21.01.2014 Views

Solutions for certain rectangular slabs continuous over flexible ...

Solutions for certain rectangular slabs continuous over flexible ...

Solutions for certain rectangular slabs continuous over flexible ...

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

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)

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!