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DEPOSITIONAL ENVIRONMENTS
1. INTRODUCTION
1.1 What does a sedimentologist mean by environment of deposition? The concept is not as easy to define as you might think. Basically, what the conditions were at the site of deposition. This is usually viewed in terms of an overall geographical complex or entity that has a characteristic set of conditions , like a river or a beach—but see below.
1.2 The term environment is really used in two different ways:
THE environment: the aggregate or complex of physical and/or chemical and/or biological conditions that exist or prevail at a given point or in a given local area at a given time or for a period of time. AN environment: a distinctive kind of geographic setting characterized by a distinctive set of physical and/or chemical and/or biological conditions.
1.3 Important: you can go out and look at all the surface environments in the modern world to help you in your depositional interpretations, but you should keep in mind that only a small subset of environments (on land, that is) are depositional environments : most are erosional environments, and they won’t help you much (and maybe even mislead you badly) about depositional environments. The somewhat strange word actualistic is used in geology to describe situations or processes that are represented on the Earth today, as opposed to non-actualistic ones, which are interpreted to have existed at a particular time or times in the past but are not represented on the modern Earth.
1.4 Table 10-1 shows a fairly detailed list of depositional environments. There are various problems with this list:
- There’s lots of overlap among the different environments.
- It’s still not a complete list.
- Some of the environments on the list have been much more common and important in the sedimentary record than others.
- The divisions are not entirely natural.
- The extremely important effect of tectonic setting is taken into account to some extent but seriously inadequately.
2. MAKING INTERPRETATIONS
2.1 Here’s a seemingly obvious but important point: interpreting depositional environments involves interpretation. You take note of objectively observable things in the rocks, and then you use your knowledge, your experience, and your intuition to make interpretations, specific or general. You can be right in your observations and wrong in your interpretations, and you’re not doing any great damage. But if you are wrong in your observations, you are not going to be right in your interpretations.
2.2 Don’t make the mistake of mixing up observation and interpretation. Don’t walk up to an outcrop and call the rock a beach sandstone or a point-bar sandstone. First of all, describe it , and then add an interpretation if you want to.
2.3 At the risk of being too synthetic, I’ll point out that two kinds of interpretation are possible (although they are not entirely distinct):
Interpret specific conditions at a point in space and time. Example: look at geometry of cross stratification and say something about current velocity. Interpret general conditions in a local area with time , in the framework of broad kinds of depositional environments you think you understand. Example: Look a sandstone–shale succession and decide that it represents deposits of a large meandering river.
2.4 Here’s a list of what you can look for in a sediment rock or a sedimentary bed that might tell you something about depositional environment:
grain size grain shape grain surface texture grain fabric sedimentary structures composition (siliciclastic; carbonate, evaporite, coal, chert) fossils (body fossils, trace fossils) stratification sequence sediment-body geometry/architecture
2.5 What are environmental interpretations based on? Three different kinds of things, basically:
- Study of modern environments
- Inferences about the results of known sedimentary processes
- Deductions about the causes of features seen in the ancient
3.5 How do you deal with facies on the outcrop? At the risk of being too prescriptive or “cookbookish”, here is a set of steps you might take:
- Cruise up and down the section a few times, slowly, examining it bed by bed.
- Let ideas about facies grow in you mind.
- Develop a tentative list of facies.
- Refine the list by looking at the section again.
- Describe your facies.
- Record the vertical succession of facies in the section, in case that might reveal some characteristic kind of upward transition.
- Think carefully about the environmental significance of the facies and their succession.
3.6 This is a good place to say something about facies models or depositional models (and make a warning about their use). Over the years, various general models of how certain depositional environments work have been developed. This involves a distillation of the facies and facies successions in a number of related environmental settings into a widely applicable model, which, with variations, helps you to categorize your own section.
3.7 The danger about facies models is that only a few have been well worked out, and you may end up trying to fit your square-peg depositional environment into a round-hole facies model, and doing more harm than good.
4. MARINE OR NONMARINE?
4.1 The broadest, and probably the most important, question of environmental interpretation that confronts you when you look at rocks is this: Are the rocks marine or nonmarine? If you don’t know that, how can you speculate about specific settings? Below are some guidelines for your consideration. Again I don’t want to be too cookbookish about this, but an annotated list seems advisable. None of the items on this list is infallible (although the first is about as close to it as you're going to get in sedimentology); consider these items to be pieces of evidence that can sway your opinion, without really proving anything.
Marine fossils Your best bet is to find marine fossils. Of course you might ask: How does one know that fossils considered marine fossils really represent organisms that lived in the ocean? You can safely consider that to be a settled matter. Then it’s up to you to identify the fossils. Don’t forget that trace fossils are as useful as
body fossils in this regard. You usually don’t have to worry about marine fossils being reworked from earlier deposits and incorporated into a nonmarine deposit, and vice versa, although it’s possible.
Carbonate rocks There are some fresh-water limestones around (and some fresh-water dolostones, too), but most of the carbonate rocks you are likely to see are marine. This is a suggestive piece of evidence, but clearly it’s not definitive.
Red beds Red beds are rocks (usually sandstone–shale successions) in which at least the finer sediments, if not the coarser, contain a small percentage of hematite, a potent rock pigment that imparts the characteristic red color. The origin of the hematite pigment has been controversial, but it’s widely agreed that the iron gets in the sediment at the time of burial detritally as hydrous ferric oxides which later, during early diagenesis, get converted to hematite, provided that there is not so much organic matter to be oxidized that the iron ends up in the ferrous state. That’s far more likely to happen in nonmarine, especially fluvial, environments than in marine environments, so red beds are good suggestive evidence of nonmarine deposition. But again there are important exceptions.
Evaporite chemistry If your succession contains evaporite minerals, you can often make a good case for marine or nonmarine on the basis of the suite of evaporite minerals present. As you learned in the earlier chapter on evaporites, the ionic composition of sea water changes very little, so there’s a rigorous regularity in the evaporite minerals formed. On the other hand, evaporites in nonmarine basins, which usually have closed drainage, can vary widely in their chemical composition, because the salt content depends atr least in part on what’s weathered out of the particular source rocks and carried into the basin.
5. PALEOFLOW INTERPRETATION
5.1 Probably the most important kind of specific environmental interpretation you can try to make is to figure out the nature of the depositing fluid flow. (Most. but not all, sediments are deposited by flowing fluids.) This deals with some possibilities for making paleoflow interpretations by examining ancient clastic sedimentary sequences. When such interpretations can be made, they serve as guides or constraints in framing a broader picture of the depositional environment. The possibilities for making such interpretations are numerous and varied, but nonetheless they are still limited_._ Further work is going to reveal a lot of useful interpretive approaches based on features of beds we still don’t know how to interpret.
5.6 This would be as good point at which to go back to the earlier chapters on particle size and, especially, on bed forms and stratification to review the potential “fodder” for paleoflow interpretations. Below are just two additional matters that you should be aware of.
cross stratification: It is all to easy to walk up to an outcrop with a cross- stratified bed and measure the direction of dip of the cross-strata, and then assume that the result is a good indication of the overall paleoflow direction. The problem is that in most cases the geometry of the cross sets is far from being uniformly dipping planar strata. You saw that in the earlier sections on small-scale trough cross-stratification and large-scale cross stratification generated by the movement of three-dimensional dunes. At the very least, you need to take a large number of dip measurements in a way that is unbiased by the geometry of the outcrop surface itself—commonly an impossible task in practice. Rib and furrow, although uncommon to see in outcrop, is the very best way of obtaining a paleoflow measurement from cross stratification.
parting lineation: Commonly, when a sandstone parts along a stratification plane, there is a subtle (or often not so subtle) “grain” or anisotropy of the parting surface, in the form of irregular steps, all approximately parallel, and usually only a fraction of a millimeter in height, which reflects an anisotropy in rock strength caused by preferential alignment of the sand grains parallel to the paleoflow. It’s is often called, alternatively and more accurately, parting-step lineation. Presumably, it’s a reflection of upper-regime plane-bed transport.
PART II. SPECIFIC ENVIRONMENTS
1. FLUVIAL ENVIRONMENTS
1.1 Introduction 1.1.1 Rivers are the main routes by which sediment derived from weathering on the continents reaches the ocean. (Remember that this sediment includes dissolved material as well as particulate material; the discussion here deals only with the particulate material.) Most of this sediment indeed reaches the ocean, but a certain smaller percentage is deposited either within the rivers themselves or where rivers end in basins of interior drainage.
1.1.2 In a sense such storage is temporary, in that it eventually is remobilized in a later geologic cycle, but commonly it is stored for geologically long times, tens to hundreds of millions of years and sometimes even billions of years—long enough for it to be deeply buried and lithified, even metamorphosed.
1.1.3 Rivers are enormously varied, in size, geometry, and dynamics. When someone speaks of rivers to you, what image comes to your mind? A rushing mountain stream? The broad and placid Mississippi? These are only two of a great many common manifestations of rivers. So it should not surprise you that fluvial sediments and sedimentary rocks are highly varied as well.
1.1.4 It’s usually considered that most rivers are either meandering or braided; straight rivers are not very common. But meandering and braiding are not mutually exclusive tendencies: either or both can be in evidence in a given river, with each with varying degrees of prominence. And both meandering and braiding show great diversity. This should suggest to you that it's not easy to compartmentalize the sedimentological behavior of rivers into a few neat models.
1.1.5 Meandering rivers lend themselves to fairly easy description or characterization, and a widely accepted facies model for the deposits of meandering rivers has been around for a long time. Braided rivers are much more variable and less easy to characterize; there have been attempts to develop facies models for braided rivers, but these have not been nearly as successful or widely used as the meandering model.
1.1.6 This is not the place to present an account of the dynamics and geomorphology of rivers, although I want you to appreciate that understanding of the geomorphology of rivers is crucial to understanding and interpretation of fluvial deposits. The major factor in how a fluvial deposit looks is the geomorphology of the river: the arrangement of channels and overbank areas, and how they change with time during slow buildup of the floodplain. All I’ll do here is present some basic things about fluvial deposition and fluvial deposits, and then outline the meandering fluvial model, with appropriate caveats on its application.
1.1.7 Keep in mind that the same problem of the modern versus the ancient that holds for marine deposits holds for fluvial deposits as well: It’s relatively easy to study sediment movement and disposition in modern rivers, but it’s rather difficult to study the vertical sequence of deposits, because of the generally high water table. In ancient rocks, on the other hand, it’s easy to study the vertical sequence of deposits, but it’s usually impossible to establish the geomorphology of the depositing river itself.
1.2 Why Are There Fluvial Deposits? 1.2.1 It’s not obvious why fluvial deposits are an important part of the ancient sedimentary record. After all, rivers drain areas of the continents that are undergoing erosion. It’s true that most rivers, except the smallest, are alluvial rivers: they have a bed, and a floodplain, composed of their own sediments. But in most cases this alluvial valley sediment isn’t very thick. Only in certain cases does the alluvial valley fill become thicker.
1.3 How Do You Know It’s Fluvial? 1.3.1 By what criteria might you tell that a sedimentary sequence is fluvial? Here are some, but remember that none is incontrovertible, because each applies to other environments as well.
absence of marine fossils presence of plant fossils red beds scoured channels unidirectional-flow cross-stratification broadly unidirectional paleocurrents paleosols desiccation cracks plant fossils
1.4 The Meandering-River Facies Model 1.4.1 Rivers carry mud, sand, and gravel. In meandering rivers, sand (and some gravel) is stored in channel beds and especially in point bars, and mud is stored in floodplains. So meandering-river deposits end up as large sand bodies, shaped like lenses and shoestrings, partly connected but often mostly isolated from one another, enclosed in mud. (In braided rivers, sand and gravel in various proportions becomes interbedded very irregularly in lenses, sheets, and channels as the individual anabranches of the stream system shift irregularly and leave bars and islands.) Figure 10-3; Walker, R.G., and Cant, D.J., 1984, Sandy fluvial systems, in Walker, R.G., ed., Facies Models, Second Edition: Geological Association of Canada, Geoscience Canada Reprint Series 1, 317 p. (Figure 1, p. 72); shows a simplified sketch of the plan-view arrangement of a typical meandering river.
1.4.2 With time, an individual meander loop tends to become "loopier" or more accentuated by outward progradation of the point bar and erosion along the concave or outer bank. At the same time the entire meander loop tends to shift downvalley. Often you can see low curving ridges, called meander scars or meander scrolls , inside the meander loop that record the earlier positions of the point bar.
1.4.3 As time goes one, the meander loop also narrows at its neck. Eventually during some flood the river breaches the neck and straightens itself by establishing a new course across the neck, thereby abandoning the meander loop. This process is called neck cutoff. The ends of the abandoned loop soon become plugged by fine sediment to form an oxbow lake. The floodplains of meandering
rivers show a complex pattern of several generations of truncated meander scars and partly or wholly filled oxbow lakes recording a long history of meandering. 1.4.4 Every now and then, probably during a really big flood, the river breaks out completely from its meander belt to reestablish its course along some distant lower part of its floodplain, leaving the entire meander belt to be eventually filled and covered by fine floodplain sediment. Such a catastrophic change in course is called avulsion. 1.4.5 In a subsiding reach of a meandering river, the shifting and abandonment of meander loops (and, every now and then, of the whole meander belt) leads to a characteristic vertical arrangement of sand bodies encased in floodplain muds. This is because the sand carried in the main channel is deposited on the sloping surfaces of the point bars as they accrete laterally, and is then left as an irregular but not grossly inequidimensional mass whose thickness is about the same as that of the bankfull depth of the river. Such deposits are called lateral- accretion deposits (Figure 10-4).
Figure by MIT OCW.
Figure 10-4: Cross section through a point bar, normal to the local course of the river
1.4.6 Sometimes you see a kind of large-scale low-angle cross stratification, reflecting the channelward slope of the point-bar surface, produced by the episodic accretion onto the point bar-surface (it’s called, infelicitously, epsilon cross stratification ), but usually such cross stratification is masked by the smaller-scale structures (planar lamination and especially large-scale cross stratification) produced by sediment movement on the point-bar surface. 1.4.7 As the channels shift to leave point-bar sand bodies while the floodplain gradually builds up by deposition of muds (called vertical-accretion deposits ), a characteristic three-dimensional arrangement of sand bodies surrounded by muds is formed. The geometry of such a fluvial deposit is termed alluvial architecture. Figure 10-5 is a simplified sketch.
POINT-BAR SAND
FLOODPLAIN MUD
sediment, whereas the presence of sediment is essential to the existence of sediment gravity flows.
2.1.3 Another sticky point about the definition is that in grain flows, universally considered to be one kind of sediment gravity flow, a sheared dispersion of sediment particles moves downslope under the pull of gravity without the necessary presence of fluid at all , either interstitial or supernatant. There can be grain flows even in a vacuum! But for almost all the sediment gravity flows of sedimentological interest, the concept is clear and useful.
2.1.4 Relatively small turbidity currents have been observed and studied in lakes and reservoirs since late in the nineteenth century, but the existence of large marine turbidity currents came to light only by deductions made by geologists about features seen in the ancient sedimentary record. Soon after the existence of large marine turbidity currents was hypothesized, instances of their occurrence in recent times were recognized and studied, and small-scale laboratory experiments (mainly by geologists!) to study their motion and deposits, together with the evidence from the ancient, convinced most geologists of their existence and importance. Interpretation of turbidity-current deposits was well established by the early 1960s.
2.1.5 Recognition of more “exotic” sediment gravity flows, which would generally be classified as submarine debris flows , was longer in coming. Although subaerial debris flows were well known, it was not until the 1970s that the concept of submarine debris flows was widely invoked to explain the coarse, poorly sorted, and seemingly deep-marine deposits so common in the sedimentary record. Even now our understanding of the dynamics and depositional effects of debris flows does not match that of turbidity currents. Many important questions, among them the following, remain unresolved:
- What’s the nature of flows transitional between turbidity currents and debris flows?
- At what rate do sediment gravity flows lose sediment by deposition as they move?
- How does one distinguish between slowly deposited and rapidly deposited sediment-gravity-flow deposits?
- More generally, how does one interpret the nature of the sediment gravity flow from the record of the deposit?
2.2 Dynamics 2.2.1 This is not the place for detailed consideration of the dynamics of sediment gravity flows; I’ll just make some brief comments. Sediment gravity flows are generated, flow for some distance, and eventually dissipate by
deposition of the sediment. The origin of sediment gravity flows is their least well understood aspect: one has to appeal to the existence of unstable sediment resting on some slope, and its mobilization by either spontaneous failure or some sudden or cyclic disturbance like shaking by an earthquake or repeated loading and unloading by passage of surface water waves. If the sediment is sufficiently rich in water, liquefaction by rearrangement of grain packing can provide mobility without introduction of additional water, but for the thinner kinds of sediment gravity flows one might have to invoke initial incorporation of water from above as the movement starts.
2.2.2 Sediment gravity flows accelerate and then decelerate again, but for most of their history this acceleration and deceleration is small, and the motion is nearly uniform. There is thus an approximate balance between the driving force, the downslope component of the excess weight per unit volume of the mixture, and a resisting frictional force, exerted mainly by the substrate on the bottom of the flow but also by the overlying fluid on the top of the flow.
2.2.3 The motion of sediment gravity flows, described briefly below, is an outcome of the interplay among three factors: the downslope component of excess weight, which acts throughout the flow; the resisting forces exerted at the upper and lower surfaces; and the local resistive properties of the mixture, which can be characterized, approximately at least, by its viscosity (to the extent that it behaves as a fluid) and its shear strength (to the extent that it behaves as a plastic). Except in a very simplified way, it’s not even possible to write down the governing equations of motion, let alone solve them, largely because of the problem of deciding upon the basic mechanical nature of the material in order to write down what are called the constitutive equations, which relate the deformation to the applied stress. So any treatment of the motions of sediment gravity flows, overall and internal, must still be semiquantitative at best.
2.3 Classification 2.3.1 Classification of sediment gravity flows is based on the nature of the mechanism or mechanisms by which the sediment is kept supported in the flow. There are considered to be four such mechanisms:
fluid turbulence matrix strength dispersive grain collisions fluidization
2.4 Motion 2.4.1 All the sediment gravity flows I have seen, or have seen movies of, have a fairly well defined head or front , where the flow is thickest and where velocities are highest, and a long body , and a tail , where velocities are lower (Figure 10-7; Walker, R.G., 1984, Turbidites and associated coarse clastic deposits, in Walker, R.G., ed., Facies Models, Second Edition: Geological Association of Canada, Geoscience Canada Reprint Series 1, 317 p. (Figure 1, p. 171)). The implication of this is that sediment gravity flows tend to be dispersive: the head outruns the tail, and the flow stretches out and becomes more diffuse as it flows. Debris flows sometimes show pulses of more active movement along their length: the flow thins and slows or even stops for a while, and then thickens and speeds up again as a pulse from upstream moves by.
2.4.2 Sediment gravity flows may at first incorporate more sediment, by erosion of the substrate, but even if they do (and presumably some are depositional almost from the beginning), when they reach a gentler slope they eventually lose sediment by deposition and therefore weaken. The velocity picture in sediment gravity flows is thus complicated: velocity varies both along the flow at a given time, and with time at any point that’s followed along with the flow. Of course, at any point on the bottom the velocity increases and then decreases as the flow passes by.
2.4.3 The state of internal motion in sediment gravity flows is complex and varied. The low-concentration kinds of sediment gravity flows, like turbidity currents, are certainly turbulent , whereas the higher-concentration kinds of sediment gravity flows, like debris flows, tend to be laminar. Relatively low- concentration sediment gravity flows behave approximately as Newtonian fluids, but relatively high-concentration sediment gravity flows must be non-Newtonian; in fact, very high-concentration flows are thought to have matrix strength (meaning that the applied shear stress must reach a certain value before the mixture starts to deform by shearing ), so they may behave as plastics.
2.4.4 Matrix strength is significant for the flow behavior of debris flows: in the interior of the flow, where shear is least, there is likely to be a rigid plug , and as the flow decelerates and the shear within the flow becomes weaker, the rigid- plug zone expands upward and downward, until the flow grinds to a halt by total rigidification. Many lower-concentration debris flows can be seen to be turbulent, however, so matrix strength must be a much less important effect in them.
2.5 Sediment-Gravity-Flow Deposits 2.5.1 Features. —Most sediment-gravity-flow deposits are event beds : relatively coarse beds, sandstones or conglomerates, underlain and overlain by finer deposits, siltstones and mudstones. They are mostly marine, although lacustrine sediment-gravity-flow deposits are of non-negligible importance.
2.5.2 The lower contacts of sediment-gravity-flow beds are almost always sharp, and often erosional, reflecting the initially very strong current. Upper contacts are usually gradational, although the gradation is often complete over a small thickness, of the order of a centimeter. Normal grading is characteristic of turbidity-current deposits, reflecting temporal decrease in current velocity, and therefore size of sediment carried. Inverse grading is common at the base of both turbidity-current deposits and debris-flow deposits; the mechanics of its development is not clear.
2.5.3 Thickness of sediment-gravity-flow deposits ranges from a few millimeters, in the case of feather-edge distal turbidites, to well over ten meters, in the case of deposits from the largest debris flows or flows intermediate between turbidity currents and debris flows.
2.5.4 Sediment-gravity-flow deposits range from well stratified (as in most turbidity-current deposits), to wholly nonstratified (as in many debris-flow deposits). Structures range from nonstratified through parallel-laminated to cross- stratified, usually but not always on a fairly small scale; soft-sediment deformation is common as well. Because sediment-gravity-flow deposits are deposited rapidly, you might expect them to have rather loose packing and excess pore water; dewatering structures, mainly dish structures and vertical pipelike structures, are common.
2.5.5 Interpretation .—How do you know that you are dealing with a sediment-gravity-flow deposit? Remember that it’s always an interpretation, because it’s a matter of genesis rather than just description. You have to use some or all of the above features, and more, to make that kind of interpretation on the outcrop. The broader stratigraphic context (what’s the overall nature of the section?) is also useful in making such an interpretation. You need practice on the outcrop.
2.5.6 The Bouma Sequence. —Working on turbidites in Spain in the late 1950s, the Dutch (now American) sedimentologist Arnold Bouma perceived a characteristic vertical sequence of sedimentary structures in turbidites , which he thought to reflect the temporal sequence of depositional conditions at a point on the bed as the turbidity current flowed by and deposited sediment from a waning current. Since then this sequence has been called the Bouma sequence. (It’s unusual for someone to be so immortalized even before one's death!) The distinctive parts of this sequence are called divisions ; Bouma designated them A through E.
2.5.7 Figure 10-8; Walker, R.G., 1984, Turbidites and associated coarse clastic deposits, in Walker, RG., ed., Facies Models, Second Edition: Geological Association of Canada, Geoscience Canada Reprint Series 1, 317 p. (Figure 4, p. 173); is a sketch of a representative turbidite showing a complete Bouma sequence, followed by a brief account of the genesis of the various divisions, according to modern interpretation.
2.5.10 A particularly important example of the foregoing point is this: one often sees thin but coarse sediment-gravity-flow beds showing evidence of strong traction in the form of planar lamination. The natural assumption is that such beds record passage of strong turbidity currents through channels in the proximal to intermediate environment, with each turbidity current leaving little or even no deposit. In such situations large-scale cross stratification, so uncommon in “classical” turbidites, is not uncommon as well. One assumes that the sediment (presumably abundant) that passed by the given point was deposited as thicker but finer beds downslope.
6.5.11 Submarine Fans. —It stands to reason that the deposit formed by repeated sediment-gravity-flow depositional events at the base of a submarine (or lacustrine) slope would be broadly fan-shaped or cone-shaped —although outcrop in the ancient is seldom if ever good enough to pin down the three-dimensional geometry of the fan. On the other hand, submarine fans, large and small, are well known in the modern; marine geologists have been studying their geometry and surface sediment for many years. (But it’s almost as difficult to study the thick vertical succession of deposits in a modern fan as it is to study the geometry of an ancient fan.) Nowadays, sophisticated seismic reflection techniques allow great insight into the innards of deeply buried submarine fans
2.5.12 During the 1970s, Italian sedimentologists were active in developing a model for the deposition of sediment-gravity-flow deposits as submarine fans. That work drew mainly upon studies in the ancient, but other sedimentologists later integrated that model with what’s known about modern fans.
2.5.13 Keep in mind that, as with any depositional models, application of the submarine-fan model involves a certain leap of faith, because there’s nothing from the outcrop that tells you directly that you are dealing with a fan, only indirectly.
2.5.14 How do submarine fans operate? There is good evidence from the modern that the sediment gravity flows are usually carried by a network of distributary channels, which change and shift irregularly with time (Figure 10-9; Stow, D.A.V., Reading, H.G., and Collinson, J.D.,, Deep Seas, in Reading, H.G., ed., Sedimentary Envbironments; Processes, Facies and Stratigraphy, Third Edition: Blackwell Science, 688 p. (Figure 10.46, p. 430, and Figure 10.51, p. 432)). Some aspects of this change are closely analogous to meandering of surface rivers, and some aspects are closely analogous to braiding of surface rivers. The essential similarity between alluvial fans and submarine fans is that upbuilding is localized on one part of the fan for a long while, until the channelized flow breaks out at some point to seek a lower elevation on some other part of the fan that hasn't been active for a long time.
2.5.15 The irregular shifting of distributary channels on a fan surface gives rise to a signal in the event-bed succession, whereby some parts of the section consist mostly or entirely of coarse event beds (this represents the active upbuilding of the fan by the channelized flow) and other parts of the section
consist mostly of finer background deposits (this represents interchannel or overbank deposition away from the areas of active upbuilding by channelized flow).
2.5.16 Packets of event beds in the submarine-fan setting often show a tendency, subtle or pronounced, for thickening and coarsening upward, or thinning and fining upward. Such packets are typically several meters to a few tens of meters thick. The model accounts for this by assuming that as a new area of the fan is being constructed, the event beds become thicker and coarser for two reasons: the new distributary channel gathers discharge slowly, and the local environment becomes more proximal as the deposit progrades. On the other hand, if flow in a given distributary channel is gradually choked off, the sequence of event beds would show a tendency to be thinner and finer upward.
2.5.17 The submarine fan model has been refined to the point where many sub-environments are recognized. I won’t elaborate except to mention three such sub-environments;
- The basin plain , the most distal environment, where the waning sediment gravity flows are no longer strongly channelized but can spread widely to the side, to leave beds that are traceable for long distances in two lateral directions, not just one.
- Throughput channels , where strong sediment gravity flows in fairly proximal positions transport large quantities of sediment past a given reach but leave little or no thickness of sediment. It’s in such environments that thin, coarse, and amalgamated sediment-gravity-flow deposits are common.
- Overbank areas lying adjacent to active distributary channels, where especially large flow events spill over the channel banks to deposit finer suspended sediment (silts and fine sands) from currents of moderate velocities to build broad natural levees.
3. OPEN SHALLOW MARINE DEPOSITS
3.1 Introduction 3.1.1 Today several percent of the area of the world’s oceans is floored by the continental shelves : the submerged shallow margins of the continents. Water depths are seldom greater than about 200 m even at the shelf edge, and relief is subdued, except where submarine canyons cut into the shelf. Widths range up to a few hundred kilometers. Average bottom slopes are so small that if they drained the ocean and parachuted you blindfolded onto the middle of the continental shelf, you wouldn’t know which way to walk to get back home, just from the lay of the land.
3.1.2 The total area of continental shelves in the world is a very sensitive function of world sea level, because along tectonically stable, passive-margin
