Solutions for certain rectangular slabs continuous over flexible ...
Solutions for certain rectangular slabs continuous over flexible ...
Solutions for certain rectangular slabs continuous over flexible ...
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ILLINOIS ENGINEERING EXPERIMENT STATION<br />
20. Concentrated Loads on the Slab Giving a Slab Deflection Which<br />
Is Anti-symmetrical With Respect to the Longitudinal Center Line.-<br />
The slab is shown in Fig. 22. The part of the slab in the region of<br />
positive y behaves as if it were a <strong>rectangular</strong> slab of width b and<br />
length a, simply supported on the three edges x = 0, x = a, y = 0,<br />
supported by an edge beam at y = b, and loaded by a single cona'7<br />
FIG. 22<br />
centrated load P at the point x = u, y = v. For the slab as shown<br />
in Fig. 22 the presence of a supporting beam along the line y = 0<br />
has no effect upon the solution since there is no deflection along<br />
that line.<br />
One may divide the slab into regions and express the deflection<br />
of the slab in these regions by the equations<br />
w1 = w' + w' <strong>for</strong> v > y > -v (117)<br />
and<br />
w2 = w' + w' <strong>for</strong> b > y > v. (118)<br />
In these equations w' and wu' are deflections of the infinitely long slab<br />
of span a due to the pair of anti-symmetrical loads shown in Fig. 22,<br />
and w' is the deflection due to corrections applied at the edges y = ± b.<br />
Thus:<br />
, Pa 2 1<br />
0 -- [( 1 + a v ) sinh ay -ay cosh ay] e - " v sin au sin ax,(119)<br />
7"/¥ 1,2,3,.. n,<br />
Pal 1<br />
w = --- - [(1+ay) sinh av - av cosh av] e-<br />
iv ,2..... n<br />
Y<br />
sin au sin ax, (120)<br />
Pa 2 1<br />
w -N<br />
2<br />
-1 (a sinh ay+di cay cosh acy) sin au sin ax. (121)