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00:01 Yeah. OK. All right. Again, lots of more references than

00:07 listed here. If you see a diagram or a topic that you're particularly

00:14 in. Look at the citation, if I put it in uh the

00:21 boulder, if not uh send me email and I'll send you the PDF

00:25 I have it. OK. Um You know, we talked about

00:37 with respect to coastal variables, those in influencing deltas are the same ones

00:44 influence tidal flats and barrier islands and plants. Um We could look at

00:53 as a list or we could think it. Kind of like a geophysicist

00:57 think about it as a flow chart uh sediment input and reservoir energy and

01:06 to get to the delta. We think about like a geologist might look

01:10 it. Uh The, the key is look at all the feedbacks and

01:15 how complex that ultimate system is that up providing the sediment input to that

01:25 uh to that standing body of OK. Uh And the influences that

01:34 variables that control the energy levels of standing body of water. OK.

01:40 we will talk about some though, not all of those. OK.

01:46 Early classifications were geom morph of uh elongate uh arguably strand plane.

01:57 The, the test of it here see was that beginning in the late

02:06 uh fisher from U T. Um , and colleagues began to think about

02:13 as being high destructive or high And again, the idea of being

02:20 relative to what Well, uh the between sediment input and we mainly wave

02:30 , sediment input is high. We elongate delta, sediment input is low

02:35 wave energy is high, high Uh Then they thought, oh,

02:39 , you know, maybe we ought add the influence of tides.

02:43 uh then we get this diagram that destructive wave influence, high destructive tide

02:51 . Bill Galloway also, uh was uh U T at the time then

03:00 out? Well, let's do this a triangle diagram. And this pretty

03:03 has remained the way we think about the delta classification, uh some relative

03:11 of sediment waves and energy. Now , you'll notice that shape of this

03:18 shape uh um was sometimes called an delta. Uh Walker said that's not

03:27 a delta, it's an estuary uh then stick out. Um We basically

03:34 that uh and the confusion is that dominated estuaries and tide dominated deltas do

03:43 look pretty simple. So, uh confusion is less real now staying along

03:51 triangular input, the most recent to into the classification for is say,

03:59 , you know, I, we that there are great L L

04:05 don't fall at the end. So have a vocabulary that allowed us to

04:14 where they fall. Uh And that's reasonable. And, and that's

04:19 particular classification has been adopted uh more than not. But then what about

04:28 type? Maybe we could add 1/4 . Um And then all of a

04:34 you got all these different kinds of different great planes and, and,

04:41 well, uh we give them that's quite true. But the difficulty

04:48 first of all, the different especially sediment and put added to the

04:53 is going to affect the morphology of del secondly, delta has changed through

05:00 . And thirdly, delta's um are show even lateral changes with short periods

05:11 time. I don't mean changing from stand to high stand, I mean

05:16 left to right. So this was of illustrated the difficulty of describing the

05:23 Delta On the Danube Delta over the couple of 1000 years or in the

05:29 I stand um would variably a wave river dominated delta. In fact,

05:37 pretty much today, you see Delta three and four are very different.

05:43 . Uh This is in spite of fact that there are no tides in

05:47 Black Sea. So we're only looking sediments fly and wave energy?

05:53 So where would that delta fall? in terms of, is this gonna

05:59 ? Well, I don't know, it, is it one place or

06:02 ? Is it kind of in the ? Uh And that's a hard

06:09 that's one of the complexities that we of dealing with deltas. Uh Also

06:15 you only had a few wealth. Would you describe this delta complex uh

06:23 a wave dominate. Delta river maybe a barrier island, uh maybe

06:29 the C delta. So these are problems that we have to reconcile.

06:37 it, it begins with looking at variability of modern deltas to anticipate the

06:46 that we might expect with ancient delta . Well, going back to uh

06:53 classification, um let's look at something might be right here big. Um

07:04 is an attempt to classify the Mitchell delta. And at first, it

07:11 looks pretty straightforward. But when we at the delta plain, uh it's

07:17 a lot of Southern das those environments tidal related thing. Uh tidal

07:26 tidal channels, tidal marshes, it wave and uh blue things like channel

07:37 bar, uh play lagoon film, beach ridges, abandon channel. Uh

07:47 just a lot of different things that here. And so here, then

07:55 , in this case, oh, looking at spits that are clearly wave

08:05 , but we're looking at tidal channels are here that are clearly tidal

08:11 And then the river channel itself is channel influenced to. So we need

08:16 figure out the relative percentage of the plane. It consists of different types

08:29 tide wave and river morphology. When do that, you can actually quantify

08:38 being 62% tides, 25% fluvial and weights. OK. Um Well,

08:49 is at least a quantitative approach to modern deltas. Uh But how do

08:58 go to the rock record? Here's a core and here you can

09:06 at the relative percentage of waved dominated doin. Well, wave generated tide

09:16 in fluvial, generated sedimentary structures. ? And that puts it way over

09:24 . OK. Now, the key is that we know at this point

09:31 types of sedimentary structures associated with the tides and rivers, OK.

09:40 cross strata, um waves, um bundles tide. So meandering bar deposits

09:52 bar deposits of two of you. we've already got the ability in mind

10:00 on the previous lectures to take a call and look at this pro grading

10:07 and say the relative percentage of species have been preserved through time because the

10:16 when we go back to here, is not the delta in as it

10:24 is the delta at a snap in . Some of these environments have a

10:30 lower preservation potential than others. And notice that if you looked at

10:39 face sheets, the surface deposits, . Her title. If you look

10:45 the rock record, most of what's is wave gene. OK. So

10:50 this tells us is that the deltas mixed. Um And we can look

11:03 a vertical section and or a cross and begin to take into account the

11:11 percentage of the sediments as preserved in context of the process that and these

11:20 examples of some of the things we look for all of which we've talked

11:25 before. So here's an example of lower Wilcox delta in core, looking

11:35 the core to figure out the relative of fluvial and title and wave generated

11:50 depending on where you are. So we're beginning to see this approach

11:57 to the ancient record and it's got distinct advantages. Uh And it's one

12:02 the ways of trying to get past members and figure out where in this

12:12 uh processes did this particular delta exists the period of time that it for

12:20 that it can change through time. with that in mind, let's think

12:25 the processes that impact deltas. There's the sediment coming in. Uh

12:35 that really is influenced by the water sediment discharge. Uh the percent suspended

12:41 grain size, seasonality, the density between the receiving base and the input

12:54 depth bottom slope and sediment type on bottle tidal range and associating currents and

13:03 wave energy and associated currents. So these are the things that we're

13:08 at. So we kind of lump of them together into buoyant forces.

13:14 buoyancy forces, frictional forces and inertial being the primary things that affect deposition

13:23 the mouth of the river. And ironically, tides and waves are

13:30 they important secondaries. But uh we're ignore them for just a couple of

13:36 . So what we're gonna do, gonna look at the relative densities of

13:42 incoming out like flows. We're and we're gonna look at Hypo uh

13:49 pal flows where the river is less than the receiving basin hyper where it's

13:59 dense and Homo where it's about the . Now, in the case of

14:04 Homo, pital flows, they tend be dominated by friction and void forces

14:10 the cases of the hyper petal flows by inertial forces as are. So

14:18 see what that might look like if trying to describe the dispersal set.

14:26 . The Hyper with more dance since on the bottom by, let's look

14:48 the hypericum for a second. Uh We're seeing it's floating and the

15:00 to which this plume is floating is to be a function of the buoyancy

15:05 here. And so experimental and field show that the mouth bar is a

15:17 where the cross sectional area of the is decreasing. So the flow is

15:30 to reach a maximum right here at bar crest. So we've got increasing

15:38 in the back of the bar maximum here and then decreasing down here.

15:46 so one of the things we're getting lower flow regime, upper flow

15:57 no, no regime. And notice we're actually talking about rude ducks.

16:07 that food number is the den meric number. Talk about it more.

16:14 , we mentioned it early on and is the oh inertial de buoyant forces

16:23 this flow here. And we've actually a hydraulic jump that's occurring going from

16:34 critical to sub critical. We get high energy. So most of the

16:39 uh is occurring at our crest now that plume is a buoyant plume.

16:51 and it doesn't feel the bottom There's not much friction here. It

16:56 to spread but not real fast because internal to this, we've got a

17:05 of got flow patterns that keep it flowing too widely or dispersing too

17:14 So at what happens is we've got tone of deposition here is the bar

17:25 and we've got kind of a funnel shaped here that's flanked by levies and

17:35 bar channel going into bar or the going into bar crest. We're gonna

17:43 this expressed differently. And I think when we look at uh some more

17:48 work, but this is just a because what it suggests is that in

17:54 hyper? I'm sorry. Um, hope it, don't saying it?

18:03 . Hi, Pope. Picked I get those confused even today.

18:10 , we have a crescentic bar levies because of that, if we look

18:21 the cross section through here, we that because the bar is scenic and

18:28 extend very far. It tends to us relatively confined for faces.

18:38 Now, what that means is that this plume. In fact, let's

18:44 at it here. This plume doesn't much. OK? Which means that

18:53 it extends, the sub aqueous levees sub aerial. So we've got levees

19:03 here that are gonna become sub aerial that bar crest will be limited to

19:10 area here. So in cross it's gonna be relatively confined la

19:20 So this is gonna be typical where have buoy and flow, especially a

19:26 of muds and deep water, deep because we wanna make sure that there's

19:34 interaction with the bottom. Ok. , consider something different where you have

19:45 water in the basin that's gonna be dominated. It's gonna spread laterally because

19:58 slowing down. The whole thing is as it slows down, it's dispersing

20:07 flow in all directions in distinct contrast that buoyancy quote. Now, the

20:17 result is you got the flow channelizing diverging and so you get it's more

20:28 middle ground bar in a lot of secondary bores again, we've got the

20:36 of sediment and greatest energy on the . But now look at the levees

20:41 beginning to display. So the Alya would be an example of that where

20:50 getting basically the shallow Alya Bay being receiving basin for the Fly River,

20:59 during floods because it wants to become Mississippi river. So we got a

21:05 bifurcation and as you might expect, gonna have a much wider sandy distribute

21:18 . OK. So we both can be hypo flow. It depends on

21:27 water depth to a large extent. is friction versus buoyancy dominated.

21:33 Well, muds tend to keep it in suspension, deep water keeps it

21:40 interacting with the bottom sands tend to lower in the water column. And

21:47 water means that there's more interaction with plot. OK. Now, even

21:55 that, we do begin to see influence of tides until finally, we

22:03 tis that become asymmetrical and we get linear tidal bars. So these river

22:11 bars, do them protic lo um one n member. Those linear tidal

22:25 I talked about uh are the other . So we'll talk more about these

22:33 . Now, an inertial dominated flow where there's more impact in slowing down

22:46 . This is deep water. It be hyper petals flow down and there's

22:51 spreading. OK. It's also decreasing , but it's not floating as

23:01 And so we get this um ex expansion. And the thought here was

23:11 that that is occurring when you had flu. It is to say that

23:20 was no a density Segre separation between incoming fluid which would tend to want

23:27 make it float. And the outlines um receiving basis for it.

23:35 Uh And that's why it expands And the other thought was that's gonna

23:42 us these Gilbert type deltas rapid deeper water, the over type.

23:52 . And that's shown here um for type deltas, I'm sorry down here

24:00 home. But we also get it hyper flow where we have so much

24:11 that uh rather, so much sediment that were slowing down the bottom.

24:25 we can get inertia dominating when it's down on the bottom is ect currents

24:33 we can get it when it's up top with home picked up. So

24:41 be looking especially at these various products we look at delta deposits.

24:50 more recently, we're looking at uh experiments. Uh I'm not gonna get

24:57 a lot of detail but notice how getting these elongated plums with narrow,

25:10 they increase levies. And this elongated , this bar is getting larger and

25:16 as it elongates. And this is couple of examples though, by the

25:21 we get down to here, notice more of a bar and even a

25:27 bar as it evolves uh with different this would be more um friction

25:38 more do it. So let's see , that we get when this channel

25:54 the standing body of water. Distribution channels, levies and the mouth

26:03 programing offshore. And we're gonna use Mississippi, not because it is the

26:08 typical of deltas, one of the , but simply because it is the

26:14 study. And if you recall, the study began when the L S

26:26 uh and uh coastal Research Center began the corps of engineers began studying the

26:35 River while they were studying the Mississippi and delta because the core is responsible

26:40 everything that's navigable. So They started the Mississippi River in the Mississippi

26:50 They started in the 40s and it's the best study delta we have.

26:55 let's look, first of all, one of the main tributaries or dis

27:00 rather. Here we have aqueous levee levee. Here we have an offshore

27:10 , kind of a protic offshore bar got a proximal part that we're gonna

27:18 the distributor mouth bars and a distal . And beyond that, we're gonna

27:25 a pro delta. And beyond that within that, we're gonna have some

27:31 these displays where there's remobilization by the delta nearby in the delta um

27:43 front. And we got winnowing by and storm waves, especially the

27:52 Winnowing is gonna be mainly the upper of the bar um storm waves will

27:59 the entire bar and you can get floods, increased pluvial deposits, giving

28:10 both these splays that are coming Think these may become eventually Hyro and

28:22 get reworking by slumping. Yeah. this is kind of a a general

28:30 of the river coming in the pausing . I've been depositing bars, those

28:39 being reworked by waves. And during , the bars are going to migrate

28:47 offshore and also generate offshore deposits. by the way, those deposits will

28:59 be generated by the storm waves. the talk, what we talked about

29:06 storm surge, wind set up and generated storm deposits going below storm wave

29:14 . Ok. That's some of these well, but we'll look for

29:19 Now, in the simplest term, got hyper protective floating deposits, sand

29:31 caused it then mixed sand and mud more or less settling out a

29:43 And what that would give us would a sandy portion and then a muddy

29:51 of that pro grading delta. Now sandy portion is typically called the delta

30:02 . OK. Uh Except here they the delta front extending all the way

30:09 here with the pro delta being mud below. Now, part of that

30:19 that even though uh Boa used this to uh as his model, the

30:29 here is that there's the sand does extend very far offshore and into very

30:37 water here. The implication is that delta front sand extends into much deeper

30:47 sand itself that suggests that the thickness the delta front may be a function

30:57 wave energy and type of setup. . Fair enough. But what that

31:04 begins to make it sound like is short face. Remember when we had

31:07 those discussions about where do you draw line with a pro grading system going

31:15 sand to mud? OK. And there's a similar confusion if you like

31:23 the use of the term delta And so I will show you examples

31:28 how this called different things. And want you to just imagine how is

31:36 might vary and this is just in at the dip section. Now,

31:42 other thing to keep in mind is when you're trying to correlate a

31:48 but from a couple of logs or roles, uh you need to be

31:55 about layer cake photography. When in , this is a delta. I'm

32:04 describe the sands as delta front, are not a straight line but form

32:15 um but likes to call shazam that extending into the offshore. OK.

32:26 each of these represents a major pulse by reworking and no pulse P

32:37 So we've got to just like we a meandering stream, uh which was

32:46 us series of packages that uh we to think about that pro grading delta

32:57 and pro delta So here is the Front, 1764 and here it is

33:04 1779. And so we can actually at the pro gradation of that delta

33:14 . Notice it's not called the delta here. Here, it's called

33:19 the sand is distributing a mount Now, all of a sudden the

33:24 becomes delta front and the pro delta way down here. Uh well,

33:30 don't use that distinction anymore. They back in the 80s, but just

33:35 you have to often translate older literature modern thinking. Ok. So what

33:47 would call the delta front now extends this. Ok. Um And I'll

33:54 back to that but notice that here's same um Mathematic shorelines. But now

34:04 what happened from 79, The 28, the delta has stopped programing

34:16 even began to be wrote. if we look at the erosion of

34:20 delta as a whole, large areas that pro grading delta front have eroded

34:28 especially if we look from 1979 look how much erosion has been occurring over

34:36 . The fact is that if you at 1940 Green is 1979 and yellow

34:49 2005, much of that delta Well, almost all of it has

34:55 depositing and much of it has actually . Ok. Now, what this

35:02 reflecting is the decrease in sediment load the 19 50s on with dams.

35:13 . Um so this delta is actually to be abandoned and we're seeing

35:21 the initial phase of it by erosion and what I couldn't find quickly,

35:31 I'll tell you is in the is there is that the marshland which is

35:37 measure of the sub sub aal delta disappearing as well. Now it's disappearing

35:48 two reasons. But the main reason the delta is subsiding at the same

35:56 , less sediment is being provided to the marshes. So all over Missis

36:06 is losing a huge amount of Siberia because submergence is greater than the sediment

36:15 can keep up. Now in natural or anthropogenic. And the answer

36:23 yes, both we had, we delta submerges because of compassion and this

36:34 compassion of the delta clay. We also get delta subsides because of

36:44 and oil and gas extraction causing the of clay. And if you wanna

36:52 into an argument, Pick one over other. Ok. Um Environmentalists want

36:59 say it's all anthropogenic petroleum companies want say no, it's all natural.

37:07 course, it's answer again is Uh But we're seeing the beginning of

37:13 transgressive phase of even this modern we'll talk more about that a little

37:19 , but that's really important to think this transition from Delta programing beginning to

37:26 abandoned. And just as a clue what's gonna follow what's gonna happen if

37:33 delta begins to be abandoned. one of the things is it's gonna

37:37 its river course, it's gonna shift form a new deal to low.

37:42 delta is forming today in Bay. we actually have some land rowing in

37:53 is the delta, which is the Mississippi delta. And most of the

38:01 that we're losing is a modern Mississippi . The loss of sediment and marsh

38:09 is in part coincident with and because the gaining of land and settlement with

38:15 fly delta. So just keep that mind. OK. So here we

38:21 this probating delta and up near the , we've got that bar crest and

38:28 bar and we'll talk about more This is that coarsening upward sequence that

38:36 the proximal out into frontal displays and delta. OK. So this is

38:46 delta front by the definition of being sand. This is clay. He's

38:55 pro delta and just like short we can argue left to right about

39:01 to call this. Is it distal front? Is it co pro

39:07 Does it have a new name? Well over here, uh it's called

39:13 pro delta. Yeah, that will . I'm not sure I care.

39:19 But uh and here it's called delta distributed him out. I'm gonna call

39:25 delta front. It's the same deposits it's just a matter of what do

39:33 call it? And going back to shore face, uh, foreshore

39:42 Welcome to the Real World. Uh I'm gonna keep this vertical section

39:47 though because it's from Boar. And got a lot of good examples of

39:52 these different face sheet by whatever Uh, cause here is that Hoing

39:59 sequence that we get, you notice in here, we get coarser splays

40:09 finally it's all delta front. let's begin with the offshore, highly

40:19 mud with intubated sand, but it's mixed up. It's really hard to

40:25 . Ok. What that says is low rates of deposition relative to rates

40:31 conurbation. Yes, mud is being out there, but it's beyond the

40:37 where the river sands over, they're relic duds left over when sea level

40:44 a little low. Ok. So primary sedimentary structures to speak of.

40:52 , we're beginning to get no primary structures, mainly graded beds of silt

41:02 mud, silk to clay. Um little bio, not much ur because

41:11 though we're beginning to get sediment that's derived from God, sediment plume,

41:21 sediment plume is also fresh pressure. we get a uh within the sediment

41:28 . We uh and because of the plume, we're getting a distressed uh

41:35 , how distressed. The relative amount bio depends on the subtleties of

41:43 frequency of floods. And so it's vary. Ok. And to get

41:49 up, we are getting into inner and mud and notice the sandstones are

41:57 to be a hum. Ok. the muds, they show these graded

42:06 that are more distal deposits of storms hyper pickle flows as we get a

42:14 higher up. You'll notice that some the sand has actually subsided for

42:24 This case is um completely separated from home layer. Uh And that's because

42:31 getting the sand coming out over very saturated, un compacted mud.

42:41 So it's loading, the sand is the underlying water, saturated blood.

42:49 we get a lot of soft sediment in that area here and that's shown

42:53 as well. Well, eventually we're then to thicker sand events associated with

43:05 pro grading point bar reworked by Uh It can be bioturbated. Uh

43:15 usually you're getting some kind of primary or structure in here. Again,

43:24 about that whole difference between the pro shore face and the pro grading river

43:32 delta. OK. Now, let's at that system as it pros and

43:42 is a real, this has been relatively narrowly confined lobe of the

43:51 So if we draw a cross section here, we're gonna see the pro

43:57 of that for delta and delta OK. And then we're gonna see

44:13 channel in the marsh deposits, marsh into bed. Now, this here

44:25 probation kind of begins to get a pack because it's mainly all sand.

44:32 this would be the distal and proximal delta. And this would be the

44:37 unit and some of that sand may be distributor channel and then very fine

44:49 get marsh. OK. Uh Here that pro grading system. Um

45:04 we might see, are they down ? Yeah. So by the time

45:11 get to this, actually, I you to mainly think about this diagram

45:18 in this diagram here. OK. In this transition here. So focus

45:33 what that looks like as that delta progra to the press you. That

45:47 what's called the bar finger sand. called the bar finger sand because

45:58 it has progra out digital digitate That is to say it hasn't bifurcated

46:05 lot. It bifurcated here and then kind of went on straight now that

46:16 finger sand is because of that hype flow and that deep water in the

46:22 plume, it just never, never widely. So we're seeing those plumes

46:32 out like this and the plumes are the sand will be deposited.

46:39 Now, if you look at it's pretty, I've messed it up

46:43 notice the variation of thickness From less 100 ft To over 200 ft.

46:54 fact, the pods are Of over m to six m. So what's

47:08 this very lumpy look? And I even add that if we look at

47:15 is a pack of uh I think a Pennsylvanian sandstone, the Antar

47:20 we get these same pods. There's about the pro, it's not exactly

47:32 . Ok. Yeah. The reason is that you pro grading over those

47:45 saturated muds again, easily compacted and forming these diap pes. And if

47:52 look at these dots, if you make a series of chores or

47:57 section, you see that this mud here is actually just the most recent

48:09 a series of older mud lumps. of course, the bar finger sands

48:15 sinking between the the dark periods. S U cord, a one of

48:25 mud lumps and they put down 300 of cool. And in 20

48:34 every bit of that core Casey had to the surface. That's how rapid

48:41 rate of uplift was due to loading those uncoached muds. And that is

48:48 course why we get these knobs of thinking and sand. And that's really

48:57 kind of the beginning of what's going with deformation further offshore that loading of

49:05 mud and the mud failing it's in of itself is causing a huge amount

49:12 instability issues with respect to that muddy . Oh, we get these little

49:22 slump of gullies and loaves all along front. Uh We get pro grading

49:36 here, but we get large scale here. We get older slumps that

49:43 being filled. Ok. So let's at that and we realized that the

49:51 delta is a mess. It is but an area of gentle deposition of

50:02 over time. Ok. And you some of these mud diap here coming

50:11 and even disrupting the delta, the sands, the rather the uh delta

50:17 sands. And then beyond that, get these growth faults. Gullies lumps

50:26 we look at how much of the has been reworked, almost all

50:34 up to 40% on the shallow delta has been reworked. The non reworked

50:44 is that lighter colored yellow? And more recent surveys show that as

50:51 get farther down, virtually, all the delta has been reworked.

51:02 And especially here, the orange is loaves. They laterally coalesce and they

51:11 are, was forming that part of delta. Now, if we look

51:18 them inside scan sooner, we see shoot and this culling and then the

51:26 is coming in. So here, the load, here's another moment,

51:37 know, a uh compression ridges. . If we draw a cross

51:46 these mud flows or um may laterally . Ok. But here's what they

51:58 up and here's the crowns, the compressions. Uh We didn't know this

52:10 of all until we started looking for and we didn't start looking for it

52:15 we lost a drilling rig after Hurricane . And in one of the A

52:23 um in the late fifties, they because of the hurricane and tried to

52:30 back. It wasn't there. They it eight miles down down slope.

52:37 And at that point, they realized um there's a lot of foundation issues

52:43 lack of stability problems uh that they taken into account. It's now the

52:49 thing you do when you go into offshore area, you do a basically

52:54 an engineering geology study uh to look the, The mobility of that lower

53:02 100 m. OK. Now, mentioned that the um delta today is

53:15 to submerge. OK? Uh It's to grow here. We'll talk more

53:23 that later, but I wanna focus the modern delta because it's what we

53:30 most about how this type of delta formed. It is a quote elongate

53:39 with the star finger sand. Um started out In 1874, very much

53:49 a bird today. It's not. and the reason is that much of

53:59 uh skinny leg of the bird's foot been fattened up with cress place.

54:08 most of the land that we see the more distal portion of the super

54:17 is actually for vast play and we monitor it by looking at Cubit's gap

54:27 right here, grew, grew, , grew and grew, OK.

54:37 By the way, it's now shrinking because of subsidence, but that's this

54:43 right here and these are some of oats, OK? Here's Cuba ga

54:55 one of the points about to And this has to CVAs places in

55:01 . What is a play in the ? It's just crevasse places that fall

55:08 that are associated rivers on deltas and into bays or going into rivers

55:16 going into floodplains. Uh Those gaps be long lived and can be

55:25 flood after flood as we've seen. here's the river Delt elongating and in

55:35 the lower delta plain is filling with blades. Ok? Now, if

55:45 look at one of those crevasse plays that view, we can look at

55:51 present active crevasse play and think of like a mini delta. We've done

55:59 like a pro delta delta front, tilt to play. But if we

56:07 more carefully, we've got evidence for older her vast play that it over

56:19 . But the expression of that, he is a little bit of a

56:26 marsh. Some Oyster reefs, the Wreaths were basically forming on the little

56:35 on the channels. And then of Bay itself. So we're gonna take

56:41 cross section down here is focusing on uh um modern, I'm sorry,

56:55 focusing on when this inactive distribution was and abandoned. And then we're gonna

57:01 a cross section more strike view to at the present day Travase play.

57:11 here's that channel, here was the play and here is that Crevasse play

57:22 into the bank. All the way here. Now that Crevasse play was

57:35 when this, when it shifted this here, notice it's still staying in

57:39 same location as the levy, but , it's shifted in the bay.

57:46 now we've got a transgressive phase erosion a beach and there's oyster reefs occurring

57:57 period in various Bethy metric highs. I've got a transgressive, I'm

58:04 a regressive transgressive cycle. Now, we look at it in cross

58:11 here's that older play again. But it has been covered by this

58:24 newer Vast Slight. OK. And this has the destruction of phase here

58:33 we don't have that here yet. let's see what uh a core might

58:40 like through here and basically, it's be coarsening upward and it's gonna go

58:51 the play and they use the delta here. Um I guess I'm OK

58:59 that, but I'm gonna use you Crevasse play, Andres Chen 12.

59:08 . So that's what you see here that's what you see for this part

59:11 here. Now, in fact, these are some of the faces that

59:19 vertical uh faces, you'd see uh upwards into the CVA play, then

59:27 upwards into the Crevasse channel. We talked about these before. We've

59:33 talked about the probating. OK? I'm not going to go over that

59:42 . Um But let me just remind that the same variables that we saw

59:49 the fluvial setting for Cres places is same in the, they aren't delta

59:57 except you're moving into a bay. bay is going to be brackish

60:03 It's gonna have a different set. gonna be standing water. It's gonna

60:07 a different set of benthic fauna and fossils and pelagic faunas and paleobiology.

60:15 . So, uh, and it's an area that's more rapidly subsiding.

60:21 . The deltas are gonna subside much rapidly than the fluvial settings. And

60:28 you got a lot more opportunity for of curves place. OK. And

60:34 here we have these uh series of upward and finding upper sequences and I'm

60:46 to suggests that they in part reflect th th this is channel abandonment,

60:58 here's a Creve uh channel and I this wrong. Um This, this

61:09 , this is coarsening up or this be, yeah, finding upwards,

61:14 sorry. Uh And then it may coarsening upwards again. So the channel

61:22 finding upwards, the plays are horsing . So let's look at what we

61:31 here. This is usually a uh I do in class, but we

61:37 , we're running a little short of . Uh So we have a series

61:41 these cyclic, small coarsening upward except for right here, we've got

61:56 chains that we can track all the across the area. So this is

62:00 flooding surface and then we get a from binding upwards to coarsening upwards and

62:13 getting thicker and thicker and somehow these to merge here. And then up

62:23 again, we've got a surface when go from binding upwards to questioning

62:31 Again, simply we lose it In short, we have a series

62:44 a complex vertically accreting series of crevasse bars, then crevasse channels. These

62:54 the little finding upper sequences and we a larger channel, this distribution

63:02 OK? And um this is an of a crevasse complex. OK.

63:14 This is an example of a dis channel with the erosion surface here.

63:28 . Now, the the one of points here is that correlation is really

63:36 . OK? I mean you not it, it's heterogeneous and it's in

63:41 dimensions. So these extremely, these river dominated deltas are just a nightmare

63:51 . Now let's also look at what is that delta begins is growing and

64:00 switches from a uh say it was distribution channel or there was a channel

64:09 that was active, smaller channel I mean a larger channel but still

64:14 channel. There are two small This channel begins to take all the

64:20 . OK? So we see a I'm here to there. All the

64:28 we have subsides, hey, as channel on the left gets bigger and

64:37 , it gets deeper and deeper, getting more and more discharge. The

64:42 are getting thicker and extending farther I mean the end of the bay

64:50 marsh, ok? Because the discharge getting bigger and bigger with that bigger

64:57 bigger channel. The levies are getting and notice you're going from a fresh

65:07 water marsh versus um failing to freshwater swamp in March. So you're

65:23 changes and those, the peat is thicker. So you're getting changes from

65:31 silt to brackish to freshwater marsh. all of this is happening as you

65:42 causing this delta to subside. And distributor is getting more and more of

65:52 , the water and set it. this coarsening upward sequence here would be

65:58 to this little core right here. . So here we have that uh

66:05 distributor, that active distributer and we a sense of that prorating uh levy

66:14 thick a grading swamp peat. This finger sand. Yeah. No,

66:29 is pretty much how this delta pro out into deeper water. So remember

66:36 is also what I would call a water delta then 150 ft of water

66:43 more. OK. Yet we know are older river courses and older

66:57 The whole scene depositional environments within the are really complicated. And this

67:07 well, the, the sequence we one to three or by actually six

67:23 7, if we draw a cross through here would look something like this

67:33 Valley Field, then a delta That's actually um around 6000 years

67:40 that's below present sea level. And by the time we get to the

67:45 , the younger deltas, they're more less at the present high stand and

67:50 get the seminar, the force, plucking line and the, at you

67:58 , there's more numbers here because you divide it up or not, you

68:02 or a splitter basically. Ok. this would be more of a lump

68:09 I'm gonna look at in particular, this pattern of delta and that's really

68:23 common. Uh Here we have it the Mississippi. Uh This is from

68:30 yellow. Um And this is not we think of and normally as the

68:42 of a delta that's occurring way down , that's occurring down here.

68:51 It's an avulsion that's occurring up street it's an evo that's occurring pretty much

69:03 a distance equivalent to the back water where we go from the channel is

69:14 mean sea level to the channel dips mean sea level. And even though

69:19 tidal effects may only extend to there is a backing up the water

69:27 backs up uh to a distance far and that's what's causing these big shifts

69:35 big rivers. Ok? And this the abortion length, the calculated backwater

69:44 . And you see it's a pretty estimate for all these rivers.

69:50 Well, if we look at think , this, uh you know,

69:57 X get this, I wanna look um, this sound right in

70:11 I'm sorry. No, I I, I wanna look at a

70:17 and they had to fly at That's this zone here. Here's the

70:22 you fly river coming in. here's another spray of the river has

70:34 brought, has been channelized down to . So there's two deltas here,

70:39 into a fly a bay. It's delta in the Wax Lake Delta.

70:48 , the Wax Lake Delta is is the younger of the two deltas

70:55 it's relatively undisturbed. There's been a bit of dredging occur here, but

70:59 is the older delta. So it's more work done. And here we

71:04 a study from 1973 to 1982. notice it starts with these little,

71:10 , little uh isolated bars, distributor bars and they tend to coalesce laterally

71:26 downstream and upstream. Notice how the bar has grown both upstream and

71:34 In fact, we can look at , this was the original bars and

71:43 at how much upstream migration as well downstream migration as these little bars laterally

71:51 . Ok. Now, what that is that when we look at the

71:55 little bar, little and as it to accrete at some point, begins

72:11 elongate and migrate upstream as well as , she kind of show like this

72:18 notice where we're beginning to get upstream . Yeah. So this is the

72:30 is nucleated here. It grew down and up street. Well, Exxon

72:41 and did a detailed study of Wax and it was, it's more of

72:44 pristine Delta. You need a lot coy. And what they found was

72:51 you look at the, the it consists of a series of these

72:58 . That's not a big surprise because what was seen with. Um,

73:06 had to fly, but these lobes , they call depositional packages and they

73:16 decided to say let's call this a deposit complex because they found that those

73:27 were the result of a creating jet . So what a jet deposit?

73:41 , this is the beet right This is what's happening has that jet

73:51 river water empties into the reservoir, forms a jet and a deposit

73:59 And so the delta itself is going be an amalgamation of those and that

74:06 deposit. This is what would look here and this is the pattern and

74:13 flu. Ok. Notice we get elongation of levies, they're called pseudo

74:24 here for some reason. And we this pod uh where the bed load

74:31 deposited. And that would be analogous that present bar and back bar,

74:39 back slope and down slope bar that saw earlier. And then down in

74:47 , we get the deposition of suspension set. That's analogous to this opal

74:57 that was described by are modified from right. OK. There's a

75:04 in here where the velocity stays high turbulent mixing hasn't really closed it

75:16 So the high velocity means there's erosion then is followed by that I drive

75:29 that rapid deposition to belong erosion to . And that's what we say

75:39 This is actually an eroding channel and is sediment is depositing in the core

75:52 bed load to distance suspended. And you look at in cross section,

76:00 see that this starts as a little , the bar begins to grow and

76:11 it begins to erode on the backside grow on the downside. He rode

76:16 the backside, rode on the the road here and also starts to

76:27 in here and fill up and that bar was here and it shifts to

76:41 and then to hear and here and forming a to get deposit complex and

76:52 add those complexes together and they get delta. OK. This, by

77:00 way is that or again? And what we saw here. Yeah.

77:24 this is again, uh what you see in cross section, the scour

77:33 grading bar, shift, scour pro bar. So here is the axis

77:42 the main channel. Is it a ? And then Phils here is those

77:51 those pro grading uh jet deposits as go extend offshore? Ok. And

78:02 is that erosion on the back scow or Phil erosion on the backside

78:13 deposition. Here's the erosion on the downstream deposition. OK. This idea

78:27 these bars nucleate and then pro grade and at least initially upstream with erosion

78:38 the back side is seen almost Once we start to look, this

78:48 in Pennsylvania. This is, of , the anti um here is the

79:00 looking at these bars and erosion of backside. Here it is. And

79:09 , uh crop. Here we're actually a little bit of the backfield uh

79:14 re notice how this bar nucleates. grows upstream and downstream and then it

79:24 to be scoured, nucleates and grows and downstream with one shoot Deposit,

79:36 shoot complex. So what this this is based on fieldwork but it

79:46 the work that uh welder and others on uh the low uh growth.

79:58 . Uh More recently, we've got data showing that with a hyper pina

80:09 , we can still get the same downstream. And even with hoopy of

80:21 grain, we can still get So this would be, let's say

80:28 grained stratified hyper course, your grains up bigger. Homo builds up a

80:41 , doesn't build down as fault. , a picture you'll recall. It's

80:49 plume spreads out more deposits quicker. it's steeper. OK. That's a

80:58 place to stop. What was, was the? Oh the great is

81:03 seven. Uh So this is the lay layered uh water. Uh It's

81:11 dense then the incoming reservoir in the case. So it's hyper the um

81:22 trying to figure out what to do that. Like is that, is

81:28 suspended on the top? On the side? Yeah. Yeah. Um

81:37 , that's in suspension. So um the hyper pick flows um it can

81:47 in suspension but it can actually become concentrated that it begins to move by

81:55 . That would be the hyper. . Uh Notice in here is behind

82:02 bar, it's all below. I'm , it's not true. On the

82:06 , it's gonna be bed load and here suspended, you're increasing velocity

82:16 peak velocity breaking waves, deposition go to thinking about, yeah.

82:27 Here where we got this increasing and here they actually suggest that the water

82:42 be uh uh less dense. Um Here they're arguing that there's so

83:01 sediment that it's more dense. It up the back, increasing velocity,

83:09 erosion deposition, relatively rapid deposition. , steeper force sets. Then if

83:21 depositions occurring over a longer area, also the deeper the water this deep

83:27 the four, we'll talk more about changes. But uh this is actually

83:35 you change notes. OK. um I'm gonna take about a five

83:41 break. Um We'll quit recording but keep uh this on. Uh You

83:47 need to get your notes out, a break if you need it and

83:51 um 3 40 now, About five 10 minutes. OK. Any questions

83:59 , before I think? No. . Recording again. OK.

84:10 we spent a lot of time looking two parts of the modern Mississippi

84:18 Uh, the bird food. It's called the Bali Lobe. And,

84:26 , that, that here. Oops the a of lion down in

84:35 Uh, yeah. Yeah. And about the differences. The,

84:44 Bali or modern bird foot is an digitate. Uh Delta is one that

84:56 in relatively deep water. It is that um has very much brilliance.

85:08 dominated uh to configuration which confines us these bar finger sans. The A

85:22 a much more low delta. It's friction dominated dispersion because it's emptying into

85:32 shallow bag. They are both modern of the Mississippi Delta and also mentioned

85:42 there are quite a few older lobes in particular, I want to look

85:52 the lobe that is in this area . It came in like this and

85:59 can see good evidence. It was by the day's delta, good evidence

86:10 this contributory pattern. OK. And called the LA delta the four.

86:27 it really is very distinct from the day. It's got a lot of

86:38 , all of which are more or active at the same time. Uh

86:44 got a wide fringe of delta front because sand is coming in from

86:52 many places. And of course, does have a pro delta for the

87:01 . If we look at the uh we've got basically, I,

87:05 need to enlarge this one day but we're looking at distribution channels and notice

87:13 they're getting smaller and smaller these that be shown like this because they're

87:23 At the same time, we get broad. Yeah. S the front

87:31 is uh consists of distributed amount bars a slope and they uh the margin

87:44 it's kind of interesting here. Uh call right one which is they

87:54 they sub differentiated the delta front into and then more vital delta fronts and

88:05 how widespread it is. The the delta front extends laterally really even

88:13 little bit beyond the uh the friendship the Isaac as you might expect is

88:23 be much more low paid compared to bird flu. Yeah. And if

88:30 look at it in three dimensions, you find is that delta front is

88:36 a sheet sand. If you could a look through here, it,

88:40 basically a sheet sand, a low sheet. If you like going into

88:46 clay and clay with channel field sitting and there, that's in contrast to

88:55 bird foot with the nearly confined she is so we, we can automatically

89:08 to see the difference between the LA and, and about A little over

89:19 1000 years ago. And uh the , the and the digit. And

89:32 we've got at albeit at different scales much better view of what a cross

89:43 might look like. This one, digitate one we talked about should be

89:50 by now, why it's so Ok. And it should begin to

89:57 apparent why the delta front here. why if we look at the vertical

90:09 of that bird foot, we go the pro delta and, and these

90:21 are kind of crazy. Uh but coarsening upwards with the cleanest sand at

90:31 top. Uh This would be also mouth or uppermost delta front. I

90:41 know what you like. OK. here and compare it with the low

90:52 , we got our mouth bars coarsening to pro delta and distribution channels.

91:00 strip channel wasn't shown on this Well, the first thing that comes

91:07 mind you might say is why, is uh it got so much more

91:13 in the mouth bar? Um My is that because in this zone

91:22 uh you're getting more river influence, down here, you're getting more

91:28 OK? But in any case, important to, to look at the

91:35 shape, OK? And coarsening And one of the things that's kind

91:51 interesting, the I need to read more carefully. Uh They're putting the

92:00 here, but uh then here they the, the distributor champ. I

92:11 know why it's not here, but should be ok. And it's pretty

92:17 . With the exception of some of the muds here. What is not

92:31 is the thickness. This is 80 , I'm sorry, 80 m.

92:42 is 20 m. Yeah, you've a very exaggerated thickness of this bird

92:56 delta and it's exaggerated for two It's being deposited in deeper water.

93:04 they have more accommodation space so the can extend into deeper waters. There's

93:14 subsidence going on. So we saw over thickening of those mouth bars as

93:20 paraded through time because of the compassion that over thick delta wedge compare that

93:30 the very thin pro delta clays of shallow water delta. There's not much

93:40 space. The muds frankly are gonna washed away. The muds are gonna

93:45 up in Western Louisiana and sheer They're gonna even end up in

93:52 but they're not gonna end up underneath within the a fly bay or

94:00 So to me, the most important to think about in these two deltas

94:09 one, the geometry of the, the delta front is I'm using it

94:14 also how thickness it is a depth water um significantly modifies both the process

94:28 the void versus frequent versus uh friction uh river processes and how the sand

94:38 deposited. Ok. Now, I go more as to what happened

94:48 Now, the delta when it was and when the new delta formed.

94:57 mean, we went through a phase a that now evolution is different than

95:02 , switching, contributory switching or is basically gonna oh the same lobe to

95:14 a little more complicated but distribution. a A V means all of the

95:24 are abandoned. Like is what's happening in the Mississippi and have been transferred

95:31 what probably would be they had to at. Now, I I described

95:37 this constructional phase where the distributor was bigger. And now I want to

95:47 about the destruction of phase as the is abandoned. It's abandon, it

95:56 to fill. Subsidence continues. So marsh will continue to grow. It's

96:07 thicken, but it's going to go um fresh water to brackish water vegetation

96:20 it continues to subside. The entire a plane is filled. You're,

96:32 not gonna have the distribution channel It's probably just be a little and

96:39 you're bumped. Now, look what's over here. You've got erosion of

96:50 what is now a salt marsh and level continues to rise and we're beginning

96:57 see a dissection of the salt marsh title a chance. Now, remember

97:04 said as sea level rises, but a relative rise, sea level,

97:09 whole abandoned low is sinking. So can think of that as the whole

97:16 lobe being flooded. Now, it's flooded over here, but the water

97:24 reached this particular spot. The ground has, it's become more contaminated.

97:33 getting more salty marsh, going from water to brackish water marsh now,

97:39 water. But now we're beginning to erosion as well. So let's imagine

97:44 active delta, let's imagine that it's . And now that act of delta

98:01 all of it is subsiding. at the front edge of the delta

98:13 being eroded by waves and we're gonna this arcuate string of barrier islands.

98:22 behind that, the delta plane is be flooded with Bay Marsh, the

98:31 delta plain and the upper delta plain continue to be marsh will vertically accrete

98:38 PETE but will gradually become more So let's look in for a section

98:46 was that original delta and here's to and it's been reworked. This is

98:59 Ravi and this is an emergent sand barrier island or bar or show

99:10 We got the flooding and actually eroding the edges and the subsides and abandoned

99:19 the chance. Ok. Now, thing is, let me just

99:30 notice we've got hence of these abandoned here, we're gonna see later.

99:40 gonna be outlined by oyster reefs typically of the higher levies of those abandoned

99:49 . Yeah. Uh This area here is here, beginning had the flooding

100:01 erosion of the bay and this is it would look like more or less

100:10 the wave erosion, uh wave uh uh Raven and we might get a

100:18 bit of Todd limit, uh save here. Now again, we've got

100:26 abandoned lobe is being submerged. we'll see complete submergence of this area

100:40 this lobe continues to grow. we can look at these different lobes

100:47 they actually represent different stages of abandonment better said they've been abandoned for longer

100:57 of time. So if we look the youngest lobes like the Saint

101:05 which they hear it in the, we look at older loaves of some

101:12 and even older, the we're looking older and older, progressively more abandoned

101:23 . So let's look at the Saint lo and look at the chandelier is

101:29 right here. Those islands are basically realm of eroded delta frog with the

101:43 behind. And so what we can is that the active delta is here

101:53 the delta fro it's abandoned. So gonna have less sediment coming in

102:02 It's gonna begin to erode and spit accretion will give us elongated spits and

102:14 islands. It'll continue to si This is now gone. It's now

102:22 detached island and then as relative sea continues to rise, the island has

102:34 some merged shots. OK. So kind of imagine this transition is illustrated

102:45 various stage like as we see OK. Well, here we've got

102:52 series of uh planking barrier islands which sorry. Um The sequence here would

103:10 now let's see. Now, I be more like here would be our

103:16 barrier island sequence, vertical sequence. . Now, right now the uh

103:24 the uh the bay has come in two sides, but it is still

103:31 here here. Ignore this for a . Hair is completely detached.

103:43 it's now a transgressive barrier island which this now is a transgressive buried is

103:53 seeds and you recall what that it was lagoon or if you like

104:01 Flo Tale Delta, wash over etcetera. OK? Now, eventually

104:06 gonna subside and it's gonna be completely . And when it does that,

104:14 continue to trans uh move la but barrier island core is being reworked into

104:25 sand and that shelf sand now is OK. And so what you see

104:34 is the crest of the should and the front and then kind of the

104:41 . So it's gonna give us a upward sequence and it's also going to

104:50 increasingly bioturbated at the ball. that be the same here. And

104:58 it sinks far enough, it's down . This is ships. So,

105:06 , which is oh in water, it's uh several meters thick but in

105:13 depth. So well, I can't now. OK. So each of

105:21 sequences is a reflection of the abandonment of this deep water delta.

105:37 Now, put those together, here's pro grading sequence active and then a

105:56 . So eventually sands moving landward to us shoal and Shoal crest.

106:04 So the constructional phase destruction phase now that but a chart, OK.

106:20 The destruction of phase is almost completely . So we're gonna see that where

106:27 not a lot of subsidence, you get this thick bay accumulation. The

106:36 problem though is scale This scale here maybe four m that reflects what might

106:46 going on today. If you look some of the older um shoals during

106:54 sea, this constructional phase 10 Now it's more like 30 or 40

107:04 . This is kind of compressed. the construction phase is actually much greater

107:11 thickness and the destruction of face even where you get these migrating barrier elements

107:19 , OK? Now, I wanna back to thinking about this transgressive regressive

107:32 , the sand and mud geometries in of the reservoir characteristics. Um Here

107:45 got a they uh our finger sand down to pro delta modes so we

107:57 envision it right about here. Let's at something a little different, maybe

108:04 for a second that we've got a section. So now we've got three

108:13 mouth bars and now let's imagine they've abandoned. OK. So what we're

108:22 at here is a pro grading phase gross and then a channel abandoned.

108:36 . Now again, different terms, bar, outer bar, call it

108:43 you like. You're looking at increased size better sorted the channels where they're

108:51 , they're gonna be pretty well mud filled when they're active. And

108:56 what we find is not a your best reservoirs within the channels are

109:02 be in the base. Your best in the bars will be at the

109:07 . Your non reservoirs are gonna be pro delta and to a certain

109:12 the outer uh bars uh your marsh the shelf. Yeah. So if

109:23 looked at the active or the mouth , let's say here in proximal

109:35 that is closest to the land, gonna be funnel shaped where you call

109:44 and outer and pro delta, you're as me. But then let's go

109:49 . Let's look at this in this . OK? We're seeing, pouring

109:57 wedges and even farther little places. what we're looking at is oops the

110:28 out of the sand giving me Now you saying that, isn't that

110:38 ? Hang on while I figure out to un animate this. Oh,

110:50 . OK. I guess that's Uh And you learn something every

110:55 even things you don't wanna learn. . So we see this as basically

111:01 pro grading strand line, pro grading island, pro grading delta front.

111:11 . With the contributory channels. Think how they feel. OK. And

111:30 saw this with any river deposit, can fill abruptly or I can fill

111:42 . Ok? And that will determine nature between uh the top cap sealed

111:50 the lower most active part reservoir. . So, oops. So let's

112:07 a cross section or rather making a section Based on four logs in

112:14 in a delta that's been abandoned. , we got certain profiles here.

112:23 got a relatively homogeneous mud with the , a little bit of thickening or

112:35 here. Then we got a worsening package serrated, abruptly kept and I'm

112:54 kind of just correlate the base of . Now above that, forcing up

113:05 sand in this place, we have course defining upwards package look kind of

113:14 this. It's separated by something And then on top of this and

113:23 , we've got delta plate. So on top of the delta plane

113:33 you got a pot of sand over , here's delta plane again and then

113:55 delta plane is capped by nothing It was hard to see what's going

114:01 here. But if this little, is a little bit of delt playing

114:14 , but it looks like something I to figure out is this relative with

114:24 and these two thick sand to finding their sands are distributor chance the coarsening

114:36 sequences the delta uh delta fraud. I might imagine this being a channel

114:49 . Now, the problem is mhm is has dealt a plane here.

114:57 I'm I must cut this off here maybe even to hear and this might

115:06 another little chat. And up here may be a transgressive face. So

115:15 see how we might do this. . Well, sure enough, here's

115:23 channel. Here's our, our finger , here's our delt to plane.

115:41 here the interpretation is this big It's probably not a crevasse channel.

115:45 another channel. Ok. Here. this is all a grading channel.

115:59 mean, a grading delt to playing grading Delt. And this truncation up

116:06 is basically the flooding during the destruction phase. OK. So you see

116:18 importance of being able to correlate the , the pro delta and the delta

116:26 environments. Now, this is a more complicated and I'm not gonna go

116:31 it, but uh I'm gonna let look at this at your leisure uh

116:37 think about this cross section worsening OK? Uh think about one,

116:52 , six up here. Uh And now is more like a low

117:01 OK? But think about how they about correlating these sands, you

117:09 I'm not gonna ask you to do on the quiz, but it's useful

117:14 have a look at the difficulties in . Um And where these came

117:25 OK. Now, clearly, sea is one of the major triggers and

117:36 regressive cycles and deltas and everything And if we think about pro grading

117:46 in programing delta packages, we could of a normal regressive or forced

117:52 you might actually have the deltas down which occurred during the last drop in

117:58 level. Yeah. And you can packages pro grading transgressing, pro grading

118:10 transgressive, probing less and transgressive or grading transgression, probating more transgression probating

118:22 transgressions. Now, what we we're at here is a retrograding pair sequence

118:31 . Each of these is a pair . This is a set of pair

118:37 . And in essence, what we're at is that there's an increasing ratio

118:44 A S. What is that accommodation to sediment supply, sediment supply is

118:53 . But when the accommodation stress, space rises gets deeper and then when

119:03 stable, it pro grades out because accommodation is not changing. SAS supply

119:09 still being added and it's accumulation rises . So these pulses of delta pro

119:19 during a relative rise in sea OK? And there's a back stepping

119:27 these packages. Here's that prograde uh gradation we looked at right two and

119:40 down here during a high stand and even older down here. So this

119:49 a retro gradation of sequence set of lobes With the oldest three being formed

120:00 rising sea level and the most recent during the high stance. OK.

120:08 what happens if sediment accumulation is faster sea level rise? That is a

120:14 A to S ratio, you get net c advance of the sea.

120:20 that's what we see here in the off trend dances. So we are

120:35 filling that base. Now imagine you've a seismic lion, the side MCLA

120:48 show very nicely these large slopes and really the growth of the shelf

120:59 Those are Sheth margin kind of But in fact, what we see

121:07 here are thin packages that we may be able to resolve initially, but

121:12 are the delta kind of forms. what we're looking at is basically a

121:22 probing until it eventually it gets to edge of the delta. At that

121:30 , the shelf can throw gray. you got this little bitty delta,

121:37 say a little bitty, they're, as thick as the shelf is

121:43 OK? And then we got these of creating content. Ok?

121:54 before we get too complacent, let's one confusion. Let's look at the

122:03 and add a sub aqueous delta. we've got two clients and those

122:11 by the way or up here, on the shelf, the Saville Delta

122:24 , which is what we've been talking and something that's been happening offshore.

122:31 see it in this area here is a pro delta Clione. Where is

122:39 coming from? It's coming from a of setting is being transported down,

122:51 displacing that kind of, I mean uh mud clini here it starts and

123:04 it migrates down is going to become and more detached. It is in

123:18 a mud fluke and it forms this Delt. OK. So when we

123:32 of those clients, again, in cases, we would actually have a

123:43 of form of that sub aqueous delta across the show. We'll come back

123:55 this a little later, but because talking about, I wanted to mention

124:00 . Now, here's those three Actually, the two that I talked

124:04 earlier, the the back stepping in pro grading delta. And you could

124:11 imagine it vertically accreting it'll vertically accrete a high stand and a low

124:18 it'll backs step during the transgression and uh prograde uh during the high stand

124:25 drop. Now, Doris Curtis early suggested that the type of delta that

124:36 get in each of these cases, gonna be a different type of delta

124:46 it will have a different style of a OK. Here you got it

125:00 very much of a wave doin delta it will a grade or, or

125:10 will accrete in the back lapping port . Here we have a low be

125:17 and it will a grade vertically. , you have a river dominated delta

125:23 it will prograde. Oh, So there's a couple of things she

125:32 that hadn't been noticed before or hadn't published before. Then, as delta's

125:42 offshore and onshore, they change. the delta that's at the shelf edge

125:49 gonna be different than the delta back the shallow water and of course,

125:55 those iso pas vertically accrete will depend whether or not it's a grading,

126:01 grading or back stepping. Now, got into this and started thinking,

126:08 , let's, let's think of maybe have river dominated here, more fluvial

126:14 wave dominated here. And then he , you know, maybe as this

126:19 gonna be even more wave dominated. . So the difference of opinion

126:26 but the key is with this wedge sediment, we, if we had

126:31 , we could talk about the But this is basically something like the

126:43 delta here hasn't yet pro graded across shelves. The prediction is when the

126:52 regression or pro pro gradation is going morph into a fluvial wave dominant

127:00 which by the way, we'll call delta. So let's look at something

127:11 we might imagine occurring with the As the progress is offshore, it's

127:21 go from a shallow water inner shelf to a deep water shelf margin

127:30 Now notice the shallow here is actually LaForce delta, yellow water friction

127:39 What is not shown is a mid birds foot delta. OK. But

127:47 it would hit the shelf edge, got a lot of sediment. So

127:58 got a river component, but it's exposed to high waves because there's no

128:05 across the shelf. So high And so this is delta is gonna

128:12 to begin to prograde. The show mean prograde the slope. It's made

128:17 across the shelf and now it's pro into deep water. So here are

128:24 you kind of forms and here are clients and these are the things you

128:35 think about is that delta went from delta to show margin. Um The

128:44 of pro gradation of the high here here. Why? Because there's more

128:52 to fill wave influence, relatively low the inner shelf, high on the

129:00 she growth faulty. We'll see, gonna start getting a lot of growth

129:06 when we get off here. Uh gonna get a lot of gravity

129:13 When we're in the deeper waters deeper slope, the slope itself will be

129:18 higher. So shell margins, different margin, deltas are really different.

129:32 ? Now, that isn't to say there's not defamation occurring on a mid

129:39 March, if there's a lot of , uh you can have a pretty

129:45 slope, all of maybe a Anything about a 5th of a degree.

129:52 there is some deformation but is the gets deeper, the defamation gets

130:02 And now we're getting a lot of , a lot of slumps and even

130:13 and shape like paradis. Ok. this shelf edge margin is really a

130:21 structurally active self. And one of that's gonna happen is we're gonna have

130:27 lot of these hypericum flows that are be coming down. I mainly river

130:39 . Now, you can also get hyper flow that is do too.

130:47 lot of sediment plunging down. I'm gonna talk about that for right

130:56 But these hyper pial flows are basically to be clothes that are, that

131:03 across the shelf and will become active the shelf margin to help accrete the

131:12 . I suggest you read these on own. But here's that high protective

131:19 here, it's forming that mud plume I talked about where you got that

131:31 . Ok. And here's that mud crossing the shelf. But for right

131:44 , at least I'm not gonna talk much about these in, in

131:51 about the fluid mud. But fluid is a type of low fluid rather

132:04 has concentrations of mud up to 30% weight. Normally, it's a couple

132:11 1%. It's such a high concentration silt and clay that it is a

132:21 flow. It's a density forms a float and it can it be formed

132:31 that zone of maximum turbidity in a , in an equator, in an

132:39 . Uh or it could be associated waves. A storm comes in d

132:47 it or it can be associated with . There's such a high influx of

132:53 that it's super concentrated and we actually about that a little bit with

133:00 Lakes are really good place. Hyper are very well developed in lakes less

133:07 in marine settings. But you get are are things that at first blush

133:13 like intertidal deposits. So this goes to my earlier comments at the very

133:21 day. Don't be too fooled by particular sedimentary structure. These are hetero

133:29 sediments. I've already mentioned probably five places where you find these hetero lithic

133:38 . Ok. But going back to margin, some margins are pretty

133:50 That doesn't mean there isn't very much and sediment slumping as material is coming

134:02 from the delta plane. But there's the large growth vaulting, for

134:09 OK. And so here you're getting , pro grading is coming down,

134:15 it's still pretty much pro gradation. ? And so here is a pro

134:22 shelf margin. Now, they would your stuff down here. But consider

134:31 alternative where it's an unstable margin. of growth faulting. It may be

134:37 master regional fault fitting right here. ? It's a very different stories.

134:47 know, if we look at just forget about the master faults, but

134:51 smaller growth faults is in here might something like this. We'll roll over

135:00 over thickening. These are sin depositional . These are the growth faults.

135:07 ? You see it here and you it in here. Now here is

135:19 is bypassing the shelf through some kind a channel submarine fan, but you're

135:29 getting slumps and failure up here. you get a little delta, they

135:36 be stacking up behind a, a here. You got a shale,

135:46 salt core or shale coal where it have a, a to a to

135:55 where it's extension here. Compression And I've got another little package for

136:03 . A lot of growth falls in . Ok. That here we got

136:12 programing margin. Here's our unstable Here's the big growth. You got

136:20 pond areas and maybe the, the down here, Compression ridge. In

136:30 , what we're looking at at the edge is a lot like a

136:35 It has a lot of same characteristics terms of the extensional head compression

136:45 Now, here is a cartoon that's a lot of backing to it in

136:52 shelf show margin. Think la fouche grading offshore mid shelf deltas depending on

137:04 sea level is doing. That could the Mississippi Delta. If it's a

137:09 sea level, if it's a forced , that is to say you're moving

137:17 , but you're also staying in shallow , still gonna be a shallow water

137:25 , but the wave energy will be because you're reducing the fetch. Is

137:30 clear that when you go from this the water depths and stay shallow

137:47 the delta, but the shoreline has that are higher because they haven't been

137:55 as much because the delta is closer the shelf age, you get to

138:04 shelf edge, it's gonna be still lot of fluvial sediment, but a

138:11 more waves as well and it's in water and it has the potential for

138:18 defamation. Then as sea level rises the rot in the deltas, a

138:26 of them are gonna form ASU. we've got a lot of estuaries that

138:32 forming so that the deltas are basically head deltas building the estuary. We

138:42 about earlier, we talked about the in sea level causing the flooding of

138:47 rivers going from delta to estuary. it's not until high stamps that the

138:59 can fill those estuaries and begin progra again. Yeah. So here we

139:10 the situation where we're looking at the or, and it's a wave dominated

139:26 and it started during the transgression is migrating, waved dominated barrier island when

139:42 filled, it became a wave dominated . That's exactly what we talked

139:54 Last time we talked about that in dominant deltas when they failed. So

140:00 looking at the transgression, an eventual of that and then it's gonna start

140:12 its way out across the delta across shelf. Yeah. Now, in

140:19 cases, there was um it goes wave dominated to a little more wave

140:26 uh I rather uh river dominated as get across. Um Here it's getting

140:34 to the shelf edge. So we're a little more sediment deposit offshore here

140:45 crossing, should note that it's crossing shelf. Now, it's beginning to

140:54 the shelf itself. So now it's stable pro grading shelf. So here's

141:03 shoff delta pro grading stable margin. it's kind of like what's happening

141:13 We had the delta pro grading across shelf and then extending to be on

141:23 shelf and notice at love stand, begins to vertically acc predict again.

141:30 then during transgression, it basically And here we have that bahe delta

141:38 . OK. That they had delta still become a either wave or river

141:53 delta and it'll prograde across the shelf start the cycle again. Now

142:03 so in this case, what has the pro gradation is the sediment supply

142:15 the shelf. So the argument would that we're at a relative high stand

142:21 the Mississippi Delta has prods the shelf . Now notice there's some submergence going

142:30 here. Um A little hard to this graphically, but you know,

142:35 Delta four sets are getting a little thicker rather. Uh And that's in

142:43 because the shelf is getting deep. shows as a horizontal shelf. It's

142:49 OK. So it's, it's getting little deeper, but still it's moving

142:54 pro grading. It is a normal . OK. Now, is that

143:02 ? Well, let's see if you at the rate at which a delta

143:11 is moving versus seven input. Uh Well, let's see how to

143:22 this. Um The Mississippi is I'm sorry, have to ignore this

143:30 just a second. Look at the at its sediment rate in the shelf

143:39 . It would take 10,000 years. had 1000, it would take 10,000

143:49 to migrate across the ship. The Take 25,000 years. The Brazos.

144:02 , it'll never get across. So it's really hard. There are

144:08 few deltas in the world that have much set that you could envision them

144:16 the shelf without a drop in Now, forced regressions exist but on

144:25 very wide, almost epic Contin epic shelf. OK. So here are

144:34 of those place to see shelf edge and they were formed during low stands

144:40 sea level and here's just a kind a vertical section. I'll let you

144:47 at it and think about uh what fluvial cycle might look like why we

144:53 some things down here. But it's a forced regression until we get to

145:03 low stand. OK. And actually it out. Then it stopped here

145:14 then began to pro out again, here in his trunk. Yeah,

145:23 is a Wheeler diagram. So it chosen it, it's not a cross

145:29 per se. It's just saying what's on. OK. Now what happens

145:35 this point here where it begins to past the previous show? The suggestion

145:45 is that it's a stable programing But what Doris Curtis saw in the

145:53 scene was that as the shelf began prograde, that is to say,

146:01 the subsequent regression began to go beyond shelf margin here, it began to

146:19 . This was the o shelf margin here. This is a newer she

146:27 failed here. So we're getting these regional roof falls that were occurring in

146:38 new one will form here where there been a long well established shelf.

146:50 as the, the delta crossed the due to drop in sea level,

146:56 it reached that point, it began have a growth fault. And those

147:01 falls can be seen all along the , the Gulf coast. These are

147:05 major regional growth falls that extend for of miles, ok? That delineate

147:14 old shelf drinks. Now, there's way that it could happen and does

147:24 you begin to prograde across the remember that there is some mud that

147:32 progressing over and that can cause a of head were migrating scarfs or

147:47 ok? And as they migrate they're gonna form a large in embayment

147:56 indentation into the shelf or rather into shelf and delta deposits. And it's

148:06 sold right here on the old It's gonna be a on the shelf

148:13 in some point it's gonna stop. there's one possibility for how it

148:20 it's gonna be like a big It's a slop skull with landslide,

148:27 material here. Extensional faulting in here this big regional bit, this big

148:36 here that slows down in a series smaller growth folds all sowing into this

148:46 decor. Now, ironically within that , there are pieces of delta slope

148:54 could be reservoirs even down in But the bulk of that scar will

149:06 filled with something else and it could filled with mud or it could be

149:13 with Progra Delta again. So let's a look and a system here.

149:24 these are growth faults, small OK. This is the how you

149:32 to try to correlate them. But is a system in Utah and you

149:41 a fault right here. It souls here. Another false here sold out

149:46 . There's even a little roll over . A little thickening here.

149:53 You can see how that thickens this section is not this the photo,

150:01 it shows the same things. So see these small growth faults that are

150:07 out basically along the pro delta. ? This is the delta front and

150:13 there's the pro delta clays below. of this is clay. OK?

150:20 down there at that transition, we over thickening. Now we have at

150:28 larger scale here is a section preserved fiord collapse, big blocks and then

150:46 pro grading still with the upper part a delta and the lower part being

150:58 , sandy to Shay turbinates. That's of what we see here. Slump

151:09 prorating fill down in here. Um flow deposits. That's what we saw

151:24 . Yeah. This particular diagram on top is based on uh Wilcox uh

151:44 . This diagram on the bottom is on exposures in the Norwegian fjords.

151:52 a surprise, Edwards worked at the fjords and then he started working in

151:58 subsurface of the Wilcox in scout And he brought that with him,

152:05 he had seen in the exposures led to recognize what was going on.

152:11 , look what we got here. got edge of a delta collapse and

152:19 with delta a gift and that, scar here. We've got big fault

152:29 . I mean, scoured blocks, block build with pro grading series of

152:40 going into delta plane. OK? we see the effect of slope edge

152:49 . OK? I'm gonna skip this I'm gonna skip that. I'm gonna

152:53 it quits here. Uh We pretty have talked about the types of failures

152:59 we get on unstable slope edges and edge deltas. OK? We're gonna

153:09 to talk about deltas and more specifically and tide dominated deltas tomorrow after the

153:19 . So that's it for today.

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