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Solutions for certain rectangular slabs continuous over flexible ...

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48 ILLINOIS ENGINEERING EXPERIMENT STATION<br />

where A 1 and Bi are given by (25). From (4) and (78)<br />

1 + - P B 1<br />

M1 = - M' = log, . (79)<br />

3 + A 27r A 1<br />

Again, previous results may be used to determine M" and M", since<br />

(79) represents the moment sum, (M, + M,), in the infinitely long<br />

slab due to a load of 2P/(3 + p) at the point x = u, y = -v.<br />

The third part of the correction, w'", may be written at once in<br />

finite <strong>for</strong>m, since it differs from (66) only by a constant multiplier.<br />

Thus<br />

1 - p' Pvy B,<br />

w'" = loge -- (80)<br />

3 + u 4rN A 1<br />

Moments may be obtained in finite <strong>for</strong>m from (80) by differentiation.<br />

The corrective bending moments due to w 2 , obtained as the sum<br />

of the effects of w', w" and w"', may be summarized as follows:<br />

(1 + ) (5 - p) P B 1<br />

M(2) = - -log,--<br />

(3 + IA) 81r A,<br />

1- P ,1 1 r(y+v)<br />

•<br />

+- - [(1+3)v+(1- )y](--) sinh<br />

3+A 8a B5i A-) a<br />

Scos 7(v + y) 7r(x - u)<br />

cosh cos - 1 '(81)<br />

(1 - Prvy L)2 a a<br />

3 + ± 4a 2 Bi<br />

c r (v + y) "(x+ u)<br />

cosh cos - 1<br />

a<br />

a

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