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3 Fundamentals of press design

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30 Basic principles <strong>of</strong> metal forming<br />

specific deformation work w id<br />

1000<br />

Nmm<br />

mm 3<br />

800<br />

700<br />

600<br />

500<br />

400<br />

300<br />

200<br />

100<br />

0<br />

flow stress k f<br />

1000<br />

N<br />

mm 2<br />

800<br />

700<br />

600<br />

500<br />

400<br />

300<br />

200<br />

100<br />

If there is no flow curve available for a particular material, it can be<br />

determined by experimentation. A tensile, com<strong>press</strong>ive or hydraulic<br />

indentation test would be a conceivable method for this. If the specific<br />

deformation work w id and the entire volume V or the displaced volume<br />

V d are known quantities, the total deformation work W is calculated on<br />

the following basis:<br />

2.2.4 Formability<br />

0<br />

St 14<br />

St 37<br />

C35(normally annealed)<br />

0,2 0,4 0,6 0,8 1,0 1,2<br />

log. principle deformation g ϕ<br />

W V w k<br />

V V k<br />

id<br />

fm<br />

= ⋅ ≅ ⋅ϕg⋅ = d ⋅<br />

η<br />

η η<br />

F<br />

Fig. 2.2.2<br />

Flow curves<br />

and curves<br />

showing the<br />

specific deformation<br />

work<br />

for different<br />

materials<br />

The identification <strong>of</strong> formability should only be based on those cases <strong>of</strong><br />

material failure caused as a result <strong>of</strong> displacement or cleavage fractures<br />

where no further deformation is possible without failure. If, therefore, a<br />

material breaks before reaching maximum force as a result <strong>of</strong> a cleavage<br />

Metal Forming Handbook / Schuler (c) Springer-Verlag Berlin Heidelberg 1998<br />

F<br />

fm<br />

F

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