Solutions for certain rectangular slabs continuous over flexible ...
Solutions for certain rectangular slabs continuous over flexible ...
Solutions for certain rectangular slabs continuous over flexible ...
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ILLINOIS ENGINEERING EXPERIMENT STATION<br />
bi = (fi - 1) cosh av - (fj - 1) av sinh av, (99)<br />
2 (1 - ,)2<br />
c1 = (fa - 1) cosh av - av sinh av. (100)<br />
A<br />
The quantities fl, fa and A are independent of the position of the load<br />
and are listed in Appendix B.<br />
The deflection of each of the edge beams is found to be<br />
1 Pa 2 1<br />
z = Ws = -- f5 sin au sin ax, (101)<br />
3<br />
Sy b 7 N 1,2,3, -<br />
where the quantity f5 is given in Appendix B.<br />
in the edge beam is then<br />
The bending moment<br />
PaH 2 1<br />
Mbeam -- -f5 sin au sin ax. (102)<br />
7• 1,2,3,a" n<br />
As the pair of loads traverses the span, a, the moment in the edge<br />
beam varies until it becomes a maximum at x = a/2 when u = a/2.<br />
The value of this maximum moment is<br />
PaH 2 f5<br />
max. Mbeam = - - (103)<br />
The curvatures due to w' are<br />
a 2 w' P 1<br />
-x- --- E -(b 1 cosh ay-c 1 ay sinh ay) sin au<br />
' 1<br />
sin ax,<br />
,rN ,23,•.. n<br />
ay 2<br />
'9w' P 1<br />
=-- -[(b- 2c 1 ) cosh ay-ci ay sinh ay] sin ausin ax.<br />
7rNw• .. n<br />
(104)<br />
At y = 0 these become<br />
0 2 w' - P 1.*<br />
- = -- - bi sin au sin ax,<br />
Ox2 Y=0 7rN . n<br />
0 2 w' 1<br />
2W - P - (bi - 2cj) sin au sin ax.<br />
y 2 J =0 rN u1,2,3,'- n<br />
(105)