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WATER DEPTH OF MUD TRANSPORT AND DEPOSITION  73
            age range of fossils is often too broad to age‐date stratigraphic   Schieber and Southard, 2009) have demonstrated that
            surfaces or intervals that formed during relatively short‐lived   flocculation of clay‐size particles occurs in the laboratory
            cycles, usually precluding the ability to definitively correlate   and in nature which provides floccules large enough to be
            strata within a high‐frequency, time‐stratigraphic framework.   transported by currents (i.e., hydraulically equivalent to silt
            Paleozoic shales can generally be resolved at third‐order   and sand size particles). Floccules have been preserved in
            cycles (~1–5 Myr duration) superimposed on a second‐order   many  Mesozoic  and  Paleozoic  shales  (O’Brien  and  Slatt,
            cycle (~10–30 Myr duration) (Fig. 4.1c). Owing to greater   1990; Slatt and  O’Brien, 2011). Hyperpycnite  muds have
            biostratigraphic resolution, Mesozoic and Cenozoic shales   been documented for the Cretaceous Lewis Shale (Soynika
            can be resolved at fourth‐order cycles (100,000–300,000   and Slatt, 2008) and other rocks in the Cretaceous western
            years duration) superimposed on a third‐order cycle, as   interior seaway deposits (Bhattacharya and MacEachern,
            demonstrated in the following.                       2009), as well as in the modern Sea of Japan, where a
                                                                 transport distance of 700 km has been documented for a
                                                                 hyperpycnal flows (Nakajima, 2006).
            4.4  WaTEr DEPTH OF muD TraNSPOrT                      It would seem that microfossils such as radiolarian and
            aND DEPOSITION                                       coccoliths might offer the best chance of deposition through
                                                                 the water column as individual particles (i.e., marine snow;
            It has long been assumed that because of their fine‐grained   Bennett et al., 1991) since they are not electrostatically
            nature, precursor muds were deposited in quiet, “relatively   charged, as are clay particles. However, even high concen­
            deep” ocean waters. More recent studies have shown that   trations of biogenic particles can move along the seabed and
            siliciclastic  muds  can be deposited  in  tidal  mud  flats   erode underlying mud (Abouelresh and Slatt, 2012a, b).
            (Rine and Ginsburg, 1985) and shelf to upper slope water   The presence of phosphate minerals in shales is often
            depths (Loucks and Ruppel, 2007) as well as in deep   attributed to upwelling currents.  The upwelling model
            basins. In addition to “hemipelagic settling” of mud parti­    proposes that cold, deep, oxygen‐deficient, phosphate‐rich
            cles, hyperpycnal flows (Bhattacharya and MacEachern,   water is drawn along the sea floor until it reaches the
            2009; Mulder and Chapron, 2011) and turbidites can also   continental slope, where it rises to the shelf edge. Organisms
            transport sediment from continental to shelf/slope/basin   thrive on the phosphate nutrients, and generate “algal
            environments;  storm  and  contour  currents can rework   blooms” (i.e., modern “red tides”) and further deplete
            mud deposited by these processes.                      dissolved oxygen, creating eutrophication of the water mass
              Many resource shales exhibit microsedimentary struc­  and deposition of the phosphates. A second model postulates
            tures such as graded beds, cross‐laminations, and cross‐beds,   that phytoplankton productivity is increased due to seasonal
            indicating current transport along the sea floor (Fig.  4.2)   nutrient input from continental weathering and runoff during
            (Abouelresh and Slatt, 2012a, b). Such transport requires   times of broad shallow seas (Lash and Blood, 2011; Rimmer
            particles larger than clay size, as these would tend to be   et al., 2004), particularly if the basin is silled (Molinares‐
            buoyed upward by a turbulent current. Schieber et al. (2007;   Blanco, 2013).




                         (a)                                                   (b)








                         (c)                       (d)                      (e)








            FIGurE 4.2  Thin section photographs of sedimentary structures in the Barnett Shale. (a) Irregular (erosional) bottom surface of a siliceous
            sponge spicule laminae. (b) Close‐up view of scour surface at base of light‐colored siltstone bed. (c) Ripple stratification, note the clay mate­
            rials (black) delineating the ripple marks. (d) Low‐angle cross lamination. (e) Hummocky lamination. Figures from Abouelresh and Slatt
            (2012a, b). Reprinted with permission of Central European Journal. Geosciences http://www.degruyter.com/
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