24.08.2013 Views

1 - Erich Schmid Institute

1 - Erich Schmid Institute

1 - Erich Schmid Institute

SHOW MORE
SHOW LESS

Create successful ePaper yourself

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

A.4 Calculation Procedure and Results<br />

The actual stress distributions σi−1 and σi−1,i are depicted in Fig.A.7(f). The total<br />

stress distribution in the actual straightened system σi is calculated by adding σi−1 and<br />

σi−1,i. The resulting stress profile as well as the moment that compensates for σi and<br />

straightens the system Mi,s = −Mi are depicted schematically for i = 2 in Fig.A.7(g).<br />

The calculation procedure is repeated until all sublayers are superimposed and the cantilever<br />

has attained its original thickness. The resulting stress profile in the straightened<br />

original cantilever is shown in Fig.A.8.<br />

Figure A.8: Stress profile in the straightened cantilever as a function of the cantilever thickness.<br />

A.4.4 Determination of the Stress Distribution in the Initial System<br />

The stress profiles in the initial system and the straightened cantilever are different,<br />

but they can be converted into each other. The stress profile in the initial system is<br />

calculated from the stress distribution and the thickness of the straightened cantilever<br />

and the substrate thickness of the initial system.<br />

First, the straightened cantilever is considered (Fig.A.9(a)). Then the eight sublayers<br />

and the substrate are separated (Fig.A.9(b)), and the bending moment that straightens<br />

the system M8,s is substituted by nine external forces F [i], with 0 < i < 8, calculated from<br />

the thicknesses t [i] and the stresses in the single sublayers of the straightened cantilever<br />

σ [i,sc] (Eq. (A.9):<br />

F [i] = σ [i],sct [i]<br />

(A.9)<br />

These balanced forces serve two purposes. They ensure that the lengths of the separated<br />

parts are the same as in the straightened cantilever lsc, and induce the same stress<br />

distribution as the moment M8,s.<br />

Now the external forces are removed and the sublayers as well as the substrate extend<br />

or contract until they are stress free (Fig.A.9(c)). The lengths of the separated parts<br />

l [i],stressfree depend on the length of the straightened cantilever, the biaxial Young’s<br />

moduli and the magnitude of the removed external forces or stresses, respectively (Eq.<br />

(A.10)):<br />

A–11<br />

A

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

Saved successfully!

Ooh no, something went wrong!