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Solutions for certain rectangular slabs continuous over flexible ...

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SOLUTIONS FOR CERTAIN RECTANGULAR<br />

SLABS<br />

Certain other properties of sgn y are important, namely,<br />

and<br />

sgn 2 y - 1<br />

sgn (-y) = -sgn y.<br />

In the analysis of <strong>slabs</strong> the relationship "y sgn y" frequently<br />

occurs. While this can always be represented by the symbol lyl,<br />

there is no provision in the latter representation <strong>for</strong> taking the derivative.<br />

It is sufficient, however, to write<br />

\y\ = y sgn y<br />

from which one obtains<br />

d d<br />

y-- \y - (y sgn y) = sgn y.<br />

dy dy<br />

A movement of the origin which results from the substitution of<br />

(y - v) <strong>for</strong> y, where v is a constant, has the effect, of course, of shifting<br />

the sign change from the line y = 0 to the line y = v.<br />

In a number of the problems in the text use is made of the relationships<br />

just given. For example, in Equation (9) there appears a<br />

function of y, namely,<br />

which may be written in the <strong>for</strong>m<br />

f(y) = (1 + aIy-v|) e-" i -<br />

f(y) = [1 + a (y - v) sgn (y - v)] e-" ( -<br />

)<br />

-* (y-'.<br />

Derivatives of this function with respect to y, when a and v are constants,<br />

are<br />

df<br />

= -a 2 (y - v) [sgn 2 (y - v)] e-"a(y - ) sgn (y-v)<br />

dy<br />

2 "<br />

= -a (y - v) e- -l,<br />

v<br />

d(f= -a [1 - a (y - v) sgn (y - v)] e-<br />

dy 2 = -a 2 (1 - ay-v) e-<br />

1 -<br />

a ,<br />

Y -)<br />

sgn (Y-v)

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