12.9 PLANE STRESS AND PLANE
STRAIN
The
general state of stress and strain is three-dimensional but there exist
particular geometric configurations that can be treated differently.
Plane Stress
The
two-dimensional, or biaxial, stress state is also called plane stress.
Plane stress
requires that one principal stress be zero. This condition is
common in some applications. For example, a thin plate or shell may also have a
state of plane stress away from its boundaries or points of attachment. These
cases can be treated with the simpler approach of equations 12.7.
Plane Strain
There
are principal strains associated with the principal stresses. If one of the
principal strains (say
3) is zero, and if the remaining strains are
independent of the dimension along its principal axis,
n
3,
it is called
plane strain
. This condition occurs in particular
geometries. For example, if a long, solid, prismatic bar is loaded only in the
transverse direction, regions within the bar that are distant from any end
constraints will see essentially zero strain in the direction along the axis of
the bar and be in plane strain. (However, the stress is not zero in the
zero-strain direction.) A long, hydraulic dam can be considered to have a plane
strain condition in regions well removed from its ends or base at which it is
attached to surrounding structures.
12.10 APPLIED VERSUS
PRINCIPAL STRESSES
We
now want to summarize the differences between the stresses
applied to an element
and the principal stresses that may occur on
other planes as a result of the applied stresses. The
applied stresses
are the nine
components of the stress tensor
(equation 12.5a, p. 348) that result from
whatever loads are applied to the particular geometry of the object as defined
in a coordinate system chosen for convenience. The
principal stresses
are the three
principal normal stresses
and the three
principal
shear stresses
defined in
Section 12-8. Of course, many of the applied-stress terms may be zero in a
given case. For example, in a tensile-test specimen the only nonzero applied
stress is the
x
term
in equation 12.5a (p. 348), which is unidirectional and normal. There are no
applied shear stresses on the surfaces normal to the force axis in pure tensile
loading. However, the principal stresses are
both normal and shear.
In
a tensile-test specimen, the applied stress is pure tensile and the maximum
principal normal stress is equal to it in magnitude and direction. But a
principal shear stress of half the magnitude of the applied tensile stress acts
on a plane 45
°
from the plane of the principal normal stress.
Thus, the principal shear stresses will typically be nonzero even in the
absence of any applied shear stress. This fact is important to an understanding
of why parts fail. The most difficult task for the machine designer is to
correctly determine the locations, types, and magnitudes of all the applied
stresses acting on the part. The calculation of the principal stresses is then
pro forma
using equations 12.5 to 12.7 (pp. 348-350).
Copyright 2004, Industrial
Press, Inc., New York, NY