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. Author manuscript; available in PMC: 2013 Feb 18.
Published in final edited form as: Magn Reson Imaging. 2008 Oct 2;27(3):311–323. doi: 10.1016/j.mri.2008.07.018

Figure 1.

Figure 1

The Simulated Cube of a Diffusion Tensor Field FA values on the section triangle, ABC, form a representative snapshot of all possible FA values in this cube. This triangle thus provides a context in which we can compare the values of FA with values of EAR for the tensors within the cube. X corresponds to eigenvalue λ1 (L1), Y to λ2 (L2), and Z to λ3 (L3). The tetrahedron OADF occupies 1/6 of the cube, the region in which λ1 ≥ λ2 ≥ λ3. The FA value for the tensor at P(a,b,c) is the trigonometric Sin operator (multiplied by a constant) of the angle between lines PO and OF. Thus, the tensors at P and Q have identical FA values, as do the tensors at P′ and Q′. Indeed, all tensors (except the tensor on origin O) that lie on a single line passing through the origin O will have identical FA values.