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Solutions for certain rectangular slabs continuous over flexible ...

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SOLUTIONS FOR CERTAIN RECTANGULAR<br />

SLABS<br />

in which<br />

2 (V 0.4c 2 + h 2 - 0.675h) <strong>for</strong> c < 3.45h<br />

c <strong>for</strong> c > 3.45h<br />

where<br />

c = diameter of a small circular area assumed to be uni<strong>for</strong>mly<br />

loaded,<br />

h = thickness of slab.<br />

In much of the work that follows, the results are presented in the<br />

<strong>for</strong>m of corrections to be added to the corresponding basic quantities<br />

given in the <strong>for</strong>egoing.<br />

III. THE INFINITELY LONG SLAB WITH SIMPLY SUPPORTED EDGES<br />

6. Concentrated Load at Any Point on the Infinitely Long Slab<br />

Having a Rigid Cross Beam.-Figure 3 shows the slab and the orienta-<br />

FIG. 3<br />

tion of the axes relative to the cross beam and the load. Without<br />

the cross beam, the deflection of the slab is given by w 0 of Equation<br />

(9). The deflection due to a line load of unknown distribution upon<br />

the line y = 0 is given by the equation<br />

Pa 2 an<br />

i = 2- 1 -3,. (1 + a-y\) e-"0 sin au sin a x<br />

wl 2drN i.e.3.. n 3<br />

where the load distribution factor a. is to be determined by the<br />

boundary condition at y = 0. The total deflection is then<br />

W = W 0 +<br />

Wi.

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