in terms of the protolith fabric, such as the relict por-
phyritic texture in a meta-andesite (Figure 14.3).
Although the imposed fabric of metamorphic rocks
created under subsolidus conditions shares some sim-
ilarities with the fabric of magmatic rocks, there are
distinct differences. Metamorphic rocks are aphanitic
and phaneritic like magmatic rocks; they are never
glassy because metamorphic systems, by definition,
never contain a melt that can quench to glass. Nor do
confined metamorphic rock systems in the deep crust
have a separate expanding volatile fluid phase that is
involved in volcanic systems. Where present, a fluid
is limited to intergranular spaces and local fractures.
There are only a limited number of ways by which
basic grain shapes can be stably arrayed in a recrystal-
lizing solid. Subsolidus equilibration of grain shapes in
metamorphic aggregates tends to converge toward a
few basic patterns and mutual relations, thus yielding
fewer fabrics than are created in crystallizing magmas.
Despite these simplifying factors, whose expression
is obvious in many isotropic fabrics (Section 14.1.2),
complex interactions between solid state recrystalliza-
tion and ductile deformation that results from imposed
nonhydrostatic stresses are widespread in metamor-
phic systems. These interactions are expressed in the
penetrative anisotropic fabrics of tectonites that typify
regional terranes in orogens. Tectonites commonly
evolve through multiple overprints of deformation and
recrystallization during polymetamorphism. Complex
tectonite fabrics are, at once, both beautiful to behold
and challenging to unravel and interpret. This com-
pound attribute has resulted in a number of richly
illustrated compendia with interpretive discussions;
these include Weiss (1972), Borradaile et al. (1982), Fry
(1984), Barker (1990), Yardley et al. (1990), Twiss and
Moores (1992, Chapter 13), Passchier and Trouw
(1996), and Snoke et al. (1998).
15.1.1 Anisotropic Fabrics of Tectonites
The penetrative aspect of tectonite fabrics implies
particular properties are present throughout every
part of the rock body. In the ideal case of a uniform,
or homogeneous, deformation, properties observable
on the microscopic scale integrate and build into the
increasing larger scale attributes possessing similar
form and geometry that can be seen in hand samples,
outcrops, and even entire terranes (Figure 14.14). This
fractal-like character of tectonites means that there
can be little real distinction between the endeavors of
the structural geologist and the metamorphic petrolo-
gist investigating tectonite fabrics; they can, in fact, be
quite complementary.
It must be pointed out, however, that many meta-
morphic bodies have been inhomogeneously deformed
because of heterogeneities in rheologic response in
different parts (Figure 14.38). In addition, overprinted
processes, such as localized high-strain-rate shear in
mylonite zones and partial melting, can also create
heterogeneous fabric on the outcrop scale (see Figure
15.5).
Imposed penetrative tectonite fabrics can be ex-
pressed in many different ways. Some depend on di-
mensional aspects of individual mineral grains in the
rock aggregate. Thus, platy phyllosilicate and graphite
grains may have a preferred orientation so that their
longest dimensions are more or less parallel in a rock;
the fabric is a planar foliation. In other rocks, columnar
or needle-like amphibole grains may have a preferred
orientation so that their one longest dimension is more
or less parallel in a rock; the fabric is a lineation. Felsic
and carbonate mineral grains that are ordinarily equant
may be flattened or elongate in some rocks so as to ex-
press a foliation or lineation or both. Other anisotropic
fabrics depend on compositional layering and inequant
aggregates of minerals; still others on structures, such
as folds. In some tectonites, the anisotropy is a cryptic
preferred orientation of crystal lattices in the mineral
grains that is not visible to the unaided eye. For ex-
ample, the c-axes of quartz grains in a mylonite can be
uniformly oriented at a large angle to the foliation.
The most common anisotropic fabric is foliation,
sometimes designated as an S-surface from the German
word Schiefer, meaning schist. Multiple foliations in a
rock may be desigated, from oldest to youngest, as S
1
,
S
2
, S
3
, and so on. A tectonite that possesses one or more
foliations is said to be an S-tectonite. Rarely are tec-
tonites only lineated; one such L-tectonite would be a
nonfoliated rock that contains subparallel columnar
amphiboles. Many S-tectonites also have a penetrative
lineation that is visible on or within foliation surfaces;
such rocks are L–S-tectonites. It should be remem-
bered that line traces of a foliation exposed on random
oblique surfaces do not constitute a true lineation
(Figure 14.12).
In tectonites, there is never a perfect preferred
orientation of inequant grains, aggregates of grains, or
lattices of grains that define the anisotropic fabric.
Not every one of the columnar amphiboles in the
L-tectonite just cited is exactly parallel. The degree
to which the preferred orientation is developed varies
between the ideal end-member extremes of perfectly
oriented (never attained in nature) and random
(isotropic).
Under the same metamorphic conditions (non-
hydrostatic state of stress, P, and T), the character
of anisotropy in a rock depends on its mineralogical
and modal composition. Understandably, abundant
oriented platy micas and chlorites in low-grade pelites
create a strong foliation so that the rock readily splits
into parallel plates or slabs when struck by a hammer.
This physically or mechanically significant foliation in
aphanitic rocks has been utilized for centuries in the
448 Igneous and Metamorphic Petrology