© Distribution of this video is restricted by its owner
Transcript ×
Auto highlight
Font-size
00:03 Now we're recording. OK. I of glossed through this because I was

00:12 of uh lost my marker on But um basically, when we

00:17 we've gone through some basic terms, know, I wanted to bring up

00:21 and the fact that grain size didn't a lot to do with it.

00:24 , but uh and then after when we get to reservoir rocks,

00:27 just look at a few things in few more in a little bit more

00:30 , but it kind of went through one kind of quick because I was

00:33 to figure out exactly where I was all this and I'm exactly where I'm

00:37 to be. Uh But one of things that we were trying to show

00:41 here was that um uh these were end members here uh in the

00:49 And uh this is the most uh , more or less the Cooper River

00:54 bringing most of the down. And was the closest to uh ocean in

00:59 of those uh fast uh the amplitudes those last harmonics. And uh and

01:05 the, the uh 14th harmonic. uh we saw similar things in some

01:10 the higher harmonics as well. Uh if you look over, see if

01:18 can get this. You look right , you know, here we have

01:26 coming in in the channel and uh can see all these sands are going

01:31 here and then um the Cooper uh you can see going all the

01:37 up the Ashley here with sand and uh the marine entrainment and that,

01:43 sand is marine sand. Uh This looking symbol is greater than 67% ocean

01:50 sediment. And um and here uh it gets kind of shallow, the

01:59 it's sort of 50 50 but then up up the channel on the Cooper

02:03 uh gets farther up uh in And of course, we had um

02:10 this is the grain, the sand particles. And then if we switch

02:15 um the silts and see something similar for this mass, that kind of

02:21 was stuck up here at the bifurcation the, one of the uh the

02:27 and the uh excuse me, the and the Aisling. And uh here's

02:32 Wando over here, but you can that uh whatever was holding up a

02:36 amount of that in the silts is a little bit farther out over

02:42 And part of that's because um the are deposited at lower energy. And

02:48 it's a different uh sort of flow for when it's gonna fall out.

02:53 uh it was interesting that a lot the silts set it up along the

02:56 banks of it as well. Um , uh it all had a lot

03:01 do with the dynamics of the but it was, uh it was

03:05 clearly indicated did a lot of the . It's coming into the harbor and

03:11 size of silt and also the size sand, sand size particles which are

03:17 all the way up in here. you've got some silk on the side

03:21 sanding gets way up here. Uh Corps of engineer proposed uh red diverting

03:27 Cooper River which was already a diversion uh the river and it sent it

03:33 to the San San River. It a billion dollars and it cost them

03:39 billion dollars to do it. And what this shows you is that entrainment

03:43 what's really filling it up. And is what they're really uh had to

03:49 excavate. And it was also uh their biggest problem is. Now,

03:54 they did the red aversion of the of the, of the Cooper waters

03:59 came down uh Lakes Mulry and uh they sent him back to the

04:05 River drainage basin where there was a where you have a lot of uh

04:09 during the spring. But uh uh cost a billion dollars. And after

04:15 did that project, it didn't do good turns out. 10 years

04:19 it wasn't any better and 20 years it's not any better. And now

04:23 , uh, quite a few years . But, uh, the,

04:30 , the sports, the sportsmen and of, uh, of South Carolina

04:34 all the canals and stuff that they to build and, and the waterways

04:37 went with it to, uh, get into things, it,

04:40 it disrupted the Biota too. And Cape Romaine uh harbor, which is

04:45 a natural harbor. It's a wildlife . And this, uh this

04:53 uh you know, kind of how plot it up 100% ocean where the

04:58 is on the 14th third line uh , are no, um at this

05:05 of it. And then, and then as you get more and

05:09 , um less and less ocean, gonna get more and more of what

05:13 the river. And uh the funny about this is we looked at the

05:18 and, you know, you how sometimes when you, when you're

05:20 to prove something scientifically, you have go to a lot of work to

05:24 it as it turns out the sand and these samples, what do you

05:29 was obvious about the sand grains in samples? They iron stained their iron

05:41 and all the santa grains out of that were from the ocean. Turns

05:45 they were crystal clear to uh to , a little bit, uh,

05:52 from a wave impact. And, , and you can imagine,

05:58 if we try to do this by counting the number of, of,

06:03 , iron stain grains versus the number , of uh nonstained grains, we

06:08 would have come up with the exact results and it would have been a

06:12 quicker because back then, uh, didn't have a lot of the tools

06:16 have. Now, we actually had hand digitize it. We had

06:19 um we'd have sand grains on a and we projected it on a,

06:25 a digit uh digitizing table. And and so there were electronics underneath the

06:31 and it could pick up where you put in the pin and it would

06:34 it that way. OK. That all be automated today. OK.

06:44 , you know, a lot a lot of uh the porosity,

06:46 and permeability that develops in um resource has to do with the fact that

06:51 of the oil has been expelled and of the oil has escaped and it's

06:56 this porosity and, and uh forth uh system that can allow uh some

07:03 some of the oil that might be around here or even just around this

07:08 get into that, that flow system get away. And so uh it

07:13 of uh um a reservoir that's been oil and gas, it's gonna have

07:20 little bit of an open framework just it's gotten rid of some of the

07:23 that was in, its turned into gets pressurized when it goes from solid

07:28 li liquid and uh and expels but eventually it's gonna be leaving uh

07:33 space in there for, for uh still under pressure going from solid to

07:39 phase and uh being able to move the pore system. Ok.

07:50 um most of what we look at uh I see a problem here again

08:14 did it go there is get up of there? OK. Well,

08:41 put, I didn't put it there there it is. OK. Um

08:48 uh most things are transported by Um And uh gravity flows uh many

08:57 ago, uh we, we knew flows were happening, but we didn't

09:01 the uh a lot of the um systems related to turbo. And uh

09:09 basically had one model that was a for model and uh and everything was

09:15 to fit that. Now, we no less than 500 models. Uh

09:20 of the most interesting things I found uh when we started to uh

09:26 when scientists started to investigate turbine plus that they realized they were more complicated

09:32 some very simple things like the delta . Uh delta model, we had

09:37 things that were dominated by the fluvial , dominated by the waves were dominated

09:42 . Uh uh So um, so had these things actually on um,

09:49 the different uh systems and, and so it's kind of an oversimplified

09:56 , but models are oversimplified on And so you would have a lot

10:01 oversimplified it. And then they got where, uh somebody who came

10:04 came up with a system of about of submarines that can turn into and

10:11 the person came up to, the came up to 40 the person came

10:16 with, I think they, they over 200 miles to um and but

10:25 fans rather and uh and so it's it's pretty and uh but the same

10:31 is true for delta, the complexity deltas is, is massive. And

10:35 although we, we do know that three things that they put on a

10:41 uh and help you lump them in categories and give you sort of a

10:46 model. They're never sufficient in terms all the details and, and the

10:50 the faces are developed around, around mass of sediment, uh that's found

10:56 accommodation space and it has a source sediment. And, or uh

11:00 tide is the other thing that uh it, terms of the uh the

11:04 and arrangement of the deposits you get the water reaches uh the uh ocean

11:12 . And uh we'll be talking about a little bit later on. Tries

11:17 say too much, too soon. ? Here is something that I

11:23 Um And of course, there's also ice transport and stuff like that.

11:29 uh in the oil business, most what we looked at is predominantly uh

11:34 to be deposits that are moved by water. And then there are

11:38 AO deposits, sand dunes and stuff that that makes some pretty significant to

11:44 post are a lot better than what see uh with uh water transportation.

11:51 is Helstrom diagram. Tell me you see this. And Bill de Praise

12:01 , how can I get rid of ? You don't remember this? I

12:10 sat in his class multiple times. he decided not to show it

12:16 So what do you think? Uh do you think about this is uh

12:21 know, here is velocity first, is going up and uh and uh

12:33 size is getting bigger in this So bigger things need higher velocities,

12:43 ? One second. So, um then if you drop that uh velocity

12:50 these certain critical levels, they drop your deposit. It usually takes more

12:57 to make things erode. This is erosion line then and they stay,

13:04 stay floated even at a slightly Once, once that frictions overcome,

13:08 drop out and at this point, all start to drop out. It's

13:12 dash line because shape can have something do it and density can have something

13:15 do with it. But based on size in general, uh, this

13:20 , this is how it works the thing with this. So,

13:23 here, uh, bigger things fall sooner, right. That, but

13:32 happens over here when we get to , this what's happening in the

13:50 So when we get smaller than, , uh, some of the,

13:55 , medium size silt, the stuff stays in suspension for a long

13:59 So it doesn't, doesn't really just out, it will settle eventually if

14:03 , if there's no current, but it's still moving around, it's not

14:07 drop out. Uh Again, you the velocity and uh and you can

14:15 from this point on you increase the and you can see bigger things get

14:21 over here, you would think decreasing vastly get smaller things, but you

14:25 have, then you can't, you erode things uh that are fine grain

14:32 easily as you can, things that in. Um In other words,

14:38 a window here that's between things that kind of loose and more easily eroded

14:48 things that are um small and very to, uh it's a hard,

14:55 hard to erode this as it is move this and that little picture right

15:06 is the whole reason why we have and systems this, this has to

15:13 with why shields are widespread. This to do with if the energy is

15:19 enough to move this it's gonna move . The sorting is gonna be

15:26 Um This is also why rivers and streams are, are they channelizing the

15:35 because the mud is more resistant than sand? The sand at this

15:42 all of the sand at this all of the sand um is,

15:49 basically, um, you look it's, it's in transport so the

15:54 can keep moving. The sand gets at this velocity. It stays in

16:00 um uh until you know, you to drop down into, into these

16:06 over here. So if you drop to one of these velocities, then

16:10 fall out. But sand, this , we call sand, the coarse

16:16 and there's kind of a plateau right . Most of the sand size particles

16:21 the easiest to motivate the last And that's why sand moves so much

16:29 sand moves so much if it's Uh when you're on a beach,

16:34 the sand is moving back and but the clays are still in suspension

16:39 they just get winnowed off. Any clay that makes it down there

16:43 gonna still be in the water column it's gonna be winnowed off. And

16:47 it's concentrating the sand. In other , this diagram explains to you why

16:53 often are well sorted. This explains conglomerates are never well sorted. This

17:04 why clay is the confining uh material keeps channels, scanner and channels in

17:13 in other words, they have things there's play signs and the point,

17:17 point bar there's deposition because the velocity down. But the only during flood

17:23 you get erosion over here on uh on the thing. And,

17:28 , and that's because it's hard to . It's mostly like playing plays.

17:33 there's the flood plain, you the river fills up when it

17:37 the planes hit, covered with this , which is hard to. And

17:41 it's actually, it's like a, natural instructor of uh of all these

17:49 um features of a river uh of pluvial system. And it's pretty amazing

17:54 it, it also relates to, don't have time right now. But

17:58 you come to uh the velocity dropping , when somebody comes down a river

18:05 hits the ocean, that also explains sand falls out first and the place

18:09 keep going 100 miles off. And helps winnow it too if uh you

18:20 won't, won't ever think about it much as I did. But if

18:23 do, you'll, you'll get the that a delta is almost like a

18:26 creature even though it has a lot creatures on it. But it's

18:31 it's almost a living breathing thing that builds itself and repairs itself during flood

18:38 , it repairs itself during storms, builds up sand uh that acts as

18:43 barriers. It's uh it's just an thing. And it all has to

18:46 with, with uh the difference between two lines with big things which were

18:55 close transportation and deposition are very close , but they're very far apart

19:06 And guess what? It has a impact on porosity permeability and good sorted

19:13 . And it, it always, always bothered me. Well, if

19:15 doesn't make any difference, why is size so good? This is why

19:19 size is so good because of the uh uh things that are transported by

19:25 . Uh In one case, takes lot of energy to move the big

19:28 . In another case, it takes lot of energy to move the

19:32 the fine grain stuff. But once in the, it's in the water

19:36 , it keeps moving. When, this slows down, it falls like

19:41 rock. Ok. So uh we these different things in uh sediment transport

19:53 um as, as, as it in a um in the oil

19:58 it's not so important uh that we understand this but, but it has

20:03 lot to do with uh why the center of the channel is full of

20:08 horse or green things with bed Uh Then if you get uh if

20:13 come around the bend, it starts drop out the sand size particles on

20:17 point bar, things like that. you're getting some of these faces are

20:21 developing because of it. And the load is why a lot of times

20:26 clays, once that clay gets it goes straight down to the drainage

20:32 and lots of mud comes out of Mississippi river is probably 95% mud and

20:37 rest of sand, it's, it's amazing amount of, uh, don't

20:41 me on that, but it's it's a huge amount of mud,

20:44 , coming down that river as opposed , uh, sand and it's,

20:49 a mud rich delta and that has lot to do with the way.

20:52 a pro delta clays and, and that the, that the,

20:57 pro grading sands actually build up on of which creates all sorts of actually

21:03 and whatnot with mud diapers and that of thing. Ok. Um,

21:11 flows are a really different thing. , um, and, uh,

21:17 you've ever seen an avalanche of, , of snow, it's sediment is

21:23 much the same thing. There are densities, different, um, carrying

21:29 . But, uh, but at same time, if you've ever

21:32 uh, ice avalanche when it breaks , it's like one solid slump,

21:37 of like a solid thing. And it starts rolling down the hill it

21:41 up speed as it picks up it starts to have this thing.

21:47 , um, it kind of looks it's plastic and it kind of does

21:51 thing and if it's got, if full of water, like what sediment

21:54 be, it's very plastic in nature some point in time. Um You

22:01 imagine if you're doing this, the are pulling further apart and more water

22:06 it's, um, it's called dynamic latency. And so you end up

22:11 a dilated dilated mass and that dilated is just a jumble of things uh

22:18 down, but it's still, it's got low lungs. It's, it's

22:22 of gone like this. So it's spread farther and farther apart at some

22:26 in time. You know. Um let me just explain. This,

22:32 me a while to, we know is a straight line, right?

22:36 is also straight flow line of all flow lines are moving together. In

22:42 words, some parallel, it it might ripple a parallel. And

22:47 so what happens is once these flow cross each other, they get t

22:52 when it starts to go and uh what happens when you get that turbine

22:58 . And if it's coming down off a pretty significant uh shelf edge like

23:02 Gulf of Mexico East, uh the of 100 miles, 200 miles

23:09 And uh the way they were first recognized was um we had uh we

23:15 have a lot of cables but we to have nothing but cables to go

23:18 the ocean uh to communicate across uh Europe. And uh sometimes they would

23:24 in the middle of the night. , uh, it took him a

23:27 to figure out they weren't monsters, weren't sea monsters that were down there

23:30 the plugs. But, uh, was turbidity currents that went, ripping

23:35 them and, uh, just, snapped them sort of like a tornado

23:40 us. But not, not quite . Anyway, with all this

23:48 Yeah. You know, in, , in addition to, um,

23:55 and composition, we also have sedimentary . And these are a lot of

24:00 sedimentary structures that we get. And are kind of small scale things for

24:05 most part. But you know, else is uh incredible about sedimentary structures

24:11 that they absolutely definitely have an impact uh and uh all of all of

24:20 ripples and uh these other types of uh laser and betting and cross

24:28 Uh because, because they have um , essentially, they have not,

24:35 not, I wouldn't call it stoic , but they have structural architecture that

24:40 it possible for um laminate to There can be uh baffles and barriers

24:45 flow and that's really the key of all. Uh And what I'm trying

24:51 get out too is that is that all of these little details about sedimentary

25:01 are important to a reservoir geologist. uh if uh if you have a

25:07 big uh homogeneous sand, it's Uh But if you, if you

25:12 one that has ripples like from the off uh off Galveston Island. A

25:19 of these uh boundaries between these uh that are forming uh will not be

25:27 or barriers. But if you were this off the east coast, you

25:30 have heavy minerals in there. It's vary. These heavy minerals can turn

25:34 the seine and seal it off and it more difficult for oil and

25:46 And um this is just showing you the velocity has an impact on,

25:52 uh the types of sedimentary structures we and the size of them. And

25:58 you know, to begin with, get ripples, then we get bigger

26:00 , we call dunes and uh then get things that are flattened or washed

26:05 fins and uh and then we get uh to a point where we have

26:10 plainer beds forming and uh and sometimes standing waves or anti dunes. And

26:19 this is uh just showing you how some of the uh lower velocities

26:25 form ripples the way they are. of course, turns moving in this

26:30 , we get, you get asymmetric ripples like this. And these are

26:36 two dimensional ripples. And then uh if they get a little bit

26:43 you know, we can have ripples on top of games and this is

26:47 two dimensional. And um to be dune is not that big. And

26:56 always thought of dunes as something that like a big, a alien

27:00 But uh but dunes can uh aren't smallest of dunes are not that

27:05 And, um, and uh here could see ripples and of course,

27:10 said that here's some really big dunes uh these are mega ripples uh between

27:18 two extremes. And, uh and the thing is, is that dunes

27:24 , can get to be uh very . And uh this is just showing

27:32 that, you know, one of reasons uh geologists like ripples is because

27:36 can tell whether they think they can whether it's tidal or not. And

27:40 normally get these asymmetric um ripples like . Uh And basically, uh you

27:50 , if, if you just have going in one direction, you're gonna

27:52 those asymmetric ripples, it's gonna be in the direction of uh the

27:58 But the idea is that if you the tides going in and the tides

28:02 out, it kind of even it doesn't always happen that way.

28:05 what happens is uh the tide comes and creates a normal uh two dimensional

28:11 going in this direction. And then it starts to come back out,

28:15 starts to erode this side. But when it gets shallower, it,

28:19 uh kind of erodes it on the to these little channels here. And

28:25 sometimes people step on the sand and help it get out. But uh

28:30 it's, it's sort of a, slight complex. It's not just the

28:34 going one way and the tide going other way. It has a lot

28:37 do with the way the water When the water level goes down,

28:40 gonna um circulate around the, around uh these little spaces here in

28:46 in the um between the ripples. , uh I, I think this

28:52 is from something Hank Chaffetz uh published in a Paleozoic uh title uh sandstone

29:00 somewhere here in Texas. It's been while since I've looked at that

29:05 And of course, you know, start out with these lower flow regime

29:08 where we have straight crested ripples, dimensional features. And uh eventually we

29:14 get things uh where you get these more sinuous ripples and they become three

29:20 . In other words, uh they're just stacking up like this, but

29:23 also cutting down into the ripples underneath . And uh and they have that

29:28 feature uh with it. And um there that is, and here are

29:38 uh big uh he says, large uh ripples uh but they're 3d,

29:48 actually dooms. Uh They're, I this is from Bill De Prey.

29:51 you see in this picture? And this is just showing you how

29:58 you know, they cut down into , as they progress, they cut

30:01 into the ripple before them. So , there's not just a ripple on

30:05 of a ripple, the ripples that cutting into the. And um uh

30:19 you just look at this, this probably some of our Gulf Coast

30:24 So there's limited things, but you see a lot of lamination in

30:28 And if, if something falls this course is denser but finer

30:34 it could cause a baffle or if , if it's uh like a heavy

30:38 , it could actually uh create cements become a barrier. And uh iron

30:44 one of the most famous things for . This is uh a picture I

30:48 in the Red River and uh north Dallas. And this is um you

30:56 see here some of the um uh uh had concentrations of iron along

31:02 And sometimes these things, sometimes it be the exact opposite of what you're

31:07 of. Sometimes it's more porous and uh water that has a higher concentration

31:17 iron is passing through it and it out. And other times it can

31:21 , there's a concentration of grains that uh higher and higher and uh we'll

31:27 that homo just because the iron is right there in the first place.

31:35 here's an upper flow regime uh thing you can see iron staining that helps

31:40 helps you actually see the laminate. many have you ever gone to

31:50 OK. When the tide goes um when the tide goes out,

31:56 you don't even have to have a an out wash. Um this

32:03 you could also see it on the along the uh the coast when the

32:08 come up and they break, they that velocity and then they start going

32:12 really, really fast and they get really high flow regime. One thing

32:16 didn't show you in the flow regime is is when the, the depth

32:19 the water goes down, the flow also goes down because you're kind of

32:23 the flow. And uh so the the depth of the water goes

32:28 the flow regime goes up and uh that velocity. And so, um

32:34 is more like what I see Um this is from South Carolina and

32:40 normally um Annie dunes will um will like this. They'll, they'll be

32:49 like this. And uh you're sitting you see the wave coming in and

32:53 breaks, you know, it'll go like this and as it starts to

32:56 back down, uh you'll see exactly what you see in this thing that

33:01 just showed you in this picture, call these uh standing waves because

33:08 there's a wave, it's just, just uh going down in the uh

33:12 happening is if you're standing here, flow is going that way. But

33:18 dunes migrate this direct and the dunes back filling on the back side,

33:24 is why they're wrong. So uh it gets over this dune, it

33:28 down, but that particle it comes here hits the back of that

33:34 And so they each keep building out this and you get that standing wave

33:38 allows that to happen, sort of you know, you get that ripple

33:42 it creates a, a, an and a break, some acceleration and

33:46 and the, the ripples that the actually, you can actually sit at

33:51 beach and watch yourself come climbing up the base of the beach beach cha

33:57 uh the water is going that way water's going out, sand is going

34:01 . The word ripples are coming in um go down to the beach and

34:07 if you can find that and then uh grab somebody and show it to

34:12 . So it's kind of freaky. that was uh when I took freshman

34:17 the beach, that was one of fun things I had to do when

34:20 went out, there was look at dunes coming up the uh shore

34:35 OK. Another type of uh uh under uh ripples. And uh you

34:44 , we had ripples and cross cross . And uh and the other thing

34:52 we can have is um there, is uh we can have leisure in

34:57 betting and that looks like uh this um this one is called Blazer,

35:17 one's called Lenticular and this one's these are N members. This one

35:24 more sand, that one has less . But uh what are you

35:31 What do you think causes a structure that or better? Yeah, let

35:48 ask you. Did you guys realize uh we use sedimentary structures to determine

35:54 environment? Are you aware of OK. But it's really complicated.

36:05 . So um but be, but you answer any questions, just look

36:10 that, which one of those do think would have the best uh permeability

36:14 porosity? A B or C? many people think the best porosity would

36:20 porosity and permeability would be C? about B eight? OK. So

36:31 is it, so that's, that's I'm showing you this picture uh wavy

36:37 uh different types of uh laser and . Sometimes we just call it wavy

36:44 that's the middle one. Uh wavy uh occurs. You remember Hilton's

36:55 So what do you think this means it alternates between sands and, and

37:02 ? Excuse me, it could be . Yes. Sometimes these are tidal

37:10 . When do the clays fall It was title one with the fall

37:28 positive. Yeah, it's for so it, it waxes it,

37:33 there's a point in the, in point in time where there's sort of

37:36 standstill sort of half between high and tide and, and that's when it

37:42 out. That would be, that be what would happen for title

37:47 ok. This can also happen uh a um uh in and around crevasse

37:55 . So you have a levy deposit water just goes a little bit over

38:00 edge of the levee deposit. It's pull a bunch of sand in some

38:03 will go down there. That water gonna be muddy, right? The

38:07 is gonna drop out right away, the muddy water that builds up and

38:11 settle down and then maybe the flood kind of tip over the edge

38:15 And so, so you might uh maybe more on this end between

38:20 of standing water that let the clays out and periods of water flowing over

38:26 edge of the levee, bringing sand it. Ok. Uh Can you

38:32 of anything else? So we got , we got tides. Fluvial systems

38:37 be a long way away from the and alluvial systems get closer. Excuse

38:43 , loal systems can get close to away from the tide. And

38:50 excuse me. Well, I was talking about flooding events. So,

38:54 , that, you know, that's the water comes over the edge.

38:58 uh and, and because if you AAA levied channel, it's more likely

39:04 , to be something like that. could also have some of these

39:08 Um, this is very similar to you might see in a rated stream

39:14 . And uh and what, and thing that another place that you could

39:18 these, uh, when you're, you're drilling well into something that's relatively

39:24 water, you know, say at 100 m deep. Um, or

39:30 little less, you may see something looks like this. And what do

39:36 think would cause that? Uh, , there are, there are,

39:53 are part of the Boma sequence actually wavy eliminations in it. Yeah.

40:00 , uh, but I was thinking something else. I'm just thinking of

40:10 , say if you're on a coastline there's a lot of storms, storm

40:14 wave based storm wave based and do most of the time, uh fine

40:19 stuff settling out. But when storm base comes in, it stirs up

40:22 sand and it winnows out some sand of the, you know, there

40:26 be sand and place it on the , it winnows out that sand,

40:31 it gets the clay out of it then you have a nice little sand

40:34 and uh so you get this type a wavy lamination. So, uh

40:38 on what coast it might be 50 deep, 25 m deep. But

40:43 you might see stuff that's um deeper that, that storm wave base and

40:50 got mostly clays and silts. But when you get to that wave

40:54 you'll start to see things that look this. The storm wave base good

41:03 was going on in the car well, it has to do with

41:15 and uh but, but um but what you said, this could be

41:19 very easily be a graded stream, it could also be a very sandy

41:23 stage on a, on, on the levee of a river.

41:28 uh but normally uh a river is look something like this. Tides.

41:34 depend on what's, what's in, in that part of the, of

41:38 channel. You could have any of kinds of things. And uh uh

41:43 I, I don't know if this the point you're making the point I'm

41:46 to make is without any other It's hard to tell exactly what it

41:49 . You have to have some kind relevant uh information. If you,

41:54 you know that you're in water that 100 and 50 m, uh You're

42:00 gonna see some wave wave base type like this. And, um,

42:07 on a, on a larger the Chandler Islands, you have this

42:12 mud delta called the Mississippi River. program it out. It's got little

42:17 with sand, lots of faces to . And when the, when the

42:20 coming in dramatically new and so the islands are big loads of the delta

42:28 , that river in the sand, little bit of sand that runs down

42:30 river, it just winnow down and into bars and then on a more

42:36 scale, uh a lot of when a storm comes through, the

42:41 has just starts to collect on it there's that part to collect it that

42:45 to collect the shell. And then to get, um, to get

42:52 to become emergent, you have to sort of a little bit of a

42:55 there already. So you get these sand ripples and waves uh that build

42:59 like that from winnowing out the, the low sand concentration, but high

43:07 concentration, the the storm will winnow enough sand. It starts to pile

43:12 at a point and uh and then shell hashes will get caught on

43:16 and start building up. Ok. is this one? What do you

43:35 causes this? Yeah, something that's flash event that's carrying all the fine

43:43 stuff along with the coarse grain And uh and this obviously is not

43:51 . So this might be some, shelf sediments uh that have that

43:56 they're fairly mature in a sense of reworking and whatnot. But you have

44:01 , you have shale and uh it starts to move together. It gets

44:05 that turbid flow, it's all mixed and then it starts to settle out

44:09 this grated bed. It's poorly but the grated bed goes from the

44:14 stuff to finer and finer uh poorly sediments as you get to the

44:20 So it's, it's high energy. big stuff starts to fall out and

44:24 energy drops off dramatically really quickly in finer grain sediments fall out.

44:33 Now, let's look at uh Turbin . And um so we're looking at

44:38 sedimentary structures and trying to explain some the processes, but uh these uh

44:44 i gravity flows have a lot to with it. And this is sort

44:47 a, a rock example uh where can see, you know, things

44:51 sliding down a slope, uh they're coherent. Uh Here's something that's slumped

44:57 it kind of gets flipped over. But here you have a mass that's

45:01 down and this, this pretty much be a uh a debris flow and

45:05 grain flow put together. And then you have the turbid flow and uh

45:13 of course, the turbid flow, no longer have this parallel flow

45:20 You have these turbid flow lines that together it gets roiled. And of

45:24 , you've got coarse grain, fine all mixed together and it's moving at

45:27 high velocity and that allows certain types features to fall out. And um

45:38 is uh the Bama sequence and when start getting these, these fine grain

45:44 with a little bit of ripples in , uh Sometimes uh this little interval

45:48 here looks like wavy lamination right in that, that the C value of

45:54 . But uh this isn't where the of, of the sediment falls,

45:58 it's where all the fine grain sediment out. And this particular model,

46:03 the one point on this model will us identify, oh which is the

46:12 of the record of a sub But as it turns out, after

46:18 , I more, more work, we were able to figure out that

46:23 is on the distal end of a of a submarine fan. It's not

46:29 it's not like in the submarine fans faces to them as well. They're

46:33 just all Boma sequences. The Bama is one faces on the distal part

46:38 the fan. And uh I think important to point out to some people

46:45 haven't um gotten much of a background this. I don't know. Did

46:50 talk about Turbos a lot and build price well good. And uh and

46:57 but again, uh if you can that this is, this is fighting

47:04 because this is a thing, high , a low energy break, high

47:09 , low energy break. Uh We uh we're not looking at this in

47:16 yet, but when, when we um one of the things that's uh

47:22 what did he tell you what happens a, to a submarine fan or

47:26 turbo? Does it fine upwards or of course and upwards, each

47:37 of the sequences is gonna fine upwards now. This is it the distal

47:43 if you get more proximal to where sediment is coming in, it's gonna

47:46 coarser and coarser grain, right? if I prograde something out like this

47:54 it's finding upwards, if there's another turbidity current that comes out and sits

48:00 on top of it, because this built up on something. The next

48:04 gonna build out a little bit farther the next one is gonna come on

48:08 of it and build out a little farther. And so the faces that

48:12 see here that are distal will be away as, as the turbo events

48:19 occurring. So, so it keeps further. So we have finding

48:24 finding upwards, finding upwards, finding . But when we're, when I'm

48:27 here, the distal part is farther . So you're getting coarser grain

48:33 it'll be coarser and coarser this So, so when it just goes

48:37 and then here, what, what out of this one is gonna be

48:41 than the one below it, then next one's gonna be coarser than the

48:44 below it. Not, not the of it, but the point,

48:48 part that's over top of it. a uh submarine fan deposit uh with

48:55 series of uh turbo currents is gonna each event is gonna fine upwards.

49:03 each, each element will be fining , but the, the overall sequence

49:08 be coarsening upwards. So this sequence fining upwards but and it's the,

49:14 it's way out very distal, this less distal. So it's coarser,

49:18 it's still a fining upward sequence. one is less, still uh distal

49:23 that. It's finding upwards, but coarser than the one below it.

49:26 the one below that. OK. . And just imagine how complicated stacks

49:39 these things would be if each one these is, you know, maybe

49:43 more than a half a meter you have another one and another

49:48 look at all these things that could barriers to flow and permeability and

49:56 OK. Other things uh biogenic Um some people live and die on

50:03 if no fossils they call them and and I find them interesting from a

50:10 standpoint and that, that um biological can do a lot of things.

50:16 of the things that can, you , build structures and cement things up

50:20 these can, can cause bales and sort of thing. You can also

50:25 pull organic minerals and stuff in here organic derived minerals that might react to

50:30 things and, and create cements and like that. Uh So you can

50:34 all sorts of things like that but don't know, but I got the

50:39 slide I can. OK. so uh that's kind of what it

50:47 like. And uh so these uh the bottom and uh this is like

50:53 you take one of these rocks and it up and look at some of

50:56 stuff because there are, there are fossils oh and biogenic structures that where

51:05 graze across the surface. And sometimes you see the bottom of that,

51:08 have a nice surface. And of , that could cause a uh a

51:12 barrier uh in that sense. And what this one is. And um

51:19 in some ways they can cause baffles barriers. But uh what I did

51:24 we were, we were looking at deposits, recent hurricane deposits uh down

51:29 um the island that's just south southwest uh of uh Galveston Island. And

51:40 you know, Freeport. And uh sand right here was, this is

51:46 uh micro ct of the sand. a micro CT do is see things

51:53 just a few microns. Uh but a, it's an x-ray machine and

51:57 you can, you can do a of uh so you need to just

52:02 to display very nice things or um that are um high density things that

52:09 um sort of intermediate density. And and I don't think this is ever

52:15 place of anything like this, but had one, you know, probably

52:18 by now, I get crazy I mean, and I thought what

52:22 , what if uh I took my on and moved it from something really

52:28 over here all the way from zero almost nothing. So plant material it's

52:36 be much lower density than the, core. When you look at this

52:41 , it looked like what we would call a massive sands. And there

52:45 , there were no structures in it all. You didn't see any

52:48 nothing. Uh It was just sandstone uh it was, it was actually

52:55 to keep it in, you in place, but it was,

52:58 was primarily sandstone with some, some stuff that kind of held it

53:04 you know, you, you hit like that, it could have

53:07 it would have been gone. So , we kept it in the

53:11 And so, you know, we out, we zeroed out the density

53:15 , of the core tube. Uh I thought, why don't we just

53:21 ? Just, just the image with to 1 with. And that's what

53:28 , this is, this is this is um x-ray uh micro x-rays

53:35 helping you image channels and portraits of . This is all ferocity in this

53:43 . Everything outside of this would have seen or been seen. Some of

53:49 things might be actual routes, some them might just be spaces or spaces

53:54 are open right now. But even the, even if the roots uh

54:00 , there's gonna be that big space . In other words, there's all

54:03 different but very complex series of channels through here. It's hard for us

54:10 understand exactly what's going on because this this is looking through something that's about

54:16 , that big. And so you're the little channels here here here and

54:21 all over layered on top of each . So it's a three dimensional thing

54:26 you see a lot going on. what you can see is there's a

54:31 of something really big right here, is interesting, which could have been

54:36 surface. In other words, this have been um the, uh,

54:43 flood of the hurricane and maybe coming out, this might have been

54:48 uh, the, of the And, uh, I, there's

54:51 enough there for me to say uh, one thing I didn't have

54:54 to do, we have the machine there now, but when I was

54:57 on it, it was a Uh, but another thing you could

55:00 is you could, could, uh, with the computer or

55:05 you could, you could actually take volume that we had. Let's

55:11 get a clear picture of what's happening the way through it. In other

55:16 , if I just have the outer or four millimeters here, uh,

55:21 know, 34 to 56 of all noise and it would disappear and we'd

55:26 able to see, see where the is and we can move back and

55:31 in it. But I, I had time to, it's really expensive

55:35 , to work, but that's, , I think that's really interesting.

55:43 I think that's something um that we to consider too when we're thinking about

55:48 complexity of poor throats and, and channels through something that looks like a

55:56 porosity sandstone or higher. And uh got all these channels in there that

56:02 uh uh probably create even more porosity more permeability. OK. Then we

56:09 to bedding and lamination and um Laina less than a milli a centimeter

56:16 And uh uh now beds can be as small as that and go up

56:23 , you know, um, meters meters, hundreds of meters thick

56:29 And uh, but all beds have surfaces and they're generally flat in

56:35 And uh these are some fine grain . Uh This is something uh from

56:42 beach slope, beach facing, probably on the Atlantic coastal plain because

56:47 can see the laminate and uh, know, you take a, you

56:50 a, you dig a hole and take a machete and you kind of

56:53 it and get it just really straight that. This one looks like they

56:57 have had a, an air hose , and uh, blew it a

57:00 bit to, uh, to get of the, the, um,

57:04 parts of where the heavy minerals are stick out a little bit farther.

57:08 , uh, and this is a deposit that's very similar to it.

57:12 smaller laminate here. And uh, , when you see something that looks

57:19 this, say, say it's a organic rich, really dark sail that

57:27 a dark shell and you saw it that. Um There's a good chance

57:33 have high to CS. But what you saw a shale that's just as

57:37 as this. If you saw that relates to what I was just talking

57:49 the books. Bye. Ok. , um, the reason we get

58:14 lot of these, these are barb lamination from probably a lake deposit.

58:19 um and so um different things are the water column at different times and

58:24 forms these kind of lamination. But , if you have of us that

58:28 falling to the surface, now there's be uh seven falls, some organic

58:35 , seven falls, some organic So if it's undisturbed, you're almost

58:40 gonna see la. Now in this deposit, it's probably like this because

58:46 water and this was in oxygen, low oxygen levels. And that would

58:53 there would be nothing falling around that biogenic starts. And if you get

59:05 well, is it C Wilson? think so. Um he was looking

59:10 the Midway, some of the midway and they're really dark and very organic

59:15 , they have to CS and the of and uh he was sort of

59:26 and we had a core that we looking at and we thought it would

59:29 very helpful. But when we looked the, the really dark sales.

59:34 , no eliminations at all. The for that is the iota as it

59:40 being deposit, we eating all the material and it was stirring it up

59:44 some. So the sediment was getting with the, with the organic

59:50 So if that was going on whatever is discriminating this, the uh

59:56 lemonade would be mixed in with with the background mass and you wouldn't

60:01 any lamination at all. And, , you know, they're only,

60:04 may only be eating a little bit a time, but, you

60:07 over hundreds of years and whatnot or uh they would be consuming most of

60:14 organic material. It might still end with a dark shale. It's really

60:25 . So when you're looking for source , you're hoping there is no bio

60:30 , you're looking for uh water conditions restrict the flow and enhance the probability

60:38 having low oxygen levels. OK. so, um, this is just

60:56 of an end slide, but this showing you this is actually, uh

61:01 talking about beds eliminations. Um Here's , here's a limestone bed, here's

61:07 shale bed, here's a, a bed, limestone bed. So I

61:11 to kind of see what I a bed looks like in, in

61:16 a smaller sense. And, uh could even call something like this unit

61:24 here that seems to have a lot limestone in it. And that unit

61:27 there has, seems to have a more shale. You could, you

61:30 actually say that's a bed of this and this is a bed of that

61:36 rather than just this being one two beds, three beds. It

61:41 be one big bed down here that more carbonates in one big bed up

61:47 and has less carbonates, by the . What do you think the TOC

61:58 in those rocks or those gray What would you guess the TOC would

62:06 in those gray rocks? You can't the fine scale of this one,

62:13 you can, can you kind of that there are lemonade in it so

62:19 the to CS of these were probably 18 to 20% and no bio turb

62:27 when these were deposited, uh they being deposited in a water depth,

62:31 have to be too deep. You a chemo cline. Uh The oxygen

62:35 much gets used up below the chemo and, and there's no way to

62:39 overturn it like a lot of lakes or they'll overturn when the density of

62:43 water shifts in the winter and in , in the spring? Ok.

62:50 we're done with that. Any comments or thoughts? Do you um

63:01 you getting a picture that sediment technology really important to reservoir geology? Hope

63:16 . Ok. You guys just had course in this So I'm gonna,

63:19 gonna breeze through this, probably. . Ok. Yeah. Anybody want

63:26 take a small break. It's been an hour, right? Yeah,

63:30 think in the afternoon you almost have break every hour. Yeah. Whether

63:35 for the bathroom or whatever. The power cord wasn't turned on.

63:57 was approaching imminent, uh, Ok. And, um,

64:14 this is just showing you some of , uh, fault traps and,

64:20 this of course, is a normal here. But uh you can see

64:24 the up front side, uh we've um the trap a lot of times

64:32 on the, on the, on side. Of course, the Strat

64:34 have to be going in a different like this relative to the fall.

64:39 uh over here, you can see thrust uh that creates some structures.

64:43 , did you look at a lot different things like this in uh in

64:47 geology? Because, because that's the , the only one we're gonna look

64:53 there this, but there's a lot configurations. This is um this is

65:02 a plaster experiment to try to recreate rift valley that looks similar to um

65:07 where they have uh some of the uh stuff. And um I'm not

65:15 , I don't, I think this , I think this is in the

65:19 Rob and, and uh uh but very similar to the central grob and

65:24 a lot of ways and it just you how the faulting occurs. And

65:29 course, you can see that um you get these offsets so that there's

65:36 for some flow to go across some them. And in other cases,

65:41 uh there's limited flow that could possibly across it. Uh in that

65:45 if these, these uh dark things to be reservoir rocks. And um

65:53 it, it is very, uh a cartoonish type thing. So it's

65:57 to tell exactly what's going on in sense. But I think what's interesting

66:00 this model and this is a part reality is, and I was trying

66:05 point this out, these things end becoming mountain peaks. And uh I

66:10 when you look at a model or a diagram like this, you

66:13 really think of, of that as a mountain. This is a mountain

66:17 and that's a deep, that's a hole and a lot of the combination

66:21 and something could erode into your fans , or fan deltas. They come

66:26 off the um off the uplift and it in. And uh that happens

66:30 lot in uh in uh in Lake and uh and the other East African

66:36 lakes right now. But it happened all of these things when, when

66:39 when the rift was pulling apart, early on in the development of the

66:44 Sea, which, which is sort an arrested riff um system or an

66:51 uh spreading ridge. Ok. Here um just showing you um how

66:59 you know, with, with uh seismic, we'll, we'll see a

67:05 of these bigger faults, but we miss uh some of these smaller faults

67:09 of course, the 3d uh seismic , uh they're, they're working on

67:14 to filter attributes uh so that they actually see some of these smaller faults

67:20 is uh or what they were normally them as lines until they know what

67:25 , what's actually causing the lines. you can do things even like this

67:29 the gravity and Magnetics. And um always uh show this to make sure

67:40 remembers what I um what a normal is versus a thrust fault. Uh

67:46 think it's important to point out uh there's a lot of different symbols used

67:53 uh a lot of times thrust faults use this. Um Here we have

68:03 , this one's kind of pixelated, it's the same kind of thing.

68:06 This, this is uh out of of the same books. This is

68:10 normal fault. This is a, thrust fault. Usually the ones that

68:14 the, the pointy diamonds are gonna uh thrust. And of course,

68:19 as you can see here, you , here's the, here's the foot

68:25 and this is uh the one that's which way is the thrust going?

68:42 doesn't even show you all these stupid , but this is, but

68:52 the arrows are usually gonna be something gonna be flinging uh to the dip

68:56 the, of the bed. uh the thrust fall, this is

69:00 be dipping down the or the dip the fault or here's the dip of

69:03 fault, but it has to, this is the wall and so it

69:07 to come up over top of And uh I mostly work in um

69:15 have work and when I did hand maps, which by the way,

69:19 got pretty good at um this is of the symbol. Sometimes the symbols

69:25 just have a box like this. times, they'll kind of make it

69:28 a little bit three dimensional like And uh but again, this is

69:32 down block, the fault is dipping way and it's down and this one

69:37 up. So it has to it has to be like that or

69:42 the normal, I don't have a normal P I. Here it

69:46 here's the normal I remember as an then you just, you just

69:58 well, and it's, and it's of reversed in a way.

70:01 it is reversed. That's why it's reversal. And um and the um

70:08 people have trouble understanding why it's a wall and that's because um this is

70:17 , a reverse or press, but is gonna be the hanging wall because

70:21 above your head in the football, the one. So if this is

70:26 football, this thing up and I another thing uh that helps uh people

70:38 what's going on even three dimensionally Yes. Um And uh if

70:45 if you look at um this just if you look at the block

70:52 itself, this is the shortest part the block. This is the shortest

70:56 of the block when they move like , the short ends get closer,

71:01 means the crust is shrinking. And in this one, um this

71:08 goes down, this one goes up here you have the uh the

71:14 the long parts of the blocks are close, which means the crust is

71:23 and it's just a, you a little thing that helps people remember

71:28 again. Sometimes things are so It's easy to get it backwards 100

71:31 80 degrees. And here is an interesting map. And um if

71:42 were mapping something like this in the , you wouldn't see this, you'd

71:48 see something that was flattened off and see the top of this sand and

71:56 a little bit farther up in this , you'd see the top of another

72:00 . But this is a surface that been pen. And that's why uh

72:05 uh mapping can often be confusing to with a lower than surface. It's

72:10 of a different game you, you're to look at say a surface that

72:14 deposited at a certain point in time it's moving up and down. But

72:20 um field mapping, you know, have a whole bunch of layers and

72:24 they tilt like this, they get pena plane off and you see,

72:27 you, you're gonna be marching from youngest to the oldest. In this

72:30 , it was dipped in the other , You see the opposite. But

72:33 this case, we're trying to look one surface of one age at a

72:37 . In other words, one of layers at a time, not the

72:41 of what it looks like when it eroded. And uh that's why three

72:45 can be uh a little bit uh complicated than what you see. Uh

72:52 you're mapping things on the surface and cross cutting relationships can be very

72:57 And I I you have to have to show people what I mean.

73:02 the uh uh when faults cut, go against the uh when you have

73:10 fault here, a normal fault here a normal fault here like this and

73:17 the um the surfaces uh normally would offset by the um by the younger

73:26 , but it's the opposite when it's , when it's just a surface.

73:31 , the only way to show it you would be with blocks. You

73:37 , you think, you know, normal cross cutting relationship in a

73:44 not on a surface but a Uh, the, uh, the

73:49 fault is gonna cut the older But in, in the, in

73:53 case, it'll look different the opposite you're just looking at a surface which

73:58 is a surface, this isn't in plane surface and it's not cut in

74:04 rock like this. It's something that's across at this point in time.

74:11 , uh, so what you see again is, uh this is probably

74:15 normal fault and uh see, we to assume it is, I guess

74:32 here, this is deeper you, a normal p so, um this

74:38 the uh the hanging wall block and a football block. Is that

74:45 You got it right? No, got it wrong. Um This

74:51 this side is sliding down, this is popping up. So this would

74:55 the, and um this, this kind of uh different from what uh

75:06 see a lot. I see it the opposite of that, which is

75:08 it just looks a little funny to . Uh I normally see things traffic

75:13 the uh the down the and here , um you can see the closure

75:22 . You can see these complex uh these complex uh a faults coming

75:29 of here, but uh see the of this vault right here, it's

75:35 a surface in which right? Do think the fault is curved. It's

75:51 . It is, but it's also that it's relatively straight because you're,

75:56 walking down, you, like if a straight fault here, this structure

76:00 actually walking down, dip along the . So like if you have a

76:11 to pick up a book, what at it in cross section, here's

76:29 fault and it's a straight and you uh features, one of the contour

76:35 there with the other contour, one that's way up here and uh 10

76:53 conor on the system. So that's 40 10. So something's hitting it

77:01 40 10 and this one down here hitting it. Let's go all the

77:17 down to here. 41 50. . So if you were, if

77:35 were to look down on the you know, this is a

77:40 a straight line, this could be straight line, this part of it

77:45 hitting here. This part is sitting here. So the P has to

77:54 around to reach that point. In words, sure, if these structures

78:04 lined up like this, then it be flat. But because this is

78:09 and it's going down, the structure you see here is uh you're going

78:14 the fault plane, you're not hitting fault plane at the same point.

78:18 words, this, this part of circle down here, it's not hitting

78:23 here, it's way out of So makes the, you're on a

78:30 surface and you're, and you're becoming like this one going down and

78:37 So the curve, the is a curve one minute. So you have

78:41 curved surface and this is a curved , curved surface hitting a flat plane

78:47 gonna make, it's gonna make that look curved. And uh when we

78:52 mapping, you'll, you'll see a bit better when you have some more

78:56 to show you. Uh And what means. Uh Here's something that the

79:01 that wrote the book and she uh with him on uh uh some surface

79:09 . Uh uh They have this they call a screwball where people start

79:17 on their contour lines with the data they have on one side and the

79:21 lines with the data they have on side and they end up thinking they

79:26 have some kind of closure in And uh uh this is, this

79:33 a normal fault, it's down thrown here. Uh Here's 59 50.

79:44 And uh here's, you know, 5900, 59 50 here. And

79:49 is, this is actually uh gotta higher than it's supposed to be.

79:58 so you can't get disclosure across here uh this is actually uplifted on uh

80:05 that side of the block. And let's see, actually looks normal to

80:26 . Can you see, can you the problem with this or not?

80:36 it's so it looks ok here, what's happening right here, this

80:50 uh, this looks normal and you focus on this part and that's part

80:54 the problem. And then, then look at here, this is

80:58 Now, what's that? In other , the, the direction of the

81:06 changed. And that's, and that's , uh what he means by a

81:10 ball. In other words, it , it looks like it's OK when

81:13 draw it like this. But um uh but it's, it's not,

81:20 has been drawn the proper way and , somebody's been, you know,

81:24 their concours this way and coming up way, drawing their concours and coming

81:28 with this and there's a reversal of contour lines across here. And

81:33 they forced the, uh they forced closure there so that they could have

81:37 reservoir, but it, it can't be that way. So there's a

81:40 mistake in how it was mapped Mhm Well, this side is higher

81:53 then this side uh over here is . So you, you've actually,

81:57 works through, it's, it's um know, he's got one well there

82:02 he's, he's drawn a map away this uh and then it starts to

82:07 back up on this side. But , uh you can see here,

82:11 is, this is much shallower than there. This is even shallower.

82:16 the contours that have come off of are making them look really strange.

82:21 right here it looks like you um, this looks like it's on

82:26 high side, like it's supposed to on a normal fault. But when

82:30 get over here it's kind of twisted . It's, uh, it's what

82:34 calls it screwed fault because it looks . But it's just, uh,

82:41 , misinterpreted. Ok. So, , if you, uh, another

82:50 about us in structural geology and especially frontier scale, you know, we

82:55 at these basins because they help us um the different types of trap styles

83:00 we're gonna find in the, in basin to uh for uh prospect.

83:07 uh we start looking at the major faults and blocks and uh and we

83:12 start getting at the scale of what would call a fairway, which we

83:16 talked about. And uh what and have uh so, and here we

83:38 , um, you know, uh becomes important to look at different faults

83:42 folds. And uh there's also uh geometries that happen around faults. It

83:48 that we were trying to talk about uh and I was trying to point

83:51 about the curvature of faults over there uh and how it's different when you're

83:57 a surface and not, not a of plane surface, a surface that's

84:02 that has not been eroded versus one has, and so it gets a

84:06 bit complicated. And then of there's uh uh fractures can be a

84:12 of uh of the structure in a because we're gonna have these stress fields

84:18 uh can enhance uh fracturing in different directions relative to sigma 12 and

84:29 OK. So, um in I'm gonna probably show you mostly tension

84:33 things because that's what I've mostly worked . But I, I wanna,

84:38 know, just go over it really um in the divergent settings or extensional

84:46 , we're gonna see a certain set things that we're used to seeing in

84:50 of the vault arrangement and the formation reservoirs and traps and uh conversion

84:57 uh compression and extensional things are gonna a little bit different than, of

85:01 , transform settings are, are the ones where we can have um uh

85:08 where the bottoms just uh seem to out of them. So, uh

85:12 we'll take a look at a few these uh divergent settings and um uh

85:18 , of course, um uh shows kind of the, the uh configuration

85:24 what you might see in a very uh rift valley or groin like

85:29 And of course, again, these tend to uh rotate out and you

85:35 a high end over here and a end over there. And uh in

85:39 rift valleys, they actually have mountains them and the uh the riff valleys

85:45 uh become air tunnels and you can really high, uh, wind speeds

85:50 through there too. And here is one that's a little bit different.

85:55 , this is from the basin and and, um, you can see

85:59 this is, uh, this isn't rift but it's, uh there's

86:04 uplift going on and it's, it's causing that whole area to be

86:10 uplifted and, uh, and it's of stretching uh the crust and you're

86:15 Robins with horse. So you have and valleys uh forming in, in

86:22 in this particular part of the, the US and other places that are

86:26 that. And uh here is uh at uh a few important rip

86:35 Um The North Sea is a fail . Uh Sometimes these things are called

86:41 lack the GS, but sometimes the the GS are very specific to shorter

86:46 groups. And here is uh West West Africa. The Pres salt in

86:52 Africa was part of that. And the East uh Brazilian stuff that we

86:58 was part of basin when the most countries separated Africa, South America.

87:04 of course, there's some other basins are uh sort of like sags that

87:09 uh failed drifts on the margins of . And uh and uh in the

87:15 Basin and places around that. And is just uh showing you a triple

87:23 with the Red Sea is, is , is a spreading, has a

87:28 rip, but it's uh they both a and we both as a kind

87:33 uh slowed down quite a bit. you can see that the elements of

87:37 triple junction extend all the way up the north here. And uh and

87:44 it's kind of a, a triple is kind of a uh standard pattern

87:47 we see. But uh at the time, we have uh this uh

87:54 rifting going on here where you can the high spots. And uh if

87:59 above uh wave base, you're, gonna be having erosion go on and

88:04 high spots filling in accommodations down If sea levels a little bit

88:09 it would be all the way down , say to there. So

88:12 you're setting up a system for the and delivery of sediments and a place

88:19 uh where we have accommodation space depending where sea level is at any point

88:24 time relative to those blocks. And is uh what the basin a range

88:31 I was trying to show you, an extension there and you can see

88:34 you're getting horse and um first blocks , and uplifts and uh and here

88:45 of it actually works like this and actually shows what I was trying to

88:48 out. But sometimes these blocks rotate when they're extending and you get mountain

88:54 on top of them from a you know, I think much of

88:58 . But these are, this is how mo similar amounts are formed.

89:05 again, you're creating um on the end, you're creating these uh sorts

89:12 sediment, you can run off this or that way into these um these

89:17 . Now, this is well above level. But uh you can imagine

89:20 similar feature for the uh for the valleys which are a little bit different

89:25 this. Uh It, those it's a different type of extension.

89:30 the rift valleys, uh they have , the fault blocks will rotate like

89:34 where you have the high ends that in the mountains and then the low

89:39 here. And because it's a uh you typically either have uh in

89:45 early stages, you have lakes in later stages, you start to have

89:49 sediments in there and you can go uh a mountain cliff to a uh

89:55 a um a basin full of accommodation down, dip in and into the

90:00 itself. And uh here's uh showing again, uh what happens with uh

90:08 compartments. And uh again, uh o oftentimes I'll rotate like this.

90:16 uh in uh when you get off passive margins, it kind of shifts

90:23 a little bit differently like in the of Mexico. But here you can

90:28 the football block is gonna be the . Here's the football block over

90:33 the draft and here's the football block here, this trap on these normal

90:38 . A lot of times I see just a completely opposite when, when

90:42 not necessarily at something, um, , that has rotated fall blocks like

90:48 extensional basin or a, a rift . There's a different attitude of,

90:59 , the dip of the beds and , uh, and the vault

91:05 Ok. And, um, sometimes get these sorts of things,

91:10 with complex ramps and that sort of . And, uh and then the

91:17 the rift valleys, when they're first out, they have a lot of

91:21 ramps on either side. They're kind like in echelon, they go back

91:24 forth from one side to the next the rift and eventually they start uh

91:29 and they lose the uh the relay . There was a, a huge

91:37 in the Jurassic sands in the North . Uh that was on one of

91:41 ramps and, um, and it up. Uh I don't know if

91:46 remember the um slide that I showed with the Jurassic sequence photography. Uh

91:53 were having a hard time uh correlate from a Jurassic sandstone here and one

91:59 was here and one that was up here, uh because uh b the

92:08 uh was a little bit different as might imagine. You know, this

92:12 uh probably catching more sediment. This would be catching less sediment and this

92:17 be catching sediment somewhere in between, terms of time. And,

92:27 here's, uh, sort of the of thing that, uh, that

92:35 , uh, see a lot. , um, and again, it

92:42 on the, um, where you're . But, uh, I think

92:48 is, uh, probably West Africa , um, what you're seeing here

92:52 a special kind of fault and, , it's called a growth fault

92:59 uh, just take a look at , what you can see here and

93:09 look on this and this is really of an important thing. Uh Here

93:13 have a relatively thin section and this include the sediments from the same amount

93:21 time is all of this one. may be uh some condensation or

93:28 but you can see here that this section expands to be this big.

93:37 uh and that's called uh a it's a special type of quality.

93:41 has a shape or spoon shape. it's sometimes called a list fault.

93:47 Sometimes there is there is salt for to slide on at the bottom.

93:53 a key component of this is it's a growth fault because uh while

93:58 fault is moving, it's creating more space here, it is here because

94:06 creating more combination space. The uh column is growing, essentially growing

94:12 So where's the depa center on It's gonna be right over here.

94:17 , the Gulf of Mexico uh they again, the rotation of these things

94:23 a complicated uh thing to calculate, they can rotate a lot differently in

94:28 places. And uh uh you have funny brand like teacher here that kind

94:36 holds things up uh over on that of it. And, and this

94:40 uh I think the continent of Africa over here. So uh here

94:45 you're seeing um some of these sediments going down like this and there's gonna

94:52 terminations up here and pinch out. could be reservoirs but probably not a

94:57 good reservoir because it actually could come the way out here until it gets

95:01 something like this and it catches Um There's uh a bunch of these

95:07 bolts uh that have a slightly different than this. And you see trapping

95:12 this trapping in the trap is actually the um uh the hanging wall

95:23 excuse me, the football block and the uh hanging wall block. But

95:26 we have to like you might have traps over here. It's really hard

95:30 see it. But here uh uh in, in the uh the hanging

95:36 block here is moving down like So if you're gonna get a

95:41 it has to be OK. Here's one similar to that uh drawn in

95:56 different direction. And uh and you can see uh that this is

96:03 growth fault and here, the way rotating, you can see that you

96:07 have some traps up on this end not on that end. And,

96:14 , but, uh, the rollover be different in with different rotational

96:19 And, uh, you can get that, uh, that a trap

96:23 this where you'll have traps up in . And, um, and that

96:28 of thing. And here, here's of the plane, the growth plane

96:31 here and you're getting this rollover, is convex rollover. And here,

96:37 , this is what I, I'm to seeing more frequently than not is

96:41 concave rollover. And you can see on the hanging wall block,

96:49 that's where you're gonna get the, traps and, uh, it's gonna

96:53 hitting up against that fault here. so, uh, this happens a

96:58 . Uh, if you have, example, a salt dump coming up

97:02 here and you have things, uh sliding down in this direction,

97:07 often get this sort of a, drag like, uh, get a

97:13 over in this concave rollover where there's drag on the. And,

97:18 and so you get the traps up and, uh, that's, that's

97:24 uh configuration I'm used to seeing more than not in, uh, and

97:30 these parts and there's, uh, another example of that. But another

97:38 that's uh interesting about them is that also get, uh, you get

97:43 faults uh forming two. And so have faults over here, uh,

97:49 come across like this. Uh, you can get traps up along where

97:54 anesthetic faults are occurring. And here , um, uh, the down

98:05 expansion of the Clayburn units. uh, this is a really good

98:10 from, uh Hackley and Ewing. , Tom Ewing is, um,

98:18 really good, uh coastal plain geologist , um, can see here

98:24 uh, we haven't talked about plays play fairways, but there's a lot

98:29 uh you have a series of these growth vaults bounding with growth vaults.

98:35 You have a lot of places where can have different configurations and anesthetic faults

98:40 get traps along here and even up way. But through this whole

98:46 what you're seeing is that while you're creating this regime that's full of

98:51 these are the major bounding ones, there are gonna be other faults uh

98:55 across like this that are anesthetic to fault. And you'll have a lot

98:59 traps developed and you'll also have a of um sediments pouring into this

99:07 So you're so you're getting all these centers. So you get a series

99:11 depot centers like from here to here here. Uh You get basin for

99:16 in different places and uh and uh slope slope to basin uh fans.

99:23 in some cases, they're not as as some of the ones that we

99:26 further offshore. And uh and um point I'm trying to make is when

99:32 you have a, you have very sequences of sadness and we have lots

99:38 ways to get the fall trash developed through through um uh roll over up

99:45 this thing, roll over, roll here. That might be um you

99:49 , just no rollover at all. that end, we can get anesthetic

99:53 in here. Uh Make a long short. Uh These types of growth

100:00 create accommodation, space and sediments. create fault fault, accessory faults,

100:08 traps and uh it's just a, just a gold mine of places to

100:12 for oil and gas. And um always have a test question on um

100:20 growth faults uh about, you why is it such a, a

100:28 habitat for uh for finding hydrocarbons and vaults are really a good habitat because

100:35 all those things because of the development a lot of structures, which is

100:40 we're talking about here. But at same time, uh that growth is

100:44 a nice thick wedge of sediments. a depot center, you're gonna

100:49 you're gonna have higher net to gross uh coming across this fall. So

100:55 gonna be a lot of sandstones in . And uh and because it's because

101:02 a relatively rapidly developing basin, uh gonna be pushing the potential source rocks

101:08 and deeper and quicker and quicker. there's obviously gonna be some sort of

101:13 rock. It turns out in the of Mexico way before all of this

101:18 , we had the Jurassic source box uh but through the process of

101:24 well, we got some midway uh rocks developing uh because of, of

101:28 subsidence of all these units going down getting deeper and into uh the oil

101:37 . And so I get really excited um you can't tell. OK.

101:51 And then of course, uh we more complicated things from convergence settings and

101:58 and like I say, I I've very rarely worked on uh on

102:04 things. Uh but you know, need, you need compression. And

102:08 , and I think one of the that I appreciate the most about it

102:13 understand what's going on in the for , in terms of compression. But

102:18 the back arc as the way it um um the uh underlying parts of

102:27 mantle and the lithosphere, uh you up getting crystal uh crystal stretching in

102:33 back arc. So this again is , is a realm that has um

102:39 and extensional features too. So it's uh mostly compression up here and

102:45 extensional back here. Um The uh I worked at Amico and Mobile,

102:52 both had um uh big holdings in types of areas. But uh uh

102:59 were very special places where uh we able to get um something that would

103:04 into a petroleum system. Uh just of, uh the way some of

103:09 things work. But at the same when they found them, they were

103:11 big. One of the uh biggest fields that mobile produced from was

103:16 uh, was a compression system uh Indonesia. And uh a lot of

103:23 they are associated with uh limestone reservoirs well. And uh, but uh

103:30 that I would work on would be here in this uh back art uh

103:34 it's a little bit different. One um that's uh I think important is

103:47 when you're in these kind of systems , that are essential because the press

103:53 is stretching by this kind of falling into the Gulf of Mexico in a

103:58 . Uh You're, you're creating a volumes in terms of area and uh

104:06 number of opportunities on the, the coast because of the, the large

104:13 sediment, uh basal sag that's going underneath us. Um The um the

104:22 of sediments and oil that can be produced out of this tends to be

104:26 pretty significant on a, on a scale because it's, it's uh as

104:32 know, the coastline of Texas is , very, very broad and uh

104:36 not just isolated uh features that we in, in a few places that

104:40 oil and gas. It's, it's most of the coastal border. And

104:54 again, you know, this is hanging wall football thing. And you

104:58 see here the hanging wall goes up , uh, and, uh,

105:04 here, uh, here's another close thing of, of a uh reverse

105:10 . Uh, but the, the crucial thing here are the thrust

105:15 and, uh, sometimes these can associated with, um, a lot

105:20 the thrust can be associated with, oil and gas that might be on

105:26 of the, um thrust sheets. one of the things that it does

105:30 uh from a different uh type of . But uh here we get these

105:34 land basins. And um the key on the four land basins is that

105:41 oh obviously, you can get some crustal sagging due to this loading

105:47 And of course, these thresh sheets massive amounts of acreage being thrust on

105:52 of each other. And um like said, sometimes the thrus sheet,

105:57 bi were, were very deep enough they might have gas research and stuff

106:01 that. But a lot of times looking for uh these, the four

106:06 of these things uh that create these very long uh basins. And um

106:14 the uh the four La Masons tend be narrow in one dimension, but

106:19 extensive in another dimension. So you have these really long things that

106:24 that are close together and uh also a lot of the features in

106:30 Uh in terms of traps and uh accumulation and reservoir rocks, you

106:38 seals and, uh and often uh very deep enough that could be a

106:44 rock. And, uh again, , I don't work in, I

106:47 worked in them a lot. Um know uh a lot of current uh

106:54 is being done also outside of these , but there are certain areas where

107:00 they're extremely productive. And, and, uh, and, and

107:09 again, I think, you if you think of the scale of

107:12 of these, of course, the , the front uh basins of uh

107:16 of the ba the ranges that we in, in North America create some

107:21 uh large areas uh that make these Orlean basins. But again, relative

107:27 say, the whole coastal plain of of uh of Texas, you

107:30 it's a really small uh area in comparison. So I think,

107:38 know, and if you look at the um the, the rift basins

107:42 the um and they um extensional margins , of like the Atlantic Ocean,

107:50 extensional margin of the Gulf of uh you're, you're looking at tremendously

107:55 areas. Uh And of course, there are some complex basin and structures

108:02 in Guyana and uh and Serena where also finding some uh pretty enormous

108:09 Uh But again, I, I work in that area but uh and

108:14 uh there's another place uh that we for, uh, right these things

108:22 it's, it's along these rift basins of course, um, uh,

108:27 already looked kind of at, at northeast samples quite a bit, I

108:31 , um, kind of get the from that. Uh, but,

108:36 , this, uh, trans rotational are full of parts are pretty interesting

108:42 , uh, I did, did on one, uh, that was

108:48 to the LA basin project and, , that was the Riff Basin

108:54 And uh the thing is uh a way to settlements. And uh and

109:06 it's uh it's basically uh nine kilometers and uh sediments are just dumping into

109:12 thing. And here you can see the custard shales, you can see

109:18 sandstones uh that pour into it. And you, and you can think

109:24 , you know, uh nothing gets into a wedge like this without having

109:29 accessory vaults somewhere in here to help develop traps. Maybe there could be

109:34 uh other types of traps and this uh was very, it's really large

109:41 system. And from a, a oil company perspective, it would have

109:48 uh a very prospective area uh to for hydrocarbons. It's, it's uh

109:56 some extent, you know, it's fairly young, you can see

110:01 the way down here in biasing. , um it's uh it's not,

110:09 not, you know, the scene an awful long gap in time.

110:15 uh but uh it's not gonna be than 25 million years or so

110:21 Uh, for those sentiments. So is, there would be one concern

110:25 things being buried deep enough. long enough. Uh, not,

110:29 , they're plenty deep, but how have they been buried if you had

110:35 rocks? Um, but it's it was a very large base and

110:41 very large lake. And do you know why it wasn't uh wasn't prospective

110:46 the end when you wanna wanna But there were a lot of

111:01 a lot of uh potential reservoirs. Good chance, you know, you're

111:05 seeing major faults on here. There , there definitely would have been some

111:09 box in, in this. Uh we got to uh looking at it

111:14 but um see all the sand short of time, 9000 9 9000 m

111:25 nine kilometers of sediment too fast. , the speed has something to do

111:31 it. But yeah, but, , if you have a lot of

111:35 in a short amount of time, do you call that? A

111:39 what lots of sediment, short amount time, high depositional sedimentation rate,

111:47 or the other? Ok. If have a high sedimentation rate and you're

111:51 it into a water mass that has , what do you think is gonna

111:55 to the concentration of the organic matter gonna go down? So there's

112:06 I I think I mentioned it, might not have been paying attention.

112:10 , but the San Jorge Basin has right hydro chemistry for high organic product

112:16 . But normally it didn't get much eight or 9% which is a great

112:20 toc. But the San Jose Basin a sodium bicarbonate basin. So it

112:26 you wonder why is the toc so ? And it's because of San Jo

112:30 is in some ways like this it had a really high rock accumulation

112:35 and it diluted the organic material, even diluted because it was a latrin

112:41 that was sodium by carbonate enriched. still had eight and 9% which is

112:45 the best marine, the best marine sort of rock you could ever find

112:51 . Two things were against us. was that high sedimentation, it was

112:55 out. The other one was the that um the uh the chemical,

113:03 height, the uh um the paleo geochemistry was such that it was enriched

113:11 calcium and sodium and chlorine. So more like a, a more a

113:15 type uh uh hydro chemistry. So would be lots of appetite in

113:22 And uh and you would, in , there is, and you would

113:26 a lot of the phosphorus that could helped the productivity was, was absorbed

113:31 the in the uh sediments or deposited sentiments it was sequestered. OK.

113:41 uh and then to go further on we are looking at, uh,

113:46 are considering unconventional, these little things fractures are really important. Right.

113:53 so, um, what's the difference a fracture and a fall?

114:05 Excuse me? Well, that's small . So they could be small

114:12 But, but what do you see these fractures hanging wall block or a

114:21 block? There's no offset. You , it's just, it's just

114:27 it's like a tear. Uh It's , it's not like this or like

114:31 . It's just a and, and a lot of times that

114:37 uh when, when the surface is and uh it can also happen when

114:42 things contract when they have thermal you can get fractures like, uh

114:48 those neat, uh the devil's mountain whatever it is where you have

114:52 the basalt columns, there's fractures in them, they're not moving up or

114:58 . But, uh, it's shrinkage , uh, and so you get

115:02 fractures in between it, then they're dis and Hexagons too. Ok.

115:11 another thing to think about with, any kind of uh faults and

115:16 um You have to worry about whether have uh communication across and uh by

115:28 large, a lot of uh faulting occurs and we'll talk about this more

115:33 the future. But uh has to with, you know, you can

115:37 , um, here you have cataclysm uh in here and uh that could

115:44 this thing even though there isn't a shale smear or anything like that

115:48 it. And um, and uh , and other things of that

115:54 uh but this, this fault can sealing the thing about uh faults though

116:01 especially a growth fault is gonna keep . And when that fault starts to

116:05 , it dilates a little bit so can have uh ceiling faults that actually

116:10 open channels. And uh there was , a huge growth fault in front

116:16 a shale ridge on South Marsh Island 28. And that huge fault uh

116:23 an event where it opened up pretty in the oil column. The hydrocarbon

116:30 from the very bottom to the very uh is really it, it's,

116:36 a huge uh hydrocarbon column. It of equilibrated such that the sands that

116:42 once it's sealed, the sands at top were full of gass. Uh

116:48 sands in the middle had gas and and the sands below that had just

116:53 . So it was almost like a a single column of oil uh across

116:59 fall will build up these sands on other side of it. Uh with

117:05 , gas, gas, gas, gas, and oil, gas and

117:07 , gas and oil and oil, , oil. You know, it

117:10 , it was densely segregated almost from to bottom. And um it was

117:15 good fault to, to ask people the fault ceiling or the faults um

117:22 . And of course, when, that uh hydrocarbon column was created,

117:27 had to be dilated and it was moving a lot and it moved to

117:32 certain position and stopped, frozen, in and it, and it saved

117:37 reservoir from leaking out to the And um there might have been more

117:42 at the top of it to keep from leaking out at the top.

117:45 But some of the things that were might have gotten a little bit and

117:49 up and, and uh when it , uh you have a lot of

117:54 in the, in the fault uh you end up with more shale

118:00 and you know, the end of course, we'll, we'll look at

118:03 of the algorithms that they use to the uh an estimation of, of

118:11 uh seal across a ball based on like uh the amount of shale that

118:17 be uh smeared into it based on the net to gross. And then

118:22 this case, you're looking at a net in the shale to uh to

118:26 that seal. And uh here's one one uh where uh you can see

118:41 gouge going on down here and there's gouge here. Uh This one with

118:45 , this might be sealing it. uh this is a small scale

118:49 But if it was on a large , uh maybe hydrocarbons could be trapped

118:53 below here. But if they were here, they might slide up this

118:57 that doesn't have anything sealing it in , in the gap. I thought

119:01 was an interesting picture just to show on a small scale what how some

119:06 these things could be worth. So this is uh this is a story

119:17 a simple little diagram. Um It of assumes an awful lot. But

119:23 if you have, you have rocks are under a certain stress field that

119:28 change through time. And so you have multiple series of fractures. But

119:33 they did these uh block models uh to try to get an idea.

119:41 um and so I have these three models then I, I think this

119:50 uh something interesting and, and uh shows uh uh joints, uh faults

120:00 ST lights uh that could, could barriers. Uh And um and it

120:07 the um the stress regime, excuse , the stress regime uh uh

120:16 with stress versus strain going on you can see uh the vertical,

120:19 this case is one s one here vertical S two is gonna be in

120:25 direction S3 is gonna be in that . And um uh what kind of

120:34 do you see here? And it you, it says normal faulting.

120:44 trying to get you guys in, to, to engage here. But

120:49 but you can see here, you tell here, but you can see

120:52 . It's, you know, you've this normal quote. So there's gotta

120:55 some tension here. So this direction is the Sigma three is gonna be

121:00 lowest stress can, can you have uh the vertical, what is the

121:09 ? That's the one who's causing What's the, what's the other name

121:21 ? Um art? Um But even basic than that, um what's another

121:27 for a normal fault? Did? . So, but it's not the

121:35 of the gravity. I hope you , you said I get that in

121:49 more general. Why is it There's a profound part of the universe

122:05 means a lot. So these are gravity faults because that's, that's what's

122:13 making them happen is, is that push. So o overburden would be

122:17 to it. But uh but uh basically slipping due to gravity and uh

122:25 not because of compression, it's because gravity. And uh and that gravity

122:30 , is allowing you to extend and course, if you work something up

122:34 this, um it's gonna split and gonna have normal faults, even if

122:40 compression and you have the SAN, gonna have the normal fault because it's

122:44 it. If it stretches of the have to fall into the space,

122:48 have to stretch it. So it's gravity fault. So, um does

122:54 here work on horizontal wells in the fracture. Yeah. Ok.

123:01 you can imagine these stress fields sometimes really important to figure out.

123:08 um, and the reason being is if you, if you have a

123:18 field like this, right, you're get, get these faults happening,

123:25 that are going like this and gravity usually bounce off, you know,

123:29 an end, you know, you're gonna bother. And uh so you

123:33 these, these things splitting like OK. Uh And when um but

123:43 you start getting joints and fractures and joint, these fractures are gonna be

123:50 a plane like this. OK? that's, that's, in other

123:56 that's the lowest, it's tension. it's just breaking open like this.

124:01 if I was drilling, if I drilling a uh horizontal well and I

124:06 to working, I wanted my hydro in concert with the natural practice.

124:13 way would I want to do Get that? Yeah. Oh I'm

124:29 . OK. You were, you uh I, I was hoping you

124:32 interested in what I was sent. OK. So, so you,

124:38 gonna, you're gonna drill a horizontal and uh if you're gonna do this

124:44 tracking and it's, it's gonna be way or this way, it's gonna

124:48 on a plane like this. So oftentimes we like to think the reason

124:56 this doesn't and sometimes we like to that if you are across that

125:05 then we're gonna enhance the natural fractures the fractures. We're trying to

125:10 we have less stress on them. this, this is your sigma three

125:16 . And so it's creating gaps on a plane like this. So

125:21 direction would I want to drill? to, to take advantage of

125:27 what direction would I want to drill this blog? So where you can

125:34 one of the acids, which acids you're gonna on to do the,

125:39 enhance the hydro relative to the stress that's creating natural fractures on this

125:49 See it's on, it's on that popping up here popping up there.

126:00 words, which one, which one the uh which one of the Sigmas

126:04 gonna line up your, that's what would do. Great. OK?

126:18 know, if you go this you know, you might miss the

126:22 , but if you go this you're cutting into all the fractures.

126:27 ? Now, there may be a why you wouldn't want to do

126:29 What would that? You have a of natural fractures? And one of

126:36 happens to go into an a or and you wanna look inside.

126:49 they can. But we're not, not looking for the fault services.

126:52 not, we're not looking to line with, with these surfaces. We're

126:57 to line up with the natural And if we're gonna line up with

127:01 natural fractures we would go in the . In reality, here's what happens

127:05 people started doing that. But if have a stress regime, people started

127:12 with these blocks when you started looking anything. But uh say this is

127:21 just to make sure it's clear. So say that our S3 is uh

127:27 more so ok. Um Like a of it. But anyway, um

127:56 have uh acres. It looks like . I could, I could,

128:03 could happens often people really get these , these long acreages like this that

128:13 narrow and sometimes it might be situated this and, and when that

128:23 it doesn't matter where the Sigma Sigma three is you, you just

128:28 to go with, with the and might have gone, you know,

128:34 does a big stress study and figures what might be the most advantageous,

128:40 those things, at least you would to do it in this case if

128:45 so well before we go like this that plane, natural fracturing is like

128:56 and you'd be shooting into of those fractures and spreading them part. So

129:02 would be, you know, with , health, the only time you

129:06 don't want to do it is one these natural factions. You really think

129:11 might go into an, you don't , don't wanna connect your uh resource

129:15 places within their app. One, other words, you want, you

129:21 your resource play, you want it be the source, you want it

129:26 be the reservoir and you also want be, uh, there's a sandstone

129:35 it or below it, uh below or above it. If you're gonna

129:39 an issue and you, uh, , and just to, uh to

129:47 problem or, uh but the, practical issue that, that most uh

129:53 themselves in is that company has done , another company does this and another

130:07 will do this and once somebody starts their lads, they give them direction

130:13 much stuck on. But I don't if it's always that way, but

130:16 know we had a city, which was a pretty good company of

130:21 the money but, uh, spent of his time, uh, working

130:25 how to arrange these things and, uh, 95% of the time,

130:29 direction we had to drill in. is always, uh, pretty,

130:34 determined by the acres that it's You know, you had a bunch

130:39 stuff like this at one spot, bunch of, you know, the

130:42 that might be available is something part this. And, um, and

130:48 what you have to do. So have to, you know, just

130:51 do a lot of life. Cause everybody else to do.

130:58 you could do it. But they, they'd find out.

131:06 So, um, this was normal . These are the stress fields,

131:12 , that you'd see with a reverse . And here, of course,

131:18 signal one is gonna be that thrust and, uh, almost the

131:26 And, uh, in fact, axis is different. And then here

131:31 the, um, wrench faulting. . And, uh, this,

131:39 shows you, you know, you've things going like this. It's a

131:43 bit like the, uh, uh, what do you call

131:48 The, um, the reverse the fields are almost the same.

131:54 can see here uh the, the Sigma two and Sigma three switch around

131:59 you can see here that and, that's to allow for uh the expansion

132:05 gonna be required uh when you shift this way on a block and you

132:09 that offset. Uh So, uh I like to ask a test question

132:17 uh let's say, you know, gonna build a horizon about clarify

132:22 I would say something like, oh you're trying to, that, this

132:28 one. They not want that. yeah, so when I write a

132:40 I like this. Um don't never nuts. Don't ever, don't ever

132:47 in your head. Yeah, that's true. But yeah,

132:50 don't add it here. OK? sure you don't add words to,

133:06 . OK? And so, uh wasn't a whole lot of uh of

133:12 , but I do want to show this one here's a, this is

133:20 reverse fault and just in case you think they can create mountains. There's

133:26 Grand Tetons and uh I wish, wish I had some pictures from uh

133:41 funded when I worked at Amico. I funded a bunch of people at

133:46 uh and uh and also um Duke to go over and um do some

133:55 in uh in some of these things , and they had great pictures

133:59 of the ranges weren't this big, they had, uh, mountain ranges

134:03 either side of the rift basins, , like Lake Turkana. And,

134:11 , they had a picture of, , um, a water spout off

134:19 the bow of their vessel. there were four water spouts and,

134:25 , did, you know, water are dangerous if you're in the water

134:28 them, they're really dangerous. uh, I thought, you

134:33 as I was growing up, you , we'd see water spouts in the

134:36 Bay. We go, yeah, it gets on shore, it's just

134:40 go away. Don't worry about So I was out on a guided

134:43 destroyer one time. I don't know I got in the Navy. Somehow

134:45 got in the Navy and I was on a guided missile destroyer in the

134:51 and a water spout pops up. , uh, this is one of

134:56 first cruises I was on and, , and to a person, everybody

135:02 running for their life jacket and we on a, a 300 ft plus

135:08 . And, uh, so water are not insignificant things if you're out

135:12 the water. So they had this , these four water spouts on their

135:17 . And, uh, but, , there's, there's a shot was

135:21 at the bow. So you could the water spouts, but just in

135:24 of the, uh, the you know, moving towards the water

135:29 when the picture was taken and you see just off to the starboard

135:34 there's a 14 ft crocodile swimming with waiting for them to fall in the

135:44 and uh talk about a safety And uh when our safety guys

135:50 were watching this uh presentation from uh , the research, they're a little

135:54 worried about them being out there in boat with water spouts and alligators.

135:58 then one of the professors used to an underwater demolition team guy. And

136:05 he uh I don't know, I think I need raw fish, but

136:10 draw picture. So here's Lake Chicago bigger than this. And um so

136:30 they have this, uh they call the, yeah, the, the

136:35 flowers. Um But uh it was so get over the sea.

136:48 and they were backing it into the and um you know, the bounds

136:54 here, the bound is very They couldn't quite get it. So

137:00 guy had, they had dynamite charges being the and um So he just

137:09 just put some charges like this. Can trace around it so that you

137:17 kind of kind of just drop the into the, into the water.

137:21 was uh OK. That sounds a thing, right? We actually had

137:26 picture taking a picture of the the going on there. A student standing

137:33 where you are and there was big her out of all of them.

137:39 . Got it. And then it worse down in Burundi in the town

137:46 Jin Borough, which is the He stored all of his dynamite in

137:52 warehouse in the middle of downtown. uh we had to get rid of

137:59 and that was a pretty, pretty wild rid anyway, I'll stop

138:06 . You guys wanna take a little of a break and then, then

138:10 can finish up in an

-
+