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Solutions for certain rectangular slabs continuous over flexible ...

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SOLUTIONS FOR CERTAIN RECTANGULAR<br />

SLABS<br />

The deflection of the <strong>continuous</strong> edge beam is<br />

1 4pa 4 1 Qa 2 1<br />

z=w ] = 4 -- d 3 sin ax- --<br />

Jy=b 5 N .s,,.- n T- ,N,.- n 3 f 7 sin avsin ax. (179)<br />

One finds, <strong>for</strong> zero deflection at the interior supports, that the<br />

concentrated reactions are given by the equation<br />

1<br />

4a --<br />

d3 sin av<br />

Q 1= f4s-n (180)<br />

7r 2 1f7 sin2 av<br />

3<br />

1 n2,3,<br />

The functions b 3 , cs, d 3 , f2, f4 and f7 are given in Appendix B.<br />

31. Rectangular Slab Having Two Opposite Edges Simply Supported<br />

and Two Edges Supported on Beams Which Are Continuous<br />

Over Interior Supports at the Third-Points; Concentrated Load on the<br />

Longitudinal Center Line.-The slab is shown in Fig. 32 where each<br />

/ Con'/nuoous F/exib/e Beam E42<br />

- -<br />

X--<br />

£2<br />

FIG. 32<br />

of the interior reactions at x = a/3 is represented as having a magnitude<br />

of (Q1 + Q 2 )/2 and the remaining interior reactions are each<br />

represented as having a magnitude of (Q1 - Q2)/2. From (109)<br />

and (113) one obtains a deflection function <strong>for</strong> b > y > 0:

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