Short Answer:
Principal stresses are the normal stresses acting on special planes (principal planes) where shear stress is zero. In a 2D stress element with normal stresses and shear , the two principal stresses are the extreme values of normal stress and are given by a compact formula that uses the average stress and a square-root term involving the stress differences and shear.
These principal stresses are
and the principal plane orientation satisfies . These equations let you find magnitudes and directions where only normal stresses act.
Detailed Explanation :
Principal Stresses
Derivation
Start with a small 2-D stress element subjected to normal stresses and on the x and y faces, and shear stress . Consider a plane through the element inclined at angle measured from the x-axis. The normal stress and shear stress on that inclined plane (using standard transformation formulas) are:
(Signs depend on the sign convention; these forms are the commonly used ones.)
Principal planes are those orientations where the shear stress on the plane is zero, i.e. . Set the expression for to zero:
Rearrange to obtain the angle of principal planes:
This gives the orientations of the principal planes (two solutions differing by ). Once is known, substitute into the expression for to get the principal stresses. However, a cleaner algebraic route avoids computing explicitly.
We want the extreme (maximum and minimum) values of with respect to . An extremum of occurs when the derivative . Differentiating the expression for :
Setting this to zero,
which is algebraically identical to the condition for and gives the same . Now evaluate at those . A standard manipulation yields the principal stresses without substituting explicitly:
Define the average normal stress and the radius term :
Then the two principal stresses (the extreme values of ) are
Writing this explicitly:
This is the standard formula for principal stresses in a 2-D stress system.
Principal plane angle
To find the angle of the principal plane (where acts), use
From you get . Note that gives the orientation of the plane on which shear vanishes and the normal stress equals or . The other principal plane is .
Alternate viewpoint: Mohr’s Circle
Graphically, these results are represented by Mohr’s circle. The circle center is at on the -axis and radius . The intersection points of the circle with the -axis are and . The top/bottom points of the circle give the maximum shear . Mohr’s circle offers a quick visual way to get principal stresses and orientations.
Remarks and uses
- is the major principal stress (largest), the minor (smallest) in plane stress.
- These formulas assume plane stress (no or ); for full 3-D stress there are three principal stresses from the characteristic equation of the stress tensor.
- Principal stresses are used in failure criteria (e.g., maximum principal stress, Tresca, von Mises), and in locating critical planes for yielding or fracture.
Conclusion
The principal stresses in a 2-D stress element are given by a simple closed form: the average normal stress plus or minus a radius term that combines half the normal stress difference and the shear. The principal directions come from . These results let engineers find the planes of pure normal stress and the extreme normal stresses—key information for safe and efficient design.