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00:06 Okay. We're talking about false segments how we link up and really ramps

00:10 false segmentation and and how it spoke vertical and lateral. And what we're

00:17 look at now are some sandbox experiments how these things link up. So

00:27 stage one and stage to represent three stages in the sandbox experiment, we're

00:35 so that the north and into the 57 m It's a plane strain north

00:43 extension. So no change in in in the in the Y direction

00:49 just in the X direction. And we see here are different fault

00:57 basically progressing with the amount of So here the extension is really

01:05 Here, it's intermediate, and you see how each one of these guys

01:09 started to grow in length there from to this From this to this,

01:18 this to this. Get the Sorry, Professor. I cannot see

01:25 , uh we consider representatives here. , hold on. Thank you.

01:39 . Are you seeing just the one now? Okay, let me get

01:50 . And I have had the laser on. Are you saying that

01:54 Yeah, Yeah. Okay, Thank you. So, uh,

02:00 this extent about this experiment, you see how these false start to

02:06 They grow laterally, and eventually they up to become one through going

02:13 That kind of thing that we talked in our problem on some of the

02:17 plots. Here's another. Here's another of a different sandbox experiment. 10

02:28 here, North South extension. It's and a half percent straining here.

02:33 pretty small amount of extension between North South Theater and 3% strain here.

02:39 pretty increase from this stage to this . And you see the false starts

02:46 nuclear here fought one football too, felt three full, additional 5% strain

02:55 false of form four and five. guys have coalesced into one through going

03:02 when we started with three. they're just a little bit more

03:06 We've got one long through going So this is what the throw profile

03:18 look like on those fall Since the 3% strange. I have low displacement

03:26 . A minimum almost zero here. minimum here, here and here again

03:32 the zero here with maximum throw here, here and here. And

03:38 , as these it is these false , the strain increases comes. We

03:45 a through going fall in the location the maximum changes, the minimum kind

03:52 stay in the same place. But master changed significantly from this point to

04:00 point then with increasing straining that maximum about the same point and the minimum

04:09 about the same price. So uh, the original fault segments the

04:16 is a lot of those really inherited the displacement profile, as it's a

04:22 false evolved in Kabul s and way that in three D in thrust

04:38 So here on the right, I've a perspective. You of Roy.

04:42 horizon in deep water Press belt college death threat is fine. Lewis

04:51 The sense of displacement divergence is towards north in this figure, in each

04:58 these lows between the different structures, see the finished with related rant from

05:07 relate relaying the displacement between these two . Another really ramp here relaying that

05:15 segments. Um, and then here didn't laying the displaced in between these

05:21 segments. So our displacement uh relays occurring in both the strike direction and

05:31 the dip direction. And we'll get different minor structures in between these

05:40 depending on how these guys go So here we're gonna have a contraction

05:47 . I'll step over. We'll have folding environment thrust, Faulty interior.

05:53 we have an extension of segment where felt Blanc is actually moving away from

05:59 fall clock here. So even though overall thrust setting, we'll actually have

06:05 extension of structures in in this So the segmentation is three G and

06:12 on how the faults overlap, you different structures in between the different fault

06:21 . Yes, right. So the couple slides are talk about different definitions

06:31 trapped closure elements. So here we're at a a structured contour map of

06:36 trap. It's just schematic fault up there inside on the left hand

06:43 , on the right, pressed here the middle, each one of these

06:49 lines representing a coming through 100 100 . At this point, it could

06:55 either time or depth, and you the dip closure is defined as this

07:02 that is just dependent on. So from, uh, I'm just

07:10 on the depending on the trap talking 300 on down, I start to

07:14 dependent on this false your capacity, deeper element of the trap and

07:25 So at the tip dependent closures off from the press to the lowest

07:33 that kids is the following. And below that I have talked dependent closure

07:39 the scrapping ability to retention abilities dependent false feel. And in this

07:45 the fault dependent closure goes from about down to down to about 5.

07:53 . Constrained by my spill point Over . See, now I'm going

07:58 down, down, down through a And then I started climb up

08:01 So this style is my spill point the constant elevation here is about 5

08:07 . So this this defines my spill for the trap And the difference between

08:13 first count through that kisses the And this spill point defines my fault

08:19 enclosure magnitude The dip closure goes from 100 to about 300. About 200

08:29 of disclosure here. The false planet goes from 305 fifties. So I've

08:35 about 150 units meters, two way time. Whatever. And enclosure

08:43 Still on. All this is constraining . This saddle over here in 5

08:48 m, or, uh, or a travel ban. Right. So

08:56 is a cross section through that showing what these elements look like.

09:00 in cross section, there's not There is the top of my

09:07 It represents just the disclosure. So is the let's least risky closure.

09:13 is just dependent on good diplo, tops your capacity of whatever topsy on

09:20 is and then below that from where contour, it's the fault. I

09:27 a fault dependent closure. It goes that point down to my spill

09:33 And this is gonna be a little riskier because it's dependent on the false

09:38 . In addition to the dip closure , all of these are constrained by

09:44 spill point over here. While I through that saddle, go through that

09:48 . Lorne and hydrocarbons start to climb in the other direction. My free

09:56 level, my oil water contact on gas water contact from many fall anywhere

10:02 here if they go down as the spill point. Or it may

10:07 higher if it goes down into the point than the trap is filled to

10:11 maximum capacity. If it's above the point, it's an under filled.

10:17 called an under filmed trap, and each one of those cases, the

10:22 column pipe is the difference between the and that Water contacted the gas water

10:30 . So the comp ICT is not same as the total closure. It

10:37 be independent of the spill point. here, it's a really important

10:45 So are there any questions or discussion this before I move on? How

10:53 is it to encounter under Philip Traps filled to this point? Yeah,

11:01 a That's a great question. It depends on your Chris Rock and your

11:07 area. If you have a really , thick service, rock be filled

11:16 the spill point. If you have A not rich, a low carriage

11:23 a civility source rock, then you have probably under filled closure artists.

11:29 we talk about individual false styles, we'll see are there. Most of

11:37 normal fault traps are filled to the capacity. Two things like, you

11:45 , all right. Salt based related in the Gulf of Mexico. I

11:54 traps in the North state have multiple , rocks, a very rich

11:59 rocks, and then he tend to filled. The maximum spoke Cassidy.

12:04 we get in tow, thrust fault they tend to be a lot of

12:09 are Underberg filled. And that's in thrust falls are you got a

12:16 ? Klein on one side, and in client on the other side that

12:22 three. The limit. The migration that can flow into the traps.

12:27 if I've got a sin Klein over , everything to the right of that

12:31 going to go out to some of trap only get tighter garments coming in

12:35 the left. This incline over here the limit of my kitchen area over

12:42 , so my skirts rock in this can be quite limited. And,

12:47 the case of threats, false in , uh, intends to be tends

12:52 lead to under field traps, whereas normal faults, as we see,

12:57 much more commonly fill to the maximum . It's a good question their hands

13:12 we leave this, Okay, I'm go on. Yeah, Are you

13:38 that this did Closure is the least , and that's dependent on my top

13:45 capacity and that, and we'll talk that in some way. That's dependent

13:51 Capitol reentry. Pressure of the top certify have salt or shale or

13:57 That makes a difference in how much this column can hold. Assault being

14:04 best seal shell, being second best still being the least at least

14:13 It also depends on the mechanical one of the top seal, and

14:18 a function of hydrocarbon buoyancy pressure in aquifer overpressure. So if I'm in

14:26 area where I have high aquifer over , that's probably gonna limit my topsy

14:32 capacity. And we'll spend a lot time talking about that and how we

14:36 that the fall dependent closure here depends my false capacity that's limited by on

14:46 my fault, sealed by false And this is where it becomes

14:51 Thio. Consider quite the spirit potential show Godreche show and things like that

14:57 what you're falsely capacity is in This tends to be a more common

15:06 factor than my topsy of failure But it depends in detail on what

15:12 tops who is and what your aquifer pressures are. Okay. And

15:25 um, this will be a kind a discussion point. Come, I

15:31 another thrown fox play, be in . I have a well that's producing

15:38 this corner of fault walk and Question for you to discuss is what

15:46 the total column player If none of false seal Yeah. What?

16:01 What pool going here? 40 Or is it in meters?

16:09 this is 2 m. 40 Yeah, I got 40 minutes as

16:16 . Yeah, so it's probably gonna about actually about 30 m. So

16:22 between 27. 80 and 2800, got just dip dependent closure. So

16:31 this little hold up better what happened false seen or not? So in

16:38 case, my total column lighting. the difference between the crest and that

16:44 concert that fixes the fall. So gonna be about 2030 m French.

16:56 . And if I I'm conservative, just the closing concert here is about

17:00 m. Be extrapolated up and down little bit. You get a little

17:03 extra. Okay. Right now, , what is the problem? Campaign

17:12 only foxy deal the same. We only two controllers. Yeah, it's

17:22 be the same. It's gonna be two countries lines here because if he

17:27 feel here, that limits the accumulation this 27 80 constitute. So

17:35 uh, IFC steals and because you have the same accumulation of about 20

17:43 40 m up in here. How about if, uh, if

17:49 the false seal it falls A, and C also feel 260. And

18:13 are you estimating that? Looks like a saddle down there to the south

18:20 the 3000 contour. If you go , you go all the way up

18:27 27. 40 right? That's that's right. Sudan Here. I've got

18:32 saddle, My contours 28 29 80 . So I go down and and

18:39 this bill point here, and I'm to climb up in the other

18:42 So this saddle here becomes my ultimate point and So if everything seals,

18:50 a b and C steel I can this up from 27 48 all the

18:57 down Thio are 2019 29 90 down to the saddle point since Okay.

19:10 , yeah. So if if b c c l and a dozen you

19:18 get about 60 m in here. ? You're also minutes fill the

19:23 Is this 2019 80 comments over here you bet 240 m 240 to 68

19:30 this spill point and this crest up here. So it's, uh it's

19:38 important to understand what you're independence. the point is and what your dependents

19:44 points are. And this is something will come back to again and again

19:48 we go through the court is actually will wind up for today to summarize

19:59 went through basic concepts and definitions of and strength. That stress is force

20:05 unit area strain is change in Change in geometry in this strain is

20:12 that we can actually measure in the structures that we see. No faults

20:20 organized in structural styles which are related , uh, stressed orientation stressed magnitude

20:27 these to constrain the fault geometries, , subsided structures. We talked about

20:33 damage zones of the relay ramps, like that. And we introduced the

20:39 of political fault these faults to represent , sis or three D contraction from

20:49 . And then we talk basic fought . The football, the hanging

20:54 the football is what you would stand , where you put your feet hanging

20:58 is where you would hang your Okay? And then we talked about

21:05 core that that high slip zone that zone represents the main part of the

21:14 and then the damage zones of minor and fractures that extended beyond that.

21:21 then I basic geometric rules that they be approximated its ellipsis with length greater

21:29 height. The throw is typically a in the middle. I play

21:38 Lincoln throw maximum varies from tending to is a good approximation of that.

21:44 if I know the maximum throw from seismic data straight on, what the

21:50 of my fault isn't Helen correlate. faults and three D seismic data faults

21:57 segmented horizontally and vertically in the Donald Plane. They're linked up by

22:05 ramps in the vertical section, linked by phone calls and the links

22:12 the vertical dimension, maybe extension of of depending on how the falls overlap

22:21 three D and then the trap closure and limiting factors are dips. Bill

22:29 talk to consult your capacity and that steel capacity depends on the mythology you're

22:36 on Percio. Uh, most this is shared with the highest

22:42 If you have to stop, that's . Silty top seals or not so

22:46 that's going to be more risky. then the falsity of capacity. And

22:52 talk about quantifying that in the session week. And that depends on what

22:58 extent of your show Godrich show uh, thickness and the shelling of

23:04 fault couch. Okay, all so that Z, that's where we

23:13 break for today. We'll break a bit. Really? Any commas comments

23:22 on anything that was covered today? have a question on the logging of

23:30 . Yes, they eventually. Hi. Put pressure on top of

23:37 or not necessarily. I'm not. necessarily know, okay, bit.

23:48 really depend on the on the amount strain, the amount of extension and

23:57 . And that's the that's the primary for those centuries. Just structures are

24:09 throughout the world. Or is it or less constrained, like golf Mexico

24:14 other, like deported grammars like that , their common in any deep water

24:24 that's had little or no strange? , so so areas in the Gulf

24:32 Mexico in between. Um, the faults you would expect to see these

24:39 Basten's. Um, like I mentioned , a trusted environment you would not

24:47 to see these except agreeing. For , we we have extension up there

24:55 you would expect to see these. down deep, where you have the

25:00 thrust belts or you would not expect to these thank this is a general

25:19 e mean. Typically for me, always sort of like the rule of

25:23 . Is anything under, uh, under 50 ft displacement or something like

25:31 ? Is this pretty like it's subsidized ? So, like what? What

25:34 you think is the smallest? you may be able to pick in

25:39 section 10. Sure. A little smaller, about 10 m is usually

25:45 good a good guest. And it very much on the resolution of your

25:53 data. Uh, it extreme would , say, some salt.

25:58 where you get below the sub salt . All right, then you can

26:06 . In the worst case, you have hundreds of meters of displacement and

26:10 see it, uh, in higher , ties back like shallow in the

26:17 of Mexico. 5 to 10 m a good rule of film.

26:24 put that over to the geophysicists. you have anything you wanna add

26:29 Yeah, I would say is mostly by the wavelength. So it's really

26:35 function of the velocity of the subsurface and frequency. So? So the

26:40 will we get usually have slower and the high frequency of the seismic

26:46 preserved. So it's much easier to the lower range off Resolution 10 m

26:54 let's say, turned up 200 m so. But as professor mentioned absorb

27:00 doing usually held Theo deeper we the higher the velocities and more more

27:05 of cared. So we have only frequencies preserved. So then we ended

27:10 being able to receive only only a hundreds or even more bigger, full

27:18 smaller than that. So I would it's really function off the wetland that

27:23 we happened in the seismic and the implement dysfunctional food, the velocity and

27:27 frequent. Thanks, David. Okay, good. Thanks for

27:36 I'll just add to that that apply in the verticals. It also prized

27:43 the times that the time slices and length of the false so got

27:50 Seeing the seismic data is really the of the resolvable part of the

27:56 And in some cases, that may quite a bit further what we see

28:01 the seismic data. I don't wanna the other one that questions right

28:21 One more question. It's about the we're talking about a heave, which

28:24 that lateral displacement e don't see that often when, uh like a you're

28:30 just doing work and operate like He is being described. Usually everybody

28:36 about what? What do you think is? What a good way Thio

28:41 the thieves Thio interpret for operation firms the heat. Yeah, we don't

28:53 . Hey, Mike, it's important mapping the fault. Gaps in our

29:00 data in operations to the the throw the displacement are much more important.

29:15 , so operations say, Well, you might want to estimate the heave

29:19 you're estimating a well path to estimate the the width of the gods own

29:26 that you're gonna go through drilling some these long laterals that we have now

29:34 then the heath would be an important to consider on your right. We

29:39 usually consider that we usually just talk the throat. But in certain situations

29:46 Horace Donald's, we should be considering heave as well the way that help

29:54 talk to taking account. The fault specifically when you're mapping is you would

30:00 to use it to fall playing map you contour the elevation of the fall

30:05 its plane and then just intersect your for the upturn in the down through

30:11 . You just match up the contours the to the fall plane and then

30:16 end up with the gap and it interact. So it z not really

30:20 Heath. But that's the only way we've a technology map of a certain

30:28 . Yes, you know that that's good way. Thio todo Is that

30:35 the he would be? That would there to be the best way.

30:40 in some of the some of the default steel programs they used that intersection

30:48 actually, where your fault is, not worried about the heat in

30:55 But they're trying toe constrain the fault to a single surfaced. And there

31:02 look at the horizon kind of troops the fault plane. And really,

31:10 only do that for one side of fault. But they use that Teoh

31:14 to constrain where the fault horizon intersections not writing anything else. Any other

31:48 discussion points. So if we think questions later on is the best way

32:00 contact you via email? Yeah, , go ahead. That would be

32:05 best way. And you can do by email. You can bring them

32:10 in when we meet again tomorrow. one of those. It's good for

32:17 . We're scheduled to start at 30. We will do that and

32:24 we'll spend the morning doing some See discussion exercises. Make sure you

32:32 from blackboard the slides that go along that s so that you can do

32:37 of those exercises a little bit Print those out. If you If

32:42 have that ability, I'm otherwise we'll them on screen. Mhm. But

32:48 take a look at those so you follow the exercises and contribute to the

32:55 . In fact, used the used we've got tonight. Use that

32:59 Take a look through those flies and . Take a look at how we're

33:04 use those slides. And then, , we'll use those tomorrow morning.

33:10 use those talk about noon, break lunch and then in the afternoon will

33:14 on and talk about game mechanics. right, well, thanks very

33:25 Take advantage of the time. I know those things from Blackboard if you

33:29 already, and I look forward to it up tomorrow morning. Thank

33:36 Thank

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