Geology of salt
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Salt is part of
a group of chemically deposited minerals which crystallize by evaporation of
salt-rich lake or seawater. Their chemical compositions reflect the original
composition of the brine. The largest known, and also economically most
important salt occurrences on earth are of marine origin. The sequence of
evaporites results from variations in the chemistry of the brine from which
they were deposited. The word salt is used as a general name for evaporitic
salts, like halite (NaCl), sylvite (KCl), carnallite (KClMgCl2.6H2O),
kainite (KClMgSO4.2.75H2O), kieserite (MgSO4.H2O)
and bischofite (MgCl2.6H2O). It occurs in the subsurface
of NW Europe in deposits of Permian, Triassic and Jurassic age.
Salt is in many
aspects unlike other sedimentary rocks. Not only is it able to form at
geologically impressive sedimentation rates of up to 10 cm/a, i.e. up to 1000
times faster than clastic sediments (Schreiber & Hsü, 1980); furthermore it
does not or hardly compact with depth since its density is controlled by its
crystal structure. Most important, however, is its ability to deform
plastically. This is shown in many different settings around the world, from
passive margins (e.g. Gulf of Mexico, West Africa), foldbelts (Zagros,
On a geological
time scale, and when buried below 500 m, salt behaves in a visco-plastic way,
whereas other sedimentary rocks show brittle deformation. Rock salt compacts
already during early stages of burial to a tight mass with a constant density
of 2168 kg/m3. Other sediments show an increase in density with
depth owing to cementation and the reduction of pore volume as a function of
overburden and pore pressures. Consequently, in near-surface positions, where
sand and clay typically show densities of 1200 to 1400 kg/m3, halite
is relatively heavy, whilst below 500 m it is lighter than surrounding rocks.
This results in an unstable situation. Under the right conditions, the salt
rises while solid rocks sink (Trusheim, 1963; Kockel, 1990; Remmelts, 1995).
This process of flowing and rising salt is called halokinesis. It
will only start when the salt successions have thicknesses of at least several
hundreds of metres, and when a fault with a significant throw affects the base
of the salt. Without such a trigger no halokinesis will occur; this is
for instance the case for the Zechstein in part of

Model for the development of salt structures (after RGD, 1993).
Salt will
initially flow mainly in a lateral sense, forming what is known as salt
pillows. Above a pillow, the sedimentary cover is not yet pierced. In the next
stage a pillow can evolve into a salt diapir. The growth of the pillow causes
extension and subsequent faulting and weakening of the sedimentary cover above
the evolving diapir (Jenyon, 1986; Remmelts, 1996). In cases of strong uplift,
erosion may further weaken this cover. These processes take millions of years.
The Zechstein
salt in the
The shapes and
the internal structures of individual salt bodies are complex; reference is
made to descriptions by De Boer (1971), Richter-Bernburg (1972, 1980), Kupfer
(1976), Bornemann (1991) and Geluk (1995). Salt diapirs outcropping in the
Iranian Dasht-e-Kavir (Jackson et al., 1990) and Zagros Mountains (Kent, 1979),
and in the Spanish Pyrenees (Wagner et al., 1971) present analogues for buried
salt structures in the Netherlands (Geluk, 1998, 2000).

Example of a salt structure which underwent Late Cretaceous compression.
NE of Assen, The
A good
understanding of the mechanical behaviour of the various components within a
salt sequence is a prerequisite to understand their deformation. Some rocks,
such as interbedded claystones, thick anhydrites (> 1 m) and carbonates are
brittle in the subsurface. Potassium-magnesium salts on the contrary are mostly
ductile during deformation. Mixed rock types behave differently than the
separate components. For instance, a thin-bedded alternation of anhydrite and
salt can be deformed in a ductile manner, while one thick layer of anhydrite
embedded in salt deforms in a brittle way (Lotze, 1957). Usually the stiffer
layers will be folded within the softer layers, a structure that can often be
observed in conventional salt mines and also in salt cores from boreholes.
Different
internal tectonic styles can be recognized in salt structures. In literature a separation
is commonly made between layers, pillows and domes or diapirs, which represent
increasing states of salt deformation (Trusheim, 1963).
In salt layers
the top and bottom of the layer are more or less parallel to the interbedded
elastic carbonate and anhydrite beds, reflecting the original deposition. Salt
layers may be faulted if the throw of sub-salt faults exceeds the thickness of
the salt, e.g. in areas with relatively thin Zechstein salt. In basinal areas
the thickness of the Z2 (Stassfurt) Salt (500-800 m) generally exceeds the
throw of the fault, which then only affects the base. The internal structures
of salt layers are mainly flow folds with horizontal axial planes (Lotze,
1957). They occur on the decimetre to decametre-scale. Potassium-magnesium
salts, with interbedded layers of halite, usually show strong folding.
Salt pillows
are formed by a local thickening of the salt due to horizontal salt flow. In
central areas of the Zechstein basin the cores of the pillows are composed of
the Z2 (Stassfurt) Salt; in marginal areas the Z1 (
In salt domes
or diapirs the movement of the salt changed from mainly horizontal to mainly
vertical, and the salt pierced the cover beds. The vertical flow results in
folds with vertical axial planes and horizontal fold axes as well as in curtain
folds with vertical fold axes. As a result of the diapirism these latter folds
usually have deformed the older generation of folds with horizontal fold axes.
However, due to the extremely high strains of more than 300% in the diapir, the
older deformation phase may be indistinguishable. Along the margins of diapirs,
friction between the cover beds and the uprising salt mass results in high
vorticities within this mass, with an additional complex fault pattern (Jackson
et al., 1990). Sometimes the salt may even envelop blocks of the overlying
succession. The salt in a diapir rarely moves at a uniform rate (Kupfer, 1976).
Shear zones separate sectors moving at higher speed, known as spines, from
those moving more slowly. The development of salt diapirs normally results in a
complicated internal structure, with folds of many different scales and
orientations (Richter-Bernburg, 1980). Compressional tectonics during the Late
Cretaceous accelerated the rate of diapirism, or strongly deformed some of the
diapirs. A generalized simplified model of Zechstein salt diapirs is that the
central part of the dome contains mostly Z2 Salt and that the marginal parts
are made up of younger salt units. This is shown to be true for structures such
as the Winschoten and Zuidwending diapirs (Harsveldt, 1980, 1986). In the
Pieterburen diapir, however, the central part is made up of younger salts and
the Z2 Salt occurs at the margin (Harsveldt, 1980; RGD, 1995); in
Several salt
domes in the
Last modified 10/03/2009