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3 Fundamentals of press design

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Deep drawing and stretch drawing<br />

blank holder<br />

die<br />

Fig. 4.2.7 Beads restraining material flow in the blank holder<br />

punch<br />

brake bead<br />

Draw energy<br />

For drawing operations on double-action <strong>press</strong>es, the required draw<br />

energy W d [Nm] is the product <strong>of</strong> the <strong>press</strong>ing force F U [N], the drawing<br />

stroke h [m] and a correction factor x [–]:<br />

Wd = x⋅FU ⋅ h [ Nm]<br />

The correction factor, which is dependent on the material and the draw<br />

ratio � = D/d, takes into account the actual drawing force characteristics;<br />

this factor fluctuates between 0.5 and 0.8. The higher level is for s<strong>of</strong>t<br />

materials, which can be drawn with the maximum draw ratio � max and<br />

for flanged shells, which are only partially but not completely drawn<br />

through. The lower level is for a small draw ratio, that is to say for short<br />

drawing depths or for harder grades <strong>of</strong> sheet metal. When drawing normal<br />

materials, calculations can be based on x � 0.65 up to 0.75.<br />

A sufficiently accurate rough calculation formula for estimating the<br />

draw energy <strong>of</strong> a double-action <strong>press</strong> is:<br />

2<br />

Wd FU h Nm<br />

3<br />

= ⋅ ⋅ [ ]<br />

With a single-action <strong>press</strong> with a draw cushion, the slide force is<br />

increased by the blank holder force F B [N]:<br />

W = ( x⋅ F + F )⋅ h [ Nm]<br />

e U B<br />

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

173

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