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Solutions for certain rectangular slabs continuous over flexible ...

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SOLUTIONS FOR CERTAIN RECTANGULAR<br />

SLABS<br />

Equations (29) are of particular interest under the load, where<br />

they become<br />

v-v<br />

7-<br />

(1+/,)P A' Pv 1 1 inh 2rv<br />

---- logeB----4 --- )sinh-a<br />

87T B' 4a B' A' a<br />

sinh 2 -<br />

±rv(1 -p)<br />

a<br />

S2a A' '<br />

S(1+,)P A' Pv 1 1 F 27rv<br />

M) = -(<br />

;<br />

)loge-; - ( -- p sinh-<br />

SJ o87 e B' 4a B' A' a<br />

V=v<br />

-(30)<br />

rv(1 -- )<br />

2a<br />

sinh 2 -<br />

a<br />

A'<br />

Mwhe<br />

27ru<br />

sin --<br />

(1 -, )Pv a<br />

U8a<br />

A<br />

Trv<br />

a<br />

27 v<br />

sinh ---<br />

a<br />

A'<br />

where<br />

2rv 27ru<br />

A' = cosh --- cos -,<br />

a a<br />

2irv<br />

B' = cosh --- 1. (31)<br />

a<br />

Equations (30) give corrective moments under the load which are<br />

to be added to the corresponding moments in the infinitely long slab<br />

without a cross beam, as given by Equations (18), in order to obtain<br />

the resultant moments under the load. Numerical values of corrective<br />

bending moments computed from (30) are given and discussed<br />

in Section 8.

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