First, the computed stresses are transformed into a local orthonormal coordinate system x1-
x2-
x3, where the
x1 direction is oriented along the SCL. In 3D, you must specify the
x2 direction, and thus implicitly the x3 direction. In 2D and 2D axial symmetry, the
x3 direction is in the out-of-plane direction — that is, the Z and azimuthal directions, respectively.
The membrane stress tensor is the average of each local stress component along the SCL:
Each component of the bending stress tensor is assumed to have a linear variation along the SCL, with the value being zero at the midpoint.
Finally, the peak stress tensor is defined at the two endpoints of the SCL. It is the difference between the actual stress tensor, and the linearized stress representation.
The stress intensity, also known as the Tresca equivalent stress, is often the ultimate goal of a stress linearization. It is computed as a worst case of the equivalent stress at the two ends of the SCL. The stress intensity is computed from the principal stresses as