The Dead Sea region has experienced six destructive earthquakes during the last 1000 years, with an average recurrence interval of around 200 years (188 to be exact) beginning with the 1060 AD earthquake. This cluster of events ended with the 1927 earthquake which had a magnitude of 6.2.
The Dead Sea Fault is a Left lateral transform plate boundary, separating the Arabian plate and the Sinai sub-plate and has been active since the Miocene, with movement still occurring in present day. (Fig. 1). (Garfunkel, 1981). This fault zone lies within the Dead Sea graben of which this post will focus upon. More specifically, depositional attributes of the laminated layers that comprise the sedimentary record of the Dead Sea and how those layers can serve as a portal into the past regarding paleo-seismic events.
With the recent drop in lake levels, the banks are quite accessable. By scraping away the halite/sand encrusted sides of these banks, layers of mud and sand/silt are exposed. Instead of being undisturbed laminated layers of sediment, you see beautful swirls and designs where the layers have intermixed. These disturbances, termed siesmites, are not only quite stunning to behold but also have an important significance in regards to providing a geologic record on ancient earthquakes along the Dead Sea transform.
The lacustrine sediments of the Dead Sea are comprised of alternating layers of aragonite and detritus sediments. The latter of which are composed of dark, silt-clayey size detritus derived from flooding (fluvial events) as suspended material and range in thickness from a couple of centimeters to almost 20 (can vary; these are my measurements). The aragonite layers are intermingled white and dark laminae of silt-clayey sized detritus, and are much thinner in comparison, being in the thicknesses of millimeters. (Bookman, et al., 2004). These layers were originally continuous alternating laminae of aragonite and fine detritus, lying flat on the bottom of the Dead Sea undisturbed. They were later fluidized (brought on by seismic events), disturbing the top of the sediment and causing it to be drawn back into suspension. Deformation of the laminae occurs when the sediment comes to rest after resettling. The event is encompassed by undisturbed sediments above and below. This mixed layer indicates a disturbance due to a seismic event, and its timing is constrained by the first overlying undisturbed lamina.
Syndepositional faulting in the Dead Sea sediments has been interpreted as when (Marco et al, 2004) a fault offsets a surface creating subaqueous scarp. The top of the sediment is deformed due to liquefaction and suspension during a seismic event, and a mixed layer forms on both sides of fault scarp. After the suspended sediments resettle, the mixed layer in down-thrown block is slightly thicker. As further sedimentation ensues, a thicker sequence accumulates on down-thrown block. The lower mixed layer in the downthrown block is also bent and overlain by folded layers.
The occurrence of seismites and their correlation to historically documented earthquakes has been determined by radiocarbon dating organic material found within the layers of sediment, solidifying the association of fluidizations of sediment and seismic events.
Bookman (Ken-Tor), R., Enzel, Y., Agnon, A. and Stein, M. 2004: Late Holocene lake levels of the Dead Sea. GSA Bulletin 116, 555 71.
Garfunkel Z (1981) Internal structure of the Dead Sea leaky transform (rift) in relation to plate kinematics. Tectonophysics 80:81-108
Marco, S., and Agnon, A., 1995. Prehistoric earthquake deformations near Masada, Dead Sea graben. Geology, 23: 695-698.
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Showing posts with label sedimentology. Show all posts
Showing posts with label sedimentology. Show all posts
Wednesday, February 17, 2010
Monday, February 15, 2010
Sediment Transport / Shields Curve
Although the experimental work and analysis were performed
by Shields, the curve termed the Shields Curve,
which is shown in Figure 9-1, was actually proposed by
Rouse (ASCE 1975). Shields curve may be expressed as
an equation, which is useful for computer programming.
I'm sure there was probably some obscure notation of Rouse in one of my textbooks, but I must have overlooked it or this would not have been a bit of a surprise to me. I looked up Rouse and discovered that he, in fact, was given little to no credit for his work. When Rouse introduced the Shields diagram, he did so with auxillary parameters. You can read more on this here.
The images to the left are that of a Shields diagram and correlating equation. (culled from EM 1110-2-4000). It's a widely used method of computation or anything other than very small Reynolds numbers, otherwise other empirical expressions are utilized. For general purposes though, the Shields diagram is a good starting point.
Further into the manual there is a section on Bank or Wall Shear Stress. Brownlie's approach appears to be the favored method, and the section is fairly well written describing the resistance equations and range of conditions. Duboy's concept where the significant assumption being that sediment
transport could be calculated using average cross-section
[hydraulic] parameters and that the main result of excess shear stress was transport of said sediment. (EM 1110-2-4000). There are a few more equations in this section, some of while were derived from Einstein, which I found interesting. Mostly because when I think of Einstein, I associate him with theoretical physics.
transport could be calculated using average cross-section
[hydraulic] parameters and that the main result of excess shear stress was transport of said sediment. (EM 1110-2-4000). There are a few more equations in this section, some of while were derived from Einstein, which I found interesting. Mostly because when I think of Einstein, I associate him with theoretical physics.
I was curious as to what other methods were implemented in calculating shear stresses in banks or walls, so I did yet another internet search. This one yielded quite a bit of interesting reading material. One of which was a paper pretty much dedicated to hydraulic shear stresses, with several different environments/situations outlined and the correlating equations: Shear Stress in Bends
Flow around bends creates secondary currents that exert higher shear forces on the channel bed
and banks than those found in straight sections. Several techniques are available for estimating
shear stress in bends. A relatively simple and widely used method, presented by U. S. Department of Transportation,2 estimates maximum shear stress on channel banks and bed occurring within bends. This equation, however, does not differentiate between bank and bed shear stress. The maximum bed/bank shear stress is primarily focused on the bank and bed on the outside portion of the bend .
Lastly was a link to a book on google books. This book, Introduction to bed, bank, and shore protection- by Gerrit J. Schiereck is by far the best [mathematically-heavy] book I have ever read. While I did not read the entire book, what I did read was so well written I forgot for a moment I was reading about math. In general, I like math, but it can be a love/hate relationship for me. I don't like to have to figure out what a writer is blundering through in addition to understanding the formulas. With this book you don't have to do that. The man is an artist, truly. When you can become so absorbed in what you are reading because they have grabbed your attention AND know how to write eloquently- well that is a book you just have to buy. So I did! You can catch a B&N link to it here, but it appears I bought the last copy. (At least I hope that is the case- my order went through, but you never know. I'll have to check my email when I finish up with this). The figure (Fig. 3.1, forces on a grain flow) at the beginning of this post comes from a section of his book.
On page 52 of the google book Schiereck describes Shield's formula for uniform flow, and how it isn't always the best choice. He explains why using shear stress as the active force this isn't always the best choice. On p. 65 he goes in to describe another environment (a dam or a groyne ) where you can use Shields eq. in conjunction with a slope correction. If you have time, read p. 72-73, as the part about geotextiles particularly is interesting.
Sources:
Introduction to bed, bank, and shore protection- by Gerrit J. Schiereck
Shear Stress in Bends
USACE EM 1110-2-4000
Rouse and Shield
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Introduction to bed, bank, and shore protection- by Gerrit J. Schiereck
Shear Stress in Bends
USACE EM 1110-2-4000
Rouse and Shield
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Saturday, February 6, 2010
Bedforms and Cross-Bedding
It has been several years since I have had sed/strat, and when I chanced across this webpage I was struck with the thought that it would have been a nice (scratch that, AWESOME) resource to have had during that course. It is via the USGS - not sure how I could have missed it, as it was an active site at the time of my course. I think perhaps the title was such that I mentally discounted it as useful because it says 'Western Coastal and Marine Geology'. However, this animation set they have is applicable to all coastal environments/paleocurrents. It (the site) is truly a masterpiece of work, and a lot of time and effort went into its development.
As those of us who have gone through a sed/strat class, it can (at times) be daunting to learn the associations between bedforms, cross-bedding, and environments. It isn't so much the absorption of knowledge that hangs a lot of us up, but rather looking at an outcrop or rock sample and associating the type of cross-bedding it exhibits. Even when I had that part pretty well mastered (of which at this present time I have only vague memories, hence my personal reason for appreciating this website) it was still difficult to visualize the environment in action. This is why these animations are so fantastic to look through!
To compliment the animations, there are detailed explanations on how to classify bedforms; transverse, oblique, or longitudinal, via various mathematical computations. Considering the aspect of unknown variables, implementing the wrong formula can produce less than desirable results. This paper explains certain pitfalls, and how they can be precluded in order for all variables to be considered.
Relations between cross-bedding, bedforms, and flow as well as two dimensional bedforms/cross-bedding are also touched upon via pdf files. The real gem of the website was refreshing my memory on the different bedding types and how they develop. I had intended upon adding more to this post, but I lost myself in browsing the site as I was composing this blog and now am too short on time. I mainly just wanted to share resource I had found, if you had not already discovered it yourself. (I may be behind the powercurve in regards to that ;0)
.
Sources:
http://walrus.wr.usgs.gov/seds/bedforms/info_panels/infoPanel5.pdf
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As those of us who have gone through a sed/strat class, it can (at times) be daunting to learn the associations between bedforms, cross-bedding, and environments. It isn't so much the absorption of knowledge that hangs a lot of us up, but rather looking at an outcrop or rock sample and associating the type of cross-bedding it exhibits. Even when I had that part pretty well mastered (of which at this present time I have only vague memories, hence my personal reason for appreciating this website) it was still difficult to visualize the environment in action. This is why these animations are so fantastic to look through!
To compliment the animations, there are detailed explanations on how to classify bedforms; transverse, oblique, or longitudinal, via various mathematical computations. Considering the aspect of unknown variables, implementing the wrong formula can produce less than desirable results. This paper explains certain pitfalls, and how they can be precluded in order for all variables to be considered.
Conceptually,the approach is to determine the unique transport vector that simultaneously would cause the observed migration of two sets of bedforms. Algebraically, this is accomplished by solving equation (2) simultaneously for the transport represented by two sets of bedforms. The solution is given by
Equation (3) can also be applied to a single set of bedforms, if they are three-dimensional. In such a situation, β is equal to 90°, V2 is the along-crest migration speed of the plan-form sinuosities, and H2 is the mean height of the bedforms meassured along profiles parallel to the generalized trend of the bedforms. In the computer-generated depositional situations, H2 was measured from contour maps of the bedform topogrraphy. Although equation (3) cannot be used with perfectly two-dimensional computer-generated bedforms, most real bedforms, including many that would be considered two-dimensional, are probably three-dimensional enough to use this approach.
Relations between cross-bedding, bedforms, and flow as well as two dimensional bedforms/cross-bedding are also touched upon via pdf files. The real gem of the website was refreshing my memory on the different bedding types and how they develop. I had intended upon adding more to this post, but I lost myself in browsing the site as I was composing this blog and now am too short on time. I mainly just wanted to share resource I had found, if you had not already discovered it yourself. (I may be behind the powercurve in regards to that ;0)
.
Sources:
http://walrus.wr.usgs.gov/seds/bedforms/info_panels/infoPanel5.pdf
.
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