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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)

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