Diapirs and cryptoexplosive structures
Why include diapirs and cryptoexplosive structures together?
They form at very different strain rates, and by different processes.
However, they both can occur in otherwise undeformed areas, and
have a central location that the deformation is often distributed
around (and hence can be considered point phenomena). Other than
this the reason is simply convenience.
Lecture index: Diapir
introduction. / Diapir traits.
/ Diapir Kinematics. / Mechanics
of diapirism. / Cryptoexplosive structures
- geoblemes or astroblemes. / Traits
of known impact structures. / Images
of Meteor Crater. / Crater morphology
as a function of size. /
Readings:
- Jackson, M. P. A. & Talbot, C. J., 1986,
External shapes, strain rates, and dynamics of salt structures;
Geol. Soc. of America Bull., v. 97, p. 305-323.
- Diapirs and circular features in Price, N.
J. & Cosgrove, J. W., Analysis of Geological Structures,
Cambridge Press. p. 110-121. This provides a good detailed summary.
Terms and concepts:
- salt pillows, salt anticlines, salt diapirs,
salt nappes, extrusive domes and salt glaciers
- various materials diapirs form from
- rim syncline and drag anticlines
- rim breccia zone
- radial and concentric fault patterns
- associated local unconformities
- caprock
- salt bulbs
- conditions of formation
- deforming forces:
- differential loading
- thermal convective
- tectonic forces
- central uplifts
- ejecta blankets
- crater lake deposits
- shatter cones
- shock lamellae
- suevite
- coesite and other high-P phases
- tektites
- cryptovolcanic vs. impact hypotheses
- Manson structure
- Serpent Mound structure
- Chixclub structure
Image from NASA's Visible Earth of a salt
diapir that has pierced an anticline (Kuh-e-namak) and an adjacent
slat diapir in the Zagros mountains of Iran (note that radial
drainage). Image source: http://visibleearth.nasa.gov/view_rec.php?id=17519
Why include diapirs and cryptoexplosive structures together?
They form at very different strain rates, and by different processes.
However, they both can occur in otherwise undeformed areas, and
have a central location that the deformation is often distributed
around (and hence can be considered point phenomena). Other than
this the reason is simply convenience.
Diapir
introduction
Reasons have been studied extensively:
- represent important petroleum traps.
- used to a greater and greater degree as storage
site (for gas, petroleum reserves), and considered as a site
for radioactive waste disposal.
- locally can cause extensive tectonism - halokinesis.
- mechanically intriguing bodies.
Intro thoughts:
- Geometry 1st discerned in 1862, in U. S.
Gulf coast area, is now a classic type locality.
- Initially mechanically enigmatic, an early
introduction to the idea the rocks can flow.
- Diapirs can consist of mud, halite, gypsum
(other salts also), serpentine, possibly gneiss. What do these
all have in common?
- Have been modeled using centrifuges by Ramberg.
Image of a mud diapir off the coast
of California (Santa Monica area). Image source and site of more
information: http://pubs.usgs.gov/of/1998/of98-518/
.
Diapir
traits
Geophysically - usually a marked gravity low
(because of the lower density of salt); useful exploration guide.
overall a mushroom shape, that typically originates
at depths of 12,000' or greater.
external structures:
- rim breccia zone:
solution and fault movement processes contribute to formation
of this breccia.
- arching and doming of strata overhead with
attendant radial and concentric patterns.
- local unconformities
in overlying strata (significance? - multiple movement episodes)
which are domed above the diapir
- radial and concentric faults: often normal
in character (local extension)
- drag anticlines and rim synclines
internal structures:
- caprock zone.
- upper bulges (lateral flowage).
- multiple bulbs
in upper head, multiple lobes of flowage.
- vertical foliation and flow lineation in
column, refolded folds.
- source bed pinch off.
Diapir Kinematics
Under what conditions does the material
become mobile?
- change in burial in density of sandstone,
shale, and salt; density of shale increases, that of salt the
same. Switch occurs at over at 3000 ', so after that would have
appropriate buoyancy forces.
- key is ability to flow in responses to differential
vertical load.
- empirically salt diapirs seem to originate
from source beds at 15,000 feet depth or greater.
- regional tectonism not necessary, but does
alter form - salt walls common, possibly controlled by anticline
crest breaching.
- rates of upward motion: generally mm/year
on average (but faster spurts possible?)
- solution related collapse perhaps unexplored
as a mechanism.
Cartoon image of history of Gulf
Coast salt tectonism. The imporatnt thing here is the multiphase
history related to loading and grwoth of sedimentary wedge on
the continental margin. Source of image: http://capp.water.usgs.gov/gwa/ch_f/F-text1.html
.
Mechanics of diapirism
Buoyancy; does it have to be positive (density
inversion with depth)? Consider gabbroic magma or serpentine.
Jackson and Talbot article provides 6 principal
mechanisms that shape salt tectonics:
- buoyancy halokinesis
- differential loading halokinesis
- gravity spreading halokinesis (for extrusive
diapirs)
- thermal convective halokinesis
- contraction tectonics
- extension tectonics
With differential loading you can easily envision
a positive feedback loop.
Dislocation glide map and temperature as critical
factor: experimentally c. 300° C is critical T at which reduce
strength and work hardening effect. Petrofabric studies (describe
for the students) indicate preferential gliding on (001) planes,
which should operate at 300° C or higher. Yet typical gradient
of 30° C/km would yield only 140°C at 15,000 feet. Is
there a thermal blanket effect? Perhaps the influence of brine
inclusions and other impurities greatly weakens the salt.
Diapiric rise of magmas?
The basic problem; given viscosity of granitic
magmas should rise so slowly that cool and crystallize before
ever get anywhere.
Fluid migration along a crack provides an alternate
model. Basically the idea is that the tips of a fluid filled crack
will migrate up a principal stress gradient. At depth vertical
fractures will be favored, but at a shallow level topography can
create a horizontal gradient.
An aside. My mother-in-law recently asked why
the extrusions didn't happen preferentially down in the valley
since it was a shorter route and should be easier for the magma
to squeeze up there. We were in Death Valley looking at the Ubehebe
Maar explosive craters and I had just related the story of the
Grand Canyon flows that had dammed the river. Clearly faults can
play a role as conduit and in some cases the faults are on the
side of the valley. However, there is another possible mechanism.
The topography itself actually can generate additional horizontal
compressive forces in the rocks in the valley floor and tensile
forces in the high flanking areas. It could be much harder to
open cracks at a shallow level right beneath the Grand canyon
floor than it is up on the shoulder. Thus the magma filled cracks
could be following the topographic stress guide.
Animations of development of salt diapirs along with explanatory text and a lot of other
material and images from Guglielmo and others at U. Texas.
References on salt diapirism:
- Jackson, M. P. A. & Talbot, C. J., 1986,
External shapes, strain rates, and dynamics of salt structures;
Geol. Soc. of America Bull., v. 97, p. 305-323. (good detailed
summary)
- Talbot, C. J. & Jackson, M. P. A., 1987,
Salt Tectonics; Scientific American, v. 257, : 2. A good bit
more general.
Cryptoexplosive structures - geoblemes or astroblemes.
A debate, that is
largely over, provides an interesting framework for this next
section. These features stand out as sites of intense deformation
within otherwise undeformed rocks. A number of them are well known
from the mid continent region. The term cryptoexplosive was coined
to try to sty descriptive, and neutral in this debae. The two
basic models as to origin of these features are : 1) they are
related to a volcanic event, perhaps volcanic gases, in some manner
similar to breccia and kimberlite pipes (a geobleme); or, 2)
they are related to meteorite impact - some level of exposure
of a crater. Most of these features are now recognized as impact
or crater structures. The crater is the surface morphology, but
what lies below?? What will it look like after the ravages of
time modify it.
This is a DEM image of Manicouagan crater
in Quebec, Canada. The circular pattern stands out. Note also
the central peak It qualifies as a cryptoexplosive structure.
Source: http://visibleearth.nasa.gov/view_rec.php?id=16403
Such features are worthy of discussion because
of:
- importance of impacts in very early history
of earth.
- importance of cratering in understanding
other planets surface processes.
- possible role in producing mass extinctions
on the earth.
- lesson in material behavior under unusual
conditions (shock waves, etc.).
- locally may be oil trap (high fracture permeability).
Typical traits or distinctive features:
- circular and kms to tens of kms in diameter.
- most apparent in otherwise undeformed rocks.
- central uplift.
- ring depressions.
- shock metamorphic minerals (coesite and stishovite,
jadeite).
- shock deformation lamellae.
- shatter cones.
- suevite (breccia with shock melt matrix).
- ejecta blankets.
- can come in multiple occurrences.
Image of shock lamallae in quartz
from the K-T boundary. Image source: http://esp.cr.usgs.gov/info/kt/boundary.html
Traits of known impact structures
List of some impact structures on earth
and elsewhere:
- a) recent unequivocal impact structures on
earth (rare).
- b) impact structures on other planets/moons.
- c) explosion cratering - bombs.
- d) laboratory-theoretical data.
Examples of unequivocal impact craters:
- Chubb crater, Canada
- Meteor (Barringer) crater, Arizona:
- circa 25,000 years old.
- 200 m deep and 1.1 km diamater of bowl shaped
depression.
- extensive ejecta blanket, 175*10^6 tons,
up to 2 km from rim, up to 25 m thick.
- 30 m of playa fill are underlain by 10 of
fallout breccia and then highly shocked and fused Coconino sandstone.
- Steinheim Basin, Germany
- Kentland, Indiana.
Images of Meteor Crater
Modified oblique computer image
of Meteor Crater from NASA's Visible Earth web site.
Image of center of Meteor Crater.
The flat floor is due to lake sediments. The talus cones on the
inner crater walls are of course post impact modifications. The
tilted strata can making up the crater rim are evident.
This is a cross section diagram
of the crater from the visitor's center.
Telephoto shot showing steeper tilting
right along the crater rim along with a subvertical radial fault
(can you see where the fault is located).
The broken jumble of white rock
above is the ejecta blanket, deposited above the tilted red, Triassic
Moenkopi sandstones.
Ejecta breccia near the crater rim
of Meteor or Barringer Crater, Arizona.
Photograph of part of the impactor!
This is a quarry wall in the Kentland,
Indiana site. Note the folded, faulted and subvertical layers
in the Paleozoic limestone. Within the craton and surrounded by
flatlying equivalent rocks, this area stands out as a point locale
of deformation. Shatter cones are also fairly common. This is
a fairly typical example of a crypto-explosive structure. Most
believe this to be an impact structure. The age of formation is
poorly constrained.
Crater morphology as a function of size
Crater processes and morphology are a function
of the size of the impactor.
- small and bowl shaped.
- flat-floored with central uplift.
- multi-ring structure with flat floor (flooded
by melts?).
King Crater on the far side of the
moon. Note the central peaks related to rebound and the central
peak. Note also the flat floor and the multiple rinc structures.
Some of this can be slump modification. This morphology is typical
of larger craters, and distinctly different than the small bowl-shaped
craters.
References
on cryptoexplosive structures and impacts
Early formulation of debate:
- Bucher, W. H., 1963, Crypto-explosion
structures caused from without or within the earth; American
Journal of Science, v. 261, # 7, p. 597-649.
- Dietz, R. S., 1963, Crypto-explosion structures:
a discussion; American Journal of Science, v. 261, # 7, 650-664.
Other useful references:
- Roddy, D. J., Pepin, R. O. & Merill,
R. B. (editors), 1977, Impact and explosion cratering;
Pergamon Press, N. Y. 1301 p.
- Silver, L. T. & Schultz, P. H., (editors),
1982, Geological implications of impacts of large asteroids
and comets on the earth; Geological Society of America Special
Paper # 190, 528 p.
- Hsu, K., 1989, Catastrophic extinctions
and the inevitability of the improbable; Journal of the Geological
Society of London, vol. 146, p. 749-754.
Copyright Harmon D. Maher Jr., This
may be used for non-profit educational purposes as long as proper
attribution is given. Otherwise, please contact me. Thank you.