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ReseaRch a n d developmenT In T h e aR m y 25<br />
<strong>as</strong>pects of it emulated more speculative studies underway in universities and industrial<br />
laboratories on the fundamental behavior of crystalline materials. 40<br />
Among the many problems faced by researchers at the Frankford Arsenal<br />
w<strong>as</strong> how to ensure with re<strong>as</strong>onable certainty that the small-arms ammunition<br />
and artillery shells turned out by the production lines would function properly<br />
on the battlefield. Maintaining high standards of quality control depended in<br />
part on a detailed understanding of the behavior of the metal components used<br />
in the manufacturing process. During World War II, laboratory research in this<br />
field focused on theoretical and experimental studies of the pl<strong>as</strong>tic deformation<br />
of metals. A metal changes shape when it is subjected to an external load, such<br />
<strong>as</strong> pressing, rolling, or forging. Depending on the arrangement of the atoms that<br />
make up its internal structure, the metal will either retain that new shape or return<br />
to its original dimensions. Pl<strong>as</strong>ticity is the mechanical property that determines<br />
the extent to which a metal maintains its shape following the application of an<br />
external force. Since the 1920s, physicists and metallurgists in the United States<br />
and Europe had constructed various theories to explain the mechanism by which<br />
metals deformed pl<strong>as</strong>tically. One explanation that gained acceptance during this<br />
period focused on the concept of the dislocation, a point defect or imperfection<br />
in the lattice structure of a metal. First introduced in 1934, dislocation theory<br />
suggested that atomic imperfections predisposed metals to deform and fracture<br />
at stress levels lower than those predicted for ideal crystals. It also provided<br />
some clues <strong>as</strong> to why pl<strong>as</strong>tically deformed metals exhibited incre<strong>as</strong>ed resistance<br />
to further deformation, a phenomenon called work hardening. By the end of the<br />
decade, dislocation theory had emerged <strong>as</strong> one of the leading explanations of<br />
pl<strong>as</strong>tic deformation in metals, and it h<strong>as</strong> continued to be an important subject of<br />
study in materials science. 41 Dislocation theory and the experimental studies that<br />
supported it had a significant impact on the development of ordnance materials<br />
at Frankford Arsenal, and within the arsenal system in general, during and after<br />
World War II.<br />
Even though the existence of dislocations w<strong>as</strong> not verified experimentally<br />
until 1955, physicists working in industrial and academic laboratories in the late<br />
1930s had used dislocation theory to explain certain types of metallic behavior<br />
that turned out to be directly relevant to ordnance development and production<br />
in the arsenal system. Internal friction w<strong>as</strong> one particularly important property<br />
that received widespread attention. The intensity of this phenomenon depends<br />
on the extent to which the vibrational energy absorbed by a metal from an<br />
external source is dissipated nonuniformly <strong>as</strong> it propagates from one atom to<br />
another in the crystal lattice. Energy loss is greatest w<strong>here</strong> imperfections, or<br />
dislocations, exist in the atomic arrangement of the metal’s internal structure.<br />
Before the war, a small team of physicists at the Westinghouse Electric and<br />
Manufacturing Company in Pittsburgh and the University of Pennsylvania in<br />
Philadelphia pioneered research on the internal friction of metals.<br />
40 See C. H. Greenall, “Non-Ferrous Metallurgical Research at Frankford Arsenal,” Journal of Applied<br />
Physics 16 (December 1945): 787–92.<br />
41 Hoddeson et al., Out of the Crystal Maze, 317–33.