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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

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