind the slope. However,
unless it is bedded upon a layer of soil of equal permeability, such as
gravel laid upon a nearly impermeable bed of clay, which should always
be mixed with sand to prevent it fissuring and bursting by heat or
water, so as to convey the water that has percolated and also that which
exudes through the slope; it may cause a localization of the flow, and,
except in peculiar cases and provided the slopes are covered, there is
no occasion for pitching if merely used to prevent slips and not
erosion, as obviously weight and a secure protection may be obtained by
other means and at less expense. For the protection of the slopes of
rivers or canals or submerged work the case is different, as then
pitching prevents erosion and may be the only secure preservative in
exposed situations, although generally the most expensive. The pitching
should rest upon a bed of permeable material, and this layer should have
a power of suction and distribution more than equal to the quantity of
water that may penetrate the joints of the pitching; there should be a
bed of impermeable material next to the soil, and in exceptional cases
even two to carry off any water that has percolated, so as to obviate
any lodgment of water, due provision being made for the land drainage
discharge.
Sir James Brunlees, Past-President Inst. C.E., found by experiment that
at a slope of 2 to 1 pitching has the greatest resistance to extraction,
_i.e._, it requires a greater effort to extract a brick at that slope.
Taking the slope of 2 to 1 as unity, the relative resistances were found
to be as follows:—
1 to 1 slope 0·71
2 to 1 slope 1·00
3 to 1 slope 0·97
4 to 1 slope 0·66
The resistances at 2 to 1 and 3 to 1 are practically the same.
Public-domain text, read in full here on John Shaqi.
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