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Solutions for certain rectangular slabs continuous over flexible ...

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ILLINOIS ENGINEERING EXPERIMENT STATION<br />

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

Having a Flexible Cross Beam.*-The slab and loading are shown<br />

in Fig. 11. The deflection of the slab without the cross beam is<br />

FiG. 11<br />

given by w 0 of Equation (9). The deflection due to<br />

unknown distribution on the line y = 0 is given by<br />

is to be determined from the boundary condition:<br />

a line load of<br />

(19) where a.<br />

q= E,I = V- - [ = -2N -(vi) .<br />

dX 4 L J =- L ay J =<br />

In this equation q is the downward load on the beam, E 1 and 1I are<br />

the modulus of elasticity and moment of inertia of the beam, respectively,<br />

z is the deflection of the beam given by the equation<br />

z = w] = [WO + Wi ,<br />

V( 1) is the shear due to w 1 , and E is an infinitesimally small positive<br />

distance.<br />

From the application of the boundary condition to (19), one finds<br />

(1 + av) e-<br />

an---- 4 4<br />

(43)<br />

where<br />

nrHi<br />

*Bay obtained solutions <strong>for</strong> a similar slab supporting either a uni<strong>for</strong>mly distributed load <strong>over</strong> the<br />

entire slab or a uni<strong>for</strong>m line load directly <strong>over</strong> the beam. See Hermann Bay, "Die Kreuzweise gespannten<br />

Fahrbahnplatten bei stahlernen Bricken," Beton und Eisen, 33, Heft 14, July, 1934, p. 222-224.<br />

aN

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