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Solutions for certain rectangular slabs continuous over flexible ...

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SOLUTIONS FOR CERTAIN RECTANGULAR<br />

SLABS<br />

10. The Infinitely Long Slab Supporting a Concentrated Load Midway<br />

Between Two Flexible Cross Beams.-Because of symmetry about<br />

the x axis as shown in Fig. 12, it is sufficient to obtain the deflection<br />

Fia. 12<br />

functions <strong>for</strong> y > 0. Letting wi and w 2 represent the total deflection<br />

of the slab <strong>for</strong> b/2 > y > 0 and <strong>for</strong> y > b/2 respectively, one may<br />

write<br />

Pa 2 1<br />

wo -- (1 + ay) e - " sin au sin a«x,<br />

27rN ..... n<br />

(47)<br />

Pa 2 k ab\ a b<br />

wl= wo-- - 1+ -)cosh ay - ay sinh ay e<br />

T sin au sin ax (48)<br />

rN,,.,... n3LR 2 /<br />

and<br />

Pa 2 k ab ab ab sinsin(49)<br />

w2=w- - E - (1+ay) cosh---sinh- e-sin ausin ax(49)<br />

rN 1.,.... n' 2 2 2 ]<br />

where k is to be determined from the boundary condition. In Equations<br />

(48) and (49) the correction to w 0 has been expressed as the sum<br />

of the deflections of the infinitely long slab,<br />

and<br />

Pa 2 k<br />

w' = - 2 -- (1 + aly - b/21)e-aly-b/21 sin au sin ax (50)<br />

27rN ,.,,... n'<br />

Pa 2 k<br />

w" = - - (1 + aly + b/2)e-aly+b/2' sin au sin ax, (51)<br />

2r3N 1.,.3... nf

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