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March, 1925 f<strong>org</strong>ing- Stamping - Heat Treating 79<br />
reduction of area on the outer portion of the bend. To<br />
avoid the extensive reduction of area on the outer side<br />
of the specimen, which would eventually lead to the<br />
rupture of the metal on this side of the article, the<br />
metal on the concave surface which is already under<br />
compression tends to flow across the bar towards the<br />
convex face, thus providing metal to compensate for<br />
the deficiencies of the material that are produced by<br />
the plastic flow on the convex surface. The metal on<br />
the inner surface is already under compression and is<br />
predisposed to flow. It is also sufficiently plastic to<br />
flow easily, and as a result it tries to travel in a general<br />
way towards the convex surface. The probability<br />
of this type of flow can readily be seen by bending the<br />
bar in the cold. The metal must have some moderate<br />
supply of ductility, as otherwise bending experiments<br />
are rather absurd. If such a bar is bent it will be found<br />
that the metal flows evenly on the convex face and for<br />
a short time evenly on the concave face. Very soon<br />
crinkles appear on the concave side and spread into<br />
the bar more and more as the bending is increased.<br />
Naturally some material is in this instance being<br />
pushed outwards, i.e., towards the radius of the bend.<br />
This means that towards the inwards, apices of the<br />
crinkles there is a stress tending to drive the metal<br />
inwards, i.e., towards the convex face. In the cold<br />
bar the metal is too rigid to flow far, but in the hot,<br />
easily deformed metal, this stress operates and does<br />
actually drive the metal towards the convex face.<br />
The nature of the action here described can be understood<br />
easily by a reference to the drawings in Fig.<br />
1. The original bar is shown in Fig. 1A. In Fig. IB<br />
is shown the theoretical way in which the metal might<br />
be expected to flow during the bending. In Fig. 1C<br />
is shown what very often does occur and what always<br />
occurs if the conditions are suitable. This figure indicates<br />
very clearly that a kink forms on the concave<br />
side of the bar by reason of the way in which the<br />
metal flows from this position towards the convex<br />
side in order to neutralize the deficiency of the metal<br />
in the part which is being stretched.<br />
Fig. 2 shows an actual section from a bend made in<br />
this way and indicates the defect that has been produced<br />
upon the inner surface of the bent article.<br />
How can this kink be avoided? The best method<br />
undoubtedly is to arrange not to bend a uniform section.<br />
The kinking can be prevented fairly definitely<br />
by increasing the diameter of the bar at the point<br />
where it is to be bent. If a kneecap of metal is put<br />
onto the bar on the inner side, more metal is available<br />
to flow across the canvex side during bending. This<br />
prevents the excessive flow of the metal at one place<br />
that eventually leads to a kink. Similarly, if there is<br />
an accumulation of metal on the outer surface there is<br />
more material to extend plastically than in a plain bar.<br />
The outer surface can then be deformed without creating<br />
a marked deficiency at any one place and therefore<br />
without calling for the flow of metal from the concave<br />
to the convex surface. Both these actions are shown<br />
in Fig. 3. The most reliable method is to combine the<br />
two actions, thus giving an excess of metal on both<br />
faces, but particularly on the convex side.<br />
If a bar has kinked in the way already described,<br />
the defect may or may not be subsequently incorporated<br />
in the f<strong>org</strong>ing. There is as great a probability that<br />
it will be, as that it will not be, for the eventual position<br />
of the defect is very considerably governed by the<br />
amount of metal that is extruded from the pattern during<br />
f<strong>org</strong>ing in the dies. The location of the defect is<br />
also affected by the quantity of metal on both sides<br />
of the bend — convex and concave — as will be shown<br />
later. It is perfectly possible, however, to produce<br />
the same type of defect in the finished f<strong>org</strong>ing from a<br />
bar which has not kinked during preliminary f<strong>org</strong>ing.<br />
This is likely to arise in several ways, but two definite<br />
examples can be examined. Both of them really arise<br />
from the same cause, which is, put briefly, a shortage<br />
of metal in the bar at the time that it is introduced<br />
between the dies.<br />
Imagine that an article containing a corner like that<br />
shown in Fig. 4A is to be made. The dies for the corner<br />
will be approximately as shown in Fig. 4A, and it<br />
can be assumed that a bent bar has been prepared.<br />
As soon as this bar is placed between the dies, work<br />
will be done upon it, and the tendency of the metal<br />
will be to flow towards the corner X. As the metal in<br />
the bar will always attempt to flow in this direction,<br />
the movement of this convex surface will tend to draw<br />
the remainder of the metal after it away from the concave<br />
corner, just as has already been described. At<br />
this side X, the excess of metal is extruded from the<br />
impression. The general action of the dies is therefore<br />
to decrease the radius at the corner, which is<br />
FiG.4 Fic.e<br />
FIG. 4 (A)—The pattern in the dies showing form of corner.<br />
(B) The defect in the resulting f<strong>org</strong>ing.<br />
FIG. 5—Outline of typical crankshaft.<br />
FIG. 6—Diagram of type of defect produced in the<br />
crankshaft at X.<br />
equivalent to making the bend more severe, or to<br />
bending the bar through a larger angle. The effects<br />
produced are therefore quite similar to those that have<br />
already been described with a plain bar. If there is<br />
sufficient metal in this portion of the bar to fill the<br />
dies completely and to make each, portion of the die<br />
do its share of work, it is probable that the dies will<br />
be kept properly filled. Under these conditions there<br />
will be an excess of metal to be extruded both at<br />
the point X and at the point Y. If on the other hand<br />
there is any deficiency of metal it will become most<br />
evident at the point Y, which is the concave side of<br />
the bend. From the position Y the metal will flow<br />
towards the position X and will draw in and kink and<br />
form a gall at Y, as shown in Fig. 4B, in just the same<br />
way as occurs in the simple bending outside the dies.<br />
This action may occur in a bar which is quite free<br />
from any initial kink or shut, the actual operation of<br />
f<strong>org</strong>ing being quite sufficient to cause it to take place.<br />
The obvious remedy for the production of this type of<br />
defect is to have sufficient metal on the bar, in the<br />
part that is likely to form a gall, and consequently to<br />
avoid the sucking action of the metal towards the convex<br />
side of the pattern.<br />
This explanation of the spontaneous production<br />
of a gall when f<strong>org</strong>ing a bar that is initially free from