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Solutions for certain rectangular slabs continuous over flexible ...

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SOLUTIONS FOR CERTAIN RECTANGULAR<br />

SLABS<br />

Re = concentrated reaction at corner, as shown in Fig. 1<br />

or,, o- = normal components of stress, in directions of x and y<br />

respectively<br />

Txv = shearing component of stress, in plane normal to x and<br />

in direction of y, or in plane normal to y and in direction<br />

of x<br />

n = an integer. A particular summation is to be carried out<br />

<strong>for</strong> the integral values indicated under the summation<br />

sign<br />

n7r<br />

a =<br />

a<br />

nirb<br />

3 = ab = -<br />

a<br />

= an infinitesimally small positive quantity or distance<br />

)2 a 2<br />

V 2 - + - , Laplace's operator in two variables<br />

X2 a9-y 2<br />

Various other quantities are defined in the text where they are<br />

used or in Appendix B.<br />

II. REVIEW OF FUNDAMENTAL EQUATIONS<br />

4. The Ordinary Theory of Slabs.-The equations pertaining to the<br />

ordinary theory of flexure of <strong>slabs</strong> will not be derived here since their<br />

derivation is available in a number of places* in the technical literature.<br />

It should be stated, however, that the ordinary theory is based<br />

upon the assumption that every line drawn through the slab normal<br />

to its middle surface be<strong>for</strong>e the slab is loaded remains straight and<br />

normal to the deflected middle surface after the slab is loaded. The<br />

theoretical results obtained under this assumption are applicable to<br />

bridge <strong>slabs</strong> except in the vicinity of a concentrated load.<br />

NAdait found the maximum stress under a loaded circular area<br />

by a special theory applicable to a thick circular slab and Westergaardt<br />

converted NAdai's results into expressions like those from the<br />

ordinary theory by the use of an "equivalent diameter" of a uni<strong>for</strong>mly<br />

loaded circular area. These results are valid when the load is sufficiently<br />

remote from a support, as it must be to produce maximum<br />

*See, <strong>for</strong> example: A. Nadai, Die elastischen Platten, 1925, p. 20; H. M. Westergaard and W. A.<br />

Slater, Moments and Stresses in Slabs, Proc. Am. Cone. Inst., V. 17, 1921, p. 415; H. M. Westergaard,<br />

Computation of Stresses in Bridge Slabs Due to Wheel Loads, Public Roads, V. 11, No. 1, March,<br />

1930, p. 2.<br />

tA. Nadai, Die elastischen Platten, 1925, p. 308.<br />

$H. M. Westergaard, Stresses in Concrete Pavements Computed by Theoretical Analysis, Public<br />

Roads, V. 7, No. 2, April, 1926, p. 25.

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