For with , the symmetric tensor has principal axeswith eigenvalues , respectively. This follows directly from the outer product: , while it annihilates vectors perpendicular to . The orthogonal matrix with rows gives .
If depend on position, this is a pointwise eigenframe, not necessarily one fixed Cartesian change of axes throughout space. For , the displayed tensor vanishes and every orthonormal basis is a principal basis. Subtracting a scalar multiple of the identity leaves its eigenvectors unchanged and shifts every eigenvalue by the same amount; this is a simple case of coaxial symmetric tensors.
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