The problem of expressing a general 3-D magnetotelluric (MT) impedance tens
or in the form of a 2-D tensor that has been distorted in some way is addre
ssed first in terms of a general theorem. This theorem shows that when the
real and quadrature parts of a tensor are analyzed separately as distinct m
atrices, all that is necessary to make a matrix with 2-D characteristics fr
om one with 3-D characteristics is to allow the electric and magnetic obser
ving axes to rotate independently.
The process is then examined in terms of the operations of twist and pure s
hear ("split") on such matrices. Both of two basic sequences of split after
twist, and twist after split, produce a typical 3-D matrix from one initia
lly 1-D, with the parameters of split contributing 2-D characteristics to t
he final matrix. Taken in reverse, these sequences offer two basic paths fo
r the decomposition of a 3-D matrix, and are seen to be linked to the initi
al theorem.
The various operations on matrices are expressed diagrammatically using the
Mohr circle construction, of which it is demonstrated two types are possib
le. Mohr circles of an observed MT tensor display all the information held
by the tensor, and the two types of circle construction respectively make c
lear whether particular data are well suited to modeling by either split af
ter twist, or twist after split. Generally, tensor decompositions may be di
splayed by charting their progress in Mohr space.
The Mohr construction also displays the invariants of a tensor and shows th
at tensor decomposition can be viewed as a process of determining an approp
riate set of invariants. An expectation that the origin of axes should be o
utside every circle categorizes as irregular any tensors which, in either t
he real or quadrature part, do not satisfy a Z(xy)Z(xy) < Z(xx)Z(yy) criter
ion.
The theory of the present paper applies equally to procedures for distortin
g 1-D and 2-D model calculations for the purpose of matching observed 3-D d
ata.