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1 - Erich Schmid Institute

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E<br />

E Mechanics of Residually Stressed Coated Systems<br />

Figure E.2: Introduced sign convention: The end where the x-axis leaves the cut system (in this case<br />

the right end) is defined as positive. The end where the x-axis enters the system is defined<br />

as negative. A negative bending moment on the positive end creates a negative curvature<br />

(bending radius respectively), a positive bending moment on the positive end creates a<br />

positive curvature. A positive bending moment on the negative end creates a negative<br />

curvature, a negative bending moment on the negative end creates a positive curvature<br />

With<br />

ɛ = ∆l<br />

l<br />

(E.3)<br />

the strain as a function of the curvature and the distance from the neutral plane is<br />

calculated:<br />

ɛ = pɛ − p<br />

p<br />

= 2 (ρ − y) π − 2ρπ<br />

2ρπ<br />

= 2ρπ − 2yπ − 2ρπ<br />

2ρπ<br />

= − 2yπ<br />

2ρπ<br />

With Eq. (E.4), Hookes Law (Eq. (E.5)) can be written as<br />

E.3 Force Balance<br />

= −y = −κy (E.4)<br />

ρ<br />

σ = Eɛ (E.5)<br />

σ = −Eκy. (E.6)<br />

Since the system is in a state of equilibrium, both forces F1 and F2 have the same magnitude<br />

but opposite signs (Fig.E.3). Otherwise, the system would drift in one direction.<br />

E–4<br />

F1 + F2 = 0 (E.7)<br />

F2 = −F1 = F (E.8)

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