Chapter 3 - Rolling of metals
Chapter 3 - Rolling of metals
Chapter 3 - Rolling of metals
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h o<br />
The maximum reduction<br />
v o<br />
The critical variables are<br />
L p and h<br />
A<br />
α<br />
R<br />
R-a<br />
B C<br />
L p<br />
A large diameter roll will permit a<br />
thicker slab to enter the rolls than will<br />
a small-diameter roll.<br />
= tanα =<br />
R<br />
L p<br />
D<br />
a<br />
h<br />
R∆h<br />
≈ ≈<br />
− ∆h<br />
/ 2 R − ∆h<br />
/ 2<br />
∆h<br />
R<br />
From triangle ABC, we have<br />
Suranaree University <strong>of</strong> Technology Tapany Udomphol<br />
Jan-Mar 2007<br />
R<br />
L<br />
L<br />
2<br />
2<br />
p<br />
2<br />
p<br />
=<br />
=<br />
L<br />
R<br />
2<br />
p<br />
2<br />
+ ( R − a)<br />
− ( R<br />
= 2Ra<br />
− a<br />
2<br />
2<br />
2<br />
− 2Ra<br />
+<br />
As a is much smaller than R, we<br />
can then ignore a 2 .<br />
L p<br />
≈ 2Ra<br />
≈<br />
R∆h<br />
Where ∆∆∆∆h = h o – h f = 2a<br />
2<br />
( ∆h)<br />
= µ R<br />
a<br />
2<br />
)<br />
…Eq.6<br />
µ …Eq.7<br />
max