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00:03 OK. So what I've been doing the last uh oh half an hour

00:08 you and I fixed the stupid things have changed between 2022 and 23.

00:19 was basically the order of some of commands, the way they pop up

00:23 up differently. Also, the packages up in a different order. Last

00:29 , we had three packages and we pick number two and you guys very

00:37 followed my directions and picked package number , which really didn't have seismic interpretation

00:43 it. So I've captured that and in the notes which I'll resend to

00:49 . So you have it in the . OK? You may end up

00:53 patrol in, in the future for project. Uh Then we'll say,

00:58 OK. I gotta make sure it's seismic interpretation in the license. Otherwise

01:02 gonna be really frustrated. It's not do what I want. Um And

01:10 what else should I do? What had everything correct for generating the coordinate

01:19 system. But in 2023 it wants is immediately when you set a new

01:26 . And you're saying, well, it asking for uh and I had

01:30 the information in there, but in and before, after you imported the

01:37 , it asked you. So I noticed which I went over with one

01:44 two of you. Uh yesterday. a good Survivor skill that I don't

01:50 in the notes is how to scan trace headers. I don't think I

01:57 it in the notes. Do I ? No? Ok. I'll put

02:01 in. Uh so that you can sure that yeah, that looks

02:08 Because typically what you'll have you OK. Even back 1015 years

02:16 people were doing artificial intelligence. I , this isn't something new. And

02:22 one of the first projects we had Amaco back 30 years ago in artificial

02:28 was reading Segway data and it would , oh, if bite 17 is

02:36 integer between uh one and 10, probably a sample sample interval and it's

02:48 a high percentage that it was recorded Petty Rae Geophysical. And then,

02:54 , if fights number such and such very large numbers like greater than

03:03 0, it's probably a coordinate. then if it's, if the next

03:07 is also probably a coordinate, then might have been recorded by CGG.

03:12 serious. This, we actually had big research project like this because,

03:17 know, companies would trade data or buy a company and then you got

03:21 these tapes. Well, what do do. So you have to have

03:24 way of looking at it. And patrol has a lot of buttons that

03:30 . I'd say 75% of the time you just say, ok, let's

03:35 to load it and it might do good. Uh But very often the

03:42 header and I don't think I captured too. When you loaded the

03:45 there was some information on the bottom said where everything is stored. And

03:51 always very rigorous to make sure that there. Sometimes people have it in

03:59 landmark and they'll just copy what the header was that said it was stored

04:04 certain bits. But now when you it from landmark, you put it

04:09 different bites and so it, it actually lie about where things are.

04:14 you gotta figure out where things So I'll try to capture that as

04:19 . OK. Lily. What you ? OK. What do you color

04:27 ? OK. So what color bar you like? So I I,

04:35 . So you're trying to save a bar or, or trying to read

04:40 in, read one in. So then here it's going to uh

04:48 called the colors. Yeah. And do do do do do do hang

05:01 . Yeah. Yeah. Yeah. on. So we're back in the

05:05 all the color. OK? OK. And you got a user

05:12 find OK? Go back to And see if I can right quick

05:24 you're looking at the template maybe I it that makes it discreet.

05:38 Yeah. Ok. Ok. Where our data set? Uh ok,

05:45 gotta go to input. Ok, it is. Ok. Ok.

05:54 what do you wanna do for the in line? Is that what you

05:57 do to kind of? Oh, . Oh, ok. So then

06:06 gonna go, there you go. ugly color. Probably just once I

06:13 um the Oh OK. So you a color bar now uh see up

06:24 see it says global color bar or . So you want to import

06:29 So now you're gonna go in here then these are ones you've used today

06:35 yesterday it green members and then there's of them. Now you're gonna have

06:41 of them and which one do you pick? How many there are?

06:45 . So you're gonna pick one if finalize history? Oh, so for

06:54 I would pick gray scale. Let's see what? Yeah. Oh

06:58 you made that OK. Good, . OK. And you say apply

07:03 but you're applying it to the seismic . Um So then you put if

07:11 , if you want just red, blue go back to click that

07:16 Now you got your red, white and then OK, that's OK.

07:21 just got the scale differently. So go to the Yeah.

07:30 So go to color make it a one and yeah, you can keep

07:38 . Oh yeah, you can do . Ok. Now you need to

07:42 let's put the limit so makes that 25 and make the bottom one minus

07:59 . Yeah. Ok. By that . Ok. Uh 01 other thing

08:05 minus 25. Yeah. Yeah, you. Ok. And uh hit

08:12 . Ok, that's good. And we go back to the wherever your

08:17 was. Yeah, so that Yeah, that's the Varian. And

08:24 I would do do do a uh quick on that guy. OK.

08:31 no um no right. Click on name and it should say info.

08:37 should be info someplace or maybe double quick on sorry, double

08:44 OK. And under info. she has this name, just erase

08:51 name and type in variants. The thing is forget the Corey because what

08:59 ? You can't read the stupid Iange. Yeah. Ge good.

09:14 , good. Now you know what is? Ok. Now you're

09:16 now you can uh again uh double on it and go to colors and

09:27 gonna, oh, you've got one . OK. You're doing pretty good

09:31 . We were playing with this um . Remember? So you got

09:37 You were in some funny, I know where you were. I wouldn't

09:45 about it. How are we You, Kathy? Ok. Uh

09:57 I'm going to the? Ok. you're ok. Good. Are we

10:09 ? Good. Good. How about ? How's your, how's your husband

10:13 with the sick? Two year Oh, I can't, you

10:18 I've got a two year old If he is sick, he didn't

10:23 there is no one. Yeah. , I know. Oh,

10:32 I'm gran, to my bigger grand . My four year old could never

10:36 Grms. So she called me grumps my two year old calls me

10:43 Jumps. OK. That's a classic . Yeah. And they scream when

10:54 want mom. How are we doing ? OK. All right. We

10:59 . Contento. OK. On a . OK. You're all right,

11:10 good, good. Um Did everybody the, the picture icon, the

11:26 icons? Let me show you interactively uh what is uh Jessica listening to

11:38 ? I am. Yeah. I'm gonna try to show something on

11:42 screen. Oh I can't show I'll show something on the screen in

11:47 bit. OK. I gotta load data we have here. We got

13:51 know it. Mm Pretty good. . It OK. OK. So

20:53 you can look at the screen a , can you see it? Let's

20:58 the I'm gonna turn the light off for a bit. OK. You

21:06 can see that. All right. I think uh Jessica and Felicia is

21:12 here. Um She can see Oh I just happened. I,

21:19 just happen to have a picture. ? Oh Where my, here it

21:23 . And I have a turbid coming here or if you can see my

21:27 thing. Oh, I wanna capture . You see up on this bar

21:33 . Bar has got a name. forgot what it's called. Got a

21:37 icon. So I'm gonna click the . It goes into the bit

21:44 I've got powerpoint over here. I'm hit control V. There you

21:51 OK. It's gonna be exactly that can click this. Uh I'll get

21:58 of this. I can click this while it's covered and it's, it

22:06 enough to do it. OK? um that's, that's quite handy.

22:12 , the only then you'll find annoying you go through your career as an

22:22 . There's lots of annoying things, one of them here, I'm looking

22:25 it. Oh, just this And then Utah says, hey,

22:34 , you see that and then he my hand, everything is rotate and

22:37 can never get back to that perspective . So I want to show before

22:41 after with interpretation without interpretation, one attribute three original seismic. I

22:48 get that same view that's like You gotta have to, you have

22:53 kind of save intermediate projects and then you can get that same view

23:00 time. But other than that, don't know, do you know of

23:04 Bob knows a different way of saving back to a particular view.

23:10 it's hard. I mean, uh just hard and it's kind of

23:15 But what can you do? And other annoying one is 3d visualization.

23:22 , and you're working with transparency, , not the exercises we're doing.

23:27 are pretty simple, but I'm talking like I've got five lines and I'm

23:33 put them together five vertical lines and gonna change the opacity curve on

23:39 the yellow, red, white blue color bar to look at the amplitude

23:46 then I'm gonna rotate them. So optically stack in a certain way,

23:52 the transparency and that fault shows up or that channel falls up beautifully.

24:00 then you come back on Monday, that channel? How do they do

24:08 ? Really annoying? So you'll find happens and then you'll come up with

24:12 own ways of remembering how you did , like writing, writing things

24:16 taking screen dumps, putting them in . That's about the only way of

24:21 it. So anyhow, OK, just want to mention that. So

24:26 you make for the, the lab that I'm asking open up powerpoints,

24:33 the figure in there, maybe write lines of notes or something like that

24:36 there's a color bar, I'd grab color bar and just put it to

24:40 side because if you publish a paper publish a, a thesis, that's

24:45 you wanna do. You have a bar that you don't want to have

24:48 little bitty color bar with all these bitty numbers that you can't read and

24:52 mean anything. Like if it's Amplitude have a color bar, maybe

24:56 white, blue, you're gonna say zero, negative. Keep it

25:02 Minus 25,000 plus 25,000. Simple. don't need all those little numbers in

25:09 . Nobody, nobody can read OK. Ok. Shout out if

25:14 got a question put on the part going to overlap his lane.

27:23 When laughing at this point depth. . It's not the right.

27:36 so you have one in front of other now. So but make this

27:41 four or is it gonna be Yeah, let me make it every

27:46 and then let's go go up a . Uh so it's 2020.

27:53 Ok, you can type it Um so and so they're both at

28:00 now or is one at one with one? Ok, so make the

28:06 one at 2000 uh 2820 16. I doing that right? My or

28:20 I guess make 14 milliseconds above the . That's what I want to

28:25 You can do that. I can't I'm looking at everything upside down.

28:32 . 2000, 2000. Well, now if you got them both at

28:35 and it's ok. Well, no this is the 2000?

28:41 ok. Ok. So that that works kind of. Ok.

28:46 . But when you put them on same level then it doesn't work,

28:48 ? Yes. Ok. So let's to the next thing you are going

28:54 . Which one is your base? guess it's gonna be the uh

28:59 So which one is the amplitude this ? 2016? Yeah. Ok.

29:05 cool. Ok. That's cool. you're gonna hit OK, Here,

29:13 this white blue thing. Click that display blue boxes. You're gonna put

29:21 check in the blue box. You're uncheck. What else do you have

29:30 here? Oh, none of OK. That's OK. So the

29:35 one you have displayed is this now click your VCR button and oops.

29:48 . Now you have one still displayed actually that where is the other one

29:55 was saying? OK. But Oh you had more stuff.

30:04 Where I only wanna have this guy the migrated data and OK. Is

30:15 what you have now? Yeah. . So take that. Yeah,

30:18 have that display. OK. So , so you can go uh

30:23 maybe, maybe animated. So they be locked together. No, it's

30:30 . OK. Wait. OK. that. Oh I don't. Oh

30:35 it's black on black. OK. on there. You another thing there

30:39 be a paint can here or some . Uh OK. Good.

30:44 Well, it's not there. Um me show you the thing because I'm

30:50 talking to here to Zach. In , I have a paint can of

30:55 on this particular picture. So, , let me go to my 3d

31:09 . Um, where was the paint at? It's the r uh,

31:17 to do. Oh, or after ? Ok. Ok. The paint

31:26 not empty and it's ok. It's upside down. You see the little

31:29 can icon, you gotta love icons patrol. You click that and you

31:36 make it go to a white Now, you can also change

31:41 So I might have it in the . I might not, you might

31:45 , click on and it'll see. right click and the de oh

31:55 Let's say you're writing um you're writing thesis for University of Houston and you

32:04 to print a hard copy. You're go through a whole lot of

32:10 a whole lot of ink with black . OK? If you wanna submit

32:16 for publication, the black background again just extra ink. The printer publisher

32:23 probably be angry at you. So know, you can change it

32:26 to uh I would call this a gray. This is white.

32:34 The touch screen. This is, anyone use the touchscreen here? Have

32:39 seen anyone use it? Who? . OK. What's he teach?

32:58 ? OK. OK. OK. modeling, geology, modeling, structural

33:05 . OK. Anyhow, it takes , takes a lot of choreography to

33:08 a touchscreen, especially in front of group that's really embarrassing. Anyhow,

33:14 is white, kind of a very gray. This is a great

33:19 OK? Because it's not stark. So uh just know that in

33:25 you know, you have to write report for work or something like that

33:28 you don't wanna like just have a done for black. You can put

33:33 and things a lot easier, you , little, little things.

33:40 So you should have them linked together , right? Oh, so

33:45 take this one off. No, quick unclick that I think that there's

33:51 issue. Nothing. Oh, you don't wanna be in a two

33:56 window. Let's do it in a window. Ok. Now you've

34:02 I see. Let's go. Let's look at the Z through the

34:08 Yeah. Take that off. Now you're gonna hit your little blue

34:11 button thing. Ok. And click variant blue button and, because they

34:22 us do all the, the majority the steps in one seat were in

34:27 . Oh, ok. Ok. fine then. Ok. I didn't

34:30 where you were and you hear you're at a True Cube. Ah.

34:35 right. All right. You're looking the, ok. That's cool.

34:39 think you're all right. Ok. . Mm. Yeah, once you

38:27 it, they can do it on computer. Now. I need to

38:37 the answer because the system will. . Right. And I, let's

38:45 at the answer. Ok. That's embarrassing. Ok, let's do

38:57 Like ch, let me make you . Mhm. Mhm. Ok.

48:17 what I did. Ok. ok, let me show is,

49:23 , Jessica on there yet. I'm still here, beer again.

49:31 still here. What you do help help the German economy. It's October

49:36 . Right? Um, actually Oktoberfest in September. Oh, your speaker

49:46 not working. OK. She's OK. So um I'll let you

49:54 her and then I'm still, you're recording me, right? OK.

50:01 . Tell me when to go and try to capture this image too.

50:13 There will be AAA PG explorer. any of you get the A PG

50:18 . It's like a, he writes Geophysical Foreigner, um which means every

50:28 he needs to have somebody to help write it. Uh And uh when

50:33 was with the big company, the two years worked fine because there were

50:38 24 geoscientists there, he could draw then after two years, people started

50:45 their doors on them. They didn't to help him anymore. And uh

50:51 then he's drafted me to help and . So though, I think it's

50:57 month's issue, the little thing calling title. It's only a two page

51:03 in the A PG explorer. So , it's getting, getting bit by

51:10 many bites. Isn't that a cute ? OK. So if you did

51:16 I just did when I was playing loading the data and then realizing

51:25 I just use the default. Hey, everybody uses the defaults and

51:30 default is you take that big which is I think 200,000 and a

51:36 number, which is maybe 100 and if I recall what it is.

51:42 then I'm gonna choose to realize the . And that means I take the

51:47 bit data and I convert it to bit data so that it's easier to

51:51 at. Oh, it actually does things. Um And I could share

51:56 with you because that's what's in the . I'll try to put that

52:00 Um It saves the data as brick . So I think in the

52:06 the first exercise I have you look in lines and go through them and

52:10 cross lines and go through them and cross lines are gonna go slower than

52:14 in lines. These computers not too because it's got a ridiculous amount of

52:19 in it. OK? But my , it goes much slower and then

52:24 slice is slower still. So uh do a time slice, guess what

52:29 have to read in every single extract one sample and throw everything else

52:36 , not very efficient. So the format breaks the data into bricks of

52:41 size, typically 64 by 64 by boxes. OK. And so what

52:50 will do for uh maybe this data , if I can do my arithmetic

52:56 ? It will be 16 bricks deep about 20 bricks wide and about 24

53:03 long. So if I wanna pick time slice, I just bring in

53:08 row of bricks. Not all of data. If I wanna look at

53:12 horizon slice, I just pick the that overlap that horizon. So you

53:18 see where it's much more efficient than in trace by trace in line,

53:24 by in line, followed by in . OK? So I just clicked

53:28 buttons. It said, realized it go eight bits. It's gonna take

53:33 number 200,000 minus 131,000. OK? divided by 255. And so the

53:44 of my bin is I can't do number in my head, but it's

53:49 400,000 divided by 250. That's the of the bin. OK? So

53:54 is those data. Then I went same data volume and I said before

54:02 realized it, let me say I the maximum value to be 2500,

54:07 minimum value to be minus 2500. almost 10 times finer or 10 times

54:15 . OK? And so 200,000 to . So eight times less, then

54:24 gonna scale that value of 225,000 minus divided by 255. That will be

54:31 B touch. So here is the , same color bar, same range

54:40 the color bars that the color bar be 25 to minus 25. And

54:47 here is rescale. Default. We're , default, we're scaling,

54:56 we're scaling. So you'll notice I can't really use my mouth but

55:04 can see my hand here, this on that color bar. That's the

55:11 that's near zero. I can show color bar. He said you can

55:19 the color bar. See here, one is the default 200,000 to minus

55:25 100 and 30. 0, it the number here minus 134 to 2200

55:29 12,000. Oh, here's my color . I'll put that over here.

55:38 says, well, I can't make a lot smaller, but I can

55:42 it a little smaller. Ok. how does, what does this

55:49 This is my a my data are binned incorrectly. Let me look at

55:54 color bar from here just to make I'm not making a mistake and colored

56:03 we go and, and, maybe that's the point no minus 25,000

56:13 25,000. Ok. So same color . So what's happened? Everything is

56:19 scared at those lower amplitude. It's , it's just not being mapped

56:27 So the, the peaks and the are doing the, the how would

56:30 call it? The high, high minimum are doing fine, but

56:37 losing the detail in between. So , you need to be careful.

56:41 can't just trust the defaults. In fact, what I'll do is

56:46 will, I think I have this here. I think Wednesday with

57:00 Um probably a raise it. OK, I'll put, put that

57:20 , I'll put that in the, the lab notes. That's the best

57:23 for it now. Um, everybody's doing. Ok. Everybody's happy

57:38 trying to figure out what, why one look like crap and the other

57:42 ? Ok. Right. Yeah. . Ok. Let me give

57:47 uh, I know I have this , uh, uh, I incorporated

57:53 in one, I did two weeks and Oman and I did lectures and

58:04 display. Same kind of thing I to you guys about but I may

58:13 added another pitfall. Where did I that pitfall? Mm hm hm hm

58:21 hm hm hm. I guess it's in there. Where would I put

58:29 ? Oh, well, that's because it's not the one on my

58:37 . There you go. No. ? Yeah, you're right.

58:51 I'll find it guys. Oh, am I gonna get that? I

59:03 why. Mhm. Because I didn't it. Yy. Yeah, I

59:24 to use the web, you Oh, yeah. Ok.

62:54 Hm. Why can I find Ok. I know I put it

63:20 . You want, I got it . Ok. I said that

64:16 So here, right? Ok. , you feel like uh everything is

64:43 pretty gone out and whatever? Ok. Hm. Thank you.

66:21 lost my, oh, maybe I was in the internet in Google

66:28 . Where did it go? This , no, this is, but

66:35 was just doing it. Um, that it? No, I got

66:41 gotta go back. No, you open it. Oh because I was

66:47 you need to uh got it. . Interesting. I know how we

66:56 . I know I was just I you know on the edge and Microsoft

67:01 ok, so we'll use edge. . That's fine. That's edge.

67:06 we need uh what its doctor? ok. I think no that's not

67:16 . So yes there um I don't leave it. Ok. Uh where

67:32 my edge go? Ok, here am. Ok. Mhm.

67:47 I was in office 365 logged in was just logged in. Oh

68:03 Ok. Many. Mhm. The what? There's no way that you

68:47 know. Yeah yeah it's perfect um thank you. Thank you.

70:12 All right. Hello. Well the . So just so when you start

70:57 um that yeah. Ok, so is ok. Yeah then I gotta

71:17 to all. I OK. Thank you so very much but that

71:57 so um you know what I know . Mhm. Mhm. That

72:29 Ok. You. Mhm. Yes, sir. I know.

72:47 funny. Ok. Yes, thank . So you um um so that

74:59 ok. Mm. Thank you. then we. Ok. Mhm.

75:29 . Mm. Ok. Ok. . Ok. I found the article

79:06 I can't remember my password from getting . Too many passwords. I'll figure

79:13 out tonight, but basically this is one getting bit by too few bites

79:18 September. And it showed that same of problem. I can show you

79:24 , a crude version of the same if you. All right with

79:28 I, I think I've got it . Uh Download tank. I gotta

79:39 to download, here's a crude This isn't it there it is.

80:08 And I know, damn it, me see if I can find the

80:17 image. Mhm. Oh OK. , no, no, no.

82:50 where it was. I remember What? Ok. Mhm.

83:30 Ok. Let's see if I can this. Uh Are we recording for

83:35 ? All right. So these are pictures from the book I'm writing and

83:39 is in the A PG thing, PC explorer for September. But what

83:45 trying to show on this picture is way we gener, we try to

83:50 data as bricks and all the commercial does this companies like blue wear,

83:57 have four and five dimensional bricks so , very efficient uh access to prestack

84:06 . And the point here is, , if I wanna slice an in

84:10 , it's pretty easy. If I slice a cross line, it's quite

84:14 bit longer. And if I want slice a time slice, it's the

84:19 of all. So if I have brick format, it's faster, then

84:24 paper goes back to uh 2001 from Earth from Texaco. People was developed

84:31 Texaco, was spun off as their company 3D Visualization. Then Landmark bought

84:37 . And that's when 3D 3D visualization commercial software uh really hit, hit

84:43 ground and uh they show uh pain still over there. Uh Here's

84:53 happens with it to 48 times. root means amplitude and the one on

85:04 right is the four times root mean of the data. OK. So

85:10 gonna, you're gonna pick some of numbers out of a hat as to

85:13 to scale the data. And in example, uh it's nice and

85:20 OK? Just like the data should . And in the previous and the

85:25 times it's quipped. Remember I well, it's OK to quip so

85:30 as you know, you're quipping. now this is what's stored in the

85:36 when it's converted da data. Now gonna compute frequencies. So in a

85:45 minutes, maybe 1015 minutes, I'll talking about instantaneous attributes. You're probably

85:51 with them right now and a sharp has higher frequencies. Than OK.

86:02 this is gonna have high frequencies to it. And so with this other

86:07 here and then what happens when you instantaneous frequencies on the left, they

86:14 a nice smooth frequencies and on the , they have a couple of artifacts

86:19 got created. OK. So his here is that when you got bright

86:25 and not, you can have artifacts the bright spot. So that's out

86:32 . Now, here's a data set to be Gulf of Mexico. Um

86:40 here's the way Petrell wanted to bring in ranging from minus 30 to plus

86:48 . And here is the histogram under around zero like we think it should

86:54 . And then I take the same here. It is in certain

87:00 they bought it but they changed the not to be 00 minus 25 to

87:15 . Thanks. So this looks fine bit data and this eight bit data

87:24 it looks OK, especially up but notice there's something different in this

87:32 box. I see a lot of areas. And then in this other

87:37 , I'm going to uns scale the minus five and five instead of minus

87:44 . And here's the default I'm gonna symmetric and I minus 25 plus 25

87:51 minus 5 to 5. And then I plot them with the same,

87:57 same except it's, yeah, this is going to have, it's got

88:06 colors. So the beams here are be tighter, five times tighter than

88:13 . So let's look at those and go look in here and I actually

88:17 it in patrol because you put your on it, you click, it

88:21 you what the values are, what amplitude is. Well, there's a

88:25 of zeros in here. OK. I've got a zero, I've got

88:30 numbers in here and here because the are d are, the number of

88:38 per bucket is five times denser. don't have that dead space in

88:47 OK? Now I'm gonna run instantaneous , huh? Instantaneous frequency because that's

88:54 Myers did 24 years ago. Here's the original data, 32 bit

89:02 Here it is on the eight beat data carefully scaled. Not that almost

89:08 . And then here is the one improperly proper, too coarsely, too

89:14 scale using the deep ball. And can see all this black hair that's

89:18 trash. It does. It, thinks it's all zero. It thinks

89:22 data are zero and they're not. it gets worse than that because here

89:32 was careful and I, I say in the text, I probably have

89:36 picture when I scale it from minus to 25. I've intervened. I

89:45 it's symmetric about zero. OK? I let it use the default minus

89:51 to plus 26.4. It's not There is no bin that is at

90:00 . So my value of zero is , and this picture is like point

90:11 . All right. And you well, that's not so bad.

90:14 , it can be disastrous because in workstation software, they don't keep trace

90:20 . So they don't know where the traces are and they don't know where

90:24 mutes are. So something is constant and I export it into patrol and

90:32 want to do a bo analysis. here I've got him oh amplitudes increasing

90:40 offset for good bright spot. Yeah. Yeah. And then it

90:44 to 0003. Well, 0003 is a dead trace. It's got a

90:50 in it. So it's gonna try fit a curve that goes like that

90:55 you get garbage. OK? And if you have mutes or do

91:01 things that are sensitive to edges. , if I have a strict zero

91:06 there, I can say, all , that's a mute zone or no

91:09 zone, whatever it is, don't in there. And then when the

91:15 wants to go in there, be careful about it, you know,

91:19 it in some way. Well, it thinks it's alive, it's,

91:23 gonna die and give you problems. the paper, the picture I just

91:28 you was for the data you're working and um you know, kind of

91:33 careful that you gotta think about The conservative thing, saving his 32

91:40 alternatively, save it as 16 So, but uh here's a problem

91:45 comes in, it's in that, that little September Geophysical corner thing

91:51 you know, I've had and Heather students coming up from Petrobras and they

91:58 , oh, we'll give you a and then you can do this

92:01 do the analysis on the deep stuff the basement. We were really interested

92:06 it, but it's not something we time. And here one of the

92:10 she came in and she had all data and up shallow, well

92:15 the top three seconds look beautiful. then where they wanted her to look

92:19 and five seconds. Well, a of the data was simply set to

92:25 because it was, they gave her eight bit data set from patrol or

92:31 wherever exported it as 32 bit. why? So she's thinking it's 32

92:38 because that's what segu is. But with eight bit converted back to 32

92:43 and she wasted like four or five not knowing what it was, what's

92:49 on. OK. So we will you know, kind of go to

92:54 place you can keep your projects open then I'll start lecturing maybe in five

92:59 . Is that ok? Ok. we'll go to close to six o'clock

93:13 I will send you that little article I get home and the church.

93:44 . It'll turn out that the eight using the default. It is bad

93:50 seismic amplitude data. Uh In contrast most, not all of the

93:57 for most attributes, eight bits going be fine. Our frequencies are gonna

94:02 from 0 to 100 and 25 It's fine. It'll be good to

94:07 half frequency coherence variants will go between and one. You'd be hard pressed

94:14 see details, you know, less 1 255th of that range. When

94:20 comes to R MS amplitude magnitude spectral , then we got to be more

94:27 . So I'll try to capture that we go through the course. Uh

94:33 I mentioned it just because recently a of our students said, oh,

94:37 have been burned by this kind of . OK. So most of you

94:42 started a little bit with grace right? So let's see what they

94:47 . What we want to be able do is visualize something called the Hilbert

94:52 of the data by looking at the seismic trace. Then second use complex

94:59 attributes as building blocks for interpretation and attributes use attributes computed from interpreted uh

95:11 structure maps to enhance subtle faults and . So we're gonna calculate like the

95:17 magnitude dip ASU of a P surface statistical measures of amplitude above or

95:23 picked horizons to map chaotic features that can't be picked. So we have

95:29 very complex uh channel system that's been three or four times. Uh So

95:41 no simple reflectors inside the channel. rather a bunch of heterogeneous packages.

95:48 , we can pick an area or may be parallel to the top of

95:53 channel system. Uh And then a simple reflector below it, not the

96:00 of the channel, but one below calculate RM amplitude. We're gonna be

96:05 to see that channel it well, . So here, let's start with

96:10 Hilbert transform. I've got uh this what the Hilbert transform looks like in

96:17 time domain. So I've got time from left to right. And here

96:23 my analysis point right here in So what I do is I take

96:30 sample that's one point to the And I multiply it by 11 point

96:36 the left, I multiply it by one, three points to the

96:42 I multiply it by three points to right. I multiplied by one

96:49 three points to the left minus one , five points to the right,

96:56 5 points to the left minus 1/5 7th, 1/9 all the odd

97:03 So basically, we're taking a weighted of that grace where the weights are

97:12 over time with respect to where the of where that sample is.

97:20 Um Zach here, of course, me to use the word convolution.

97:24 I'll say yes, we can evolve little brown pattern with the seismic

97:33 That's all it is. It's just weighted average. OK. Now,

97:38 of all, I want to say not instantaneous, it's a weighted average

97:42 some kind. So the instantaneous attributes instantaneous. They're not measuring exactly at

97:50 spot. It's smeared by the Hilbert . And then because our seismic wavelet

97:57 you know, peak and sidewalks, also smeary. So nothing really instantaneous

98:04 . That's the word that has historically used. OK. Paper from Tory

98:10 in 1979 I might have included It's a classic and here's the seismic

98:18 , here's the data. This one here is a Hilbert transform. It's

98:22 three names. We call it the transform of the data. We call

98:27 the quadrature of the data. We it the imaginary part and, and

98:33 . Is it the quadrature or Hilbert quadrature? OK. So that comes

98:41 electrical engineering. And Hilbert transform is mathematics. People from Kant and

98:49 but also other uh sign analysis. they like to use complex numbers.

98:56 they'll talk about real and imaginary Three names are the same thing get

99:01 to it. OK? It makes head spin. You'll read the documentation

99:06 patrol and they'll talk about the imaginary . Hold on. What's the imaginary

99:11 to help her transform or I'm the quadrature. So they'll call it

99:16 different things in the documentation. Add confusion. OK. Let's look at

99:23 peak. A peak goes from a to plus zero crossing a trough goes

99:32 a plus to minus zero, crossing minus to plus zero, crossing goes

99:39 a trough and a plus to minus crossing goes to a peak. So

99:46 it does is it rotates the data 90 degrees. OK. Um Not

99:52 to do um If you have thin a thin reservoir, what will happen

100:05 that, that tuning effect is well, we'll go into that but

100:09 gonna go rotate those data by 90 . OK? Now I've got the

100:14 transform. I can plot the data a horizontal axis. I can plot

100:21 Hilbert transform on a vertical axis and can think of them as real and

100:26 parts. Um But first of let's take the data squared, the

100:33 transform squared, some of them take square root that's called the envelope.

100:39 got another name too. Reflection And what for I? And you

100:48 see the envelope is insensitive to So even though this one is 90

100:53 phase, the envelope. Thank Here's my plot. So what we

101:03 then here I'm gonna calculate an angle the real axis and here is sample

101:10 milliseconds, 2002, 2004 2006, , 2010. Ah The phase is

101:18 and then here for whatever reason, , the phase is decreasing, it's

101:24 in the other direction, then the increases again. OK. So here's

101:31 phase and it's gonna be the art of the Hilbert transform of the part

101:38 the data and the original data. uh so here's zero degree phase.

101:43 increasing. Oops wraps around, comes , wraps around. Oops here goes

101:48 . What the heck is that? ? Now, if you think of

101:53 is, I mean perspective, just it. So that's what this bottom

102:05 is saying. We gonna take the of the phase and everything is kind

102:10 fine except what, what the heck negative frequency. And my vibrator only

102:16 to 60 Hertz. How do I 90 Hertz in the data? That

102:21 make any sense? What are computational ? And then here is the um

102:30 those artifacts occur. I've got a one negative frequency here. Oh That's

102:36 my phase went backwards. This is my phase went backward phase went

102:41 What about the positive ones? Oh phase went particularly fast. Well,

102:46 do they occur? Uh at the of the envelopes, see how they

102:52 the red wines all are at the of the envelopes. So what we

102:56 is the wave packets are interfering with other and that's what's causing those,

103:03 uh artifacts and phase. So if want to fix that and I recommend

103:09 do fix it, we're gonna take weighted average frequency. OK. This

103:14 what most people do. But there , there are instantaneous instantaneous frequencies out

103:21 . So we're gonna take a window 11 samples and it's stable at the

103:28 . So it's gonna have a nice answer. Uh It's gonna be biased

103:33 the peak of the envelopes by this of weighted average. OK. I

103:39 down to Terry Tanner's uh office while was still on this earth because

103:44 he died maybe 10 years ago. this is how we used to display

103:48 at seg meeting kind of like uh kids might do in uh junior high

103:54 . You get a big piece of board and then you carefully get some

104:00 , try not to gloop it too and then and wetter gas and plastic

104:08 with something called the Leroy pen real . You're very fortunate to have to

104:12 that anymore pain. His, his are perfectly well. OK. But

104:23 we are for envelope instantaneous frequency weighted . And the apparent polarity is that

104:34 envelope finds the kind of the OK. Let's look at the bed

104:41 and the wedge model high impedance, impedance, high impedance, negative reflection

104:47 the top positive reflection on the bottom peak trough for the zero phase part

104:53 the reflection peak trough peak for then degree phase part of the reflection and

105:02 they interfere, we have tuning and it gets weaker and weaker goes to

105:08 . Here's the Hilbert transform. It the data by 90 degrees. So

105:13 I have a trough here, I a zero fraud. And where I

105:19 a fee on the bottom, I there it is uh is always a

105:28 crossing at time. Uh 50 in picture. Well, you can see

105:35 was there. So for a thin , it's not uncommon if you're gonna

105:40 a horizon that's at the top of thin bed. Let's pick, let's

105:46 pick the zero crossing on the original . But then display the Hilbert transform

105:52 to actually show how, what's the change in that thin bed? Otherwise

105:59 get zero. That's not very OK? All right. So here's

106:07 answer for the not talking to There's too much information in there.

106:28 ? It's just not telling me much the wavelet. It's telling me about

106:32 particular part of the wavelet. What's face? So there's another thing we

106:40 . Mm W what attributes? So gonna as the zones by the

106:52 No stop the envelope and then the the same like we saw and then

107:10 and the drop times where, where the, the minimum in the envelope

107:17 ? OK. Here, here, , here, here and here.

107:23 . So we're gonna go then hello, extract the instantaneous frequency where

107:33 nice and stable and apply it to . We're gonna gonna go to the

107:39 low one constant value per energy We're gonna do the next one.

107:45 then the next one is to get idea how we're taking the value of

107:50 attribute at the envelope peak and say represents the range of the envelope and

107:56 kind of stabilizes the thing. You get any negative frequencies which don't mean

108:01 . We don't have any erratic positive , we get very reasonable ones.

108:07 here is the envelope. Um that's OK. Maybe I'm losing some

108:13 I still see the tuning frequency or the tuning is strong and here's the

108:19 phase. Now this one I like than that previous. It had all

108:25 to put out here. And what have is the top here is kind

108:30 like purple. Oh that's minus 180 plus 180 and here is yellow.

108:38 that's zero. So remember I had zero phase wavel at the bottom and

108:43 negative reflection or 100 and 80 degree at the top. Then as I

108:50 it read oh 96. OK. wavelength frequency OK. Uh kind of

109:01 moderate frequency of let's say 25 or Hertz here, then it gets a

109:07 lower because of the side of and it gets higher here at 30 after

109:14 I mean, there's the instantaneous. in my book, the uh wavelength

109:20 are better finding you use these Um They're in every commercial software package

109:31 was really easy to write. They their impact when he was at the

109:37 Service Road up, uh happen to Fort Worth Station and he's got the

109:47 frequency. So uh high frequencies and is in yellow and lower frequencies are

109:57 blue and then he's only got some the wells shown. He's got actually

110:01 100 wells. So he's got a map. Ok? And I remember

110:09 or maybe. Yeah. Yes. I shut out blend colors and

110:14 That's what I did here. These the kind of things you do.

110:21 ? Now another attribute that's used particularly a Strat ofer. OK. The

110:31 don't tell Jay. I did OK? I just took a drink

110:36 water. Damn. You can put on your hands and say because it's

110:41 you're, you're worried about COVID. Oh, if you're a Strat

110:52 any of you guys, photographers or ofer wanna be Strat first. Absolutely

111:00 . OK. She's got good. you're a geophysicist man sequence Strat

111:06 Really painful. Where's my geology folks us about why? Why do we

111:17 about sea level rise and fall? , it was OK. Good.

111:23 you know something. So OK, share with us, please. Why

111:29 we care about sea level rise and in terms of the depositional environment,

111:33 say right here in the Gulf of is like creating the entire for

111:44 OK. OK. OK. So say I wanna look for turbines in

111:58 Gulf of Mexico. Where do I look? I mean, I got

112:02 seconds of data. There are a of places to look for, of

112:22 . OK. So right now 2023 at a high stand going higher.

112:32 anybody live in Queer Lake where I to live, I was 10 ft

112:35 sea level. Anyhow, as sea rises, we're gonna flood more of

112:42 earth. Oh, there the ocean transgressing against me like sinning against

112:48 That's how I remember transgressing. It's like doing something against me.

112:53 right. So sea level is rising it's gonna dump more clay and stuff

112:58 top of everything. If sea level , that regresses. If sea level

113:06 , we'll have a falling stage And then we have a low stand

113:10 sea level is an absolute low. during the ice age, then all

113:15 the sand and uh sand fans like Mississippi Delta all of a sudden that's

113:22 above ground and it's unstable and we'll a flood, heavy rain and it's

113:29 take all that stuff and send it into the deep Gulf of Mexico and

113:35 a turbine. OK. So where look for Turbos is that low

113:42 So you were, you were you, you, if you had

113:45 more positive attitude about Strat gray, could have answered that very cogently.

113:53 . So one of the pieces of , oh, this is a turbid

113:58 and it's gonna be sand rich is know where does it fit in the

114:03 boundary? In carbonates, high stand low stand. If I've gotten a

114:09 platform and if I can tell when a low stand, well, then

114:14 Bahama Islands are gonna be exposed to , they're gonna dissolve and have more

114:24 in them. And if I can the level high and preserve that

114:32 that understanding of when things happen when migrated when they were exposed is all

114:39 of the exploration system. And that's what your seismic and sequence ders

114:44 and mechanically what they do on this with the arrow. Now, that's

114:50 you don't wanna do it. I that Stephanie, you don't, you

114:53 wanna pick all those fingerprint. Ok. So my brother worked,

115:00 my brother, uh, Alan, worked for FBI for a bit and

115:07 they were doing finger based databases, it, they didn't start by matching

115:12 the fingerprints they matched at the on and a lapse, the intersection of

115:18 swirls. Yeah, you've got a on your hand. You're real

115:24 You know, you cut yourself as knife. Remember when you were

115:27 Yeah. Become a blood brother with , your best friend, you got

115:31 little scars makes you really easy to , but that's how they did

115:36 OK. So here, uh let's , instead of the, the amplitude

115:45 , let's take the phase and compute cosine of phase. And what that

115:50 is it equalizes everything and it be it in a gray scale. It

115:54 it really not really easy. It's tedious, but it's easier to see

116:00 the terminations. You see the weak and the strong terminations. So you'll

116:05 those folks who do that use this quite a bit, then we can

116:11 things. So you might call this meta attribute. I would prefer to

116:16 it uh with color instead of but it's OK. And this is

116:22 that made it into the into the uh was originally developed at Texaco and

116:29 called it sweetness. OK? And they called it bitterness, nobody want

116:34 use it, right. Yeah. sweetness. Oh These are the sweet

116:39 because they recognized in the Gulf of and offshore um uh West uh Northwest

116:49 that if I had a sand channel in a shale, well, the

116:53 channel gave a stronger reflection. It be a negative amplitude but a stronger

117:00 . So high envelope and it expressed it because it was more homogeneous.

117:07 didn't have the higher frequencies in So it was also a lower

117:12 So let's put the strong amplitude in though lower uh frequency in the denominator

117:21 call it sweetness. And then they a square root in there just for

117:25 you know, just what they felt good. OK. So you'll see

117:31 I think in picture. All OK. So instantaneous attributes provide a

117:38 but very fast estimate of envelope phase frequency of sic reflection. They degenerate

117:44 multiple reflections interfere with each other. , remember the little spikes and the

117:54 frequency. So some good friends of here in the city using machine

118:06 they'll put these instantaneous attributes in for survey like the Eagle Ford. And

118:12 they'll put an instantaneous frequency in uh and other things phase and then they'll

118:19 , oh look, I now have millisecond resolution because of uh artificial

118:26 machine learning. No, what they is they have some attribute that's got

118:33 in it where you're interfering. So not giving you better resolution. It's

118:39 you where the edge is. when you start working with var,

118:44 , you're working with variants. So is plotted the variant and you'll notice

118:48 you look at it carefully, those edges are one vel thin.

118:55 they're 25 m. OK? They're vel thin. It's not smeared,

119:00 pretty sharp. So well, hold . What about resolution? It may

119:07 one vel thin but guess what? could be 75 m to one side

119:13 75 m to the other side, don't really know where those data

119:18 OK. So you think of if did a physics class and might have

119:23 about Fornell zones and limits of resolution so forth? So there's a uh

119:30 difference between what the, what the ? OK. Good example. Mm

119:44 test madam Gis, right? So something profound. So that Stephanie is

119:55 . OK? Don't, don't oh don't say I there's something profound

120:01 satellite uh mapping with Gis about what the resolution between me and Bob and

120:14 where Bob and I are. you're both in the lab.

120:26 Triangulation? Well, they, they triangulation. So there's relative distances which

120:34 really, really good at. So when they say like 1 m 2

120:40 resolution, it can tell that Bob I are two or 3 m

120:45 But if it, if you asked where Bob and I are, it

120:50 know I'm in this room or it know I'm in this building.

120:54 That's absolute location. So you OK, we're always this far

120:58 But are we here or are we ? So we got that kind of

121:02 thing in there too. So when see the coherence is oh man,

121:06 fault is perfectly resolved. That looks . Yeah, but that fault may

121:11 be there. It's here. But those are the kind of trade

121:17 we have. So you look at giso talk, you, you homework

121:21 the weeks, you're gonna go look say, what's the, the relative

121:26 and the absolute. Now some of may be in a different class.

121:31 ever do surveying? OK. So surveying. We're really good with taking

121:38 tape measure and saying that, you , I'm 2015 ft from Haydn because

121:48 can measure it. But now if want to put us on a

121:51 well, then I've got to do these measurements until I find a benchmark

121:57 I know from many, many people tens and tens of to know where

122:04 benchmark is. What's my relationship or relationship to that benchmark? Those are

122:09 questions. OK. All right. response. Wait it out to be

122:16 general. Um, let's raise that gonna see everywhere. I'm, I

122:31 didn't say the effect but they, ones you're gonna see and then complex

122:36 can be used as auxiliary volumes and voxel interpretation to constrained auto pickers.

122:43 I would say, uh, not can it, but I would say

122:48 default, it's in all the auto today. So does, uh,

122:54 have any question? I don't think . Ok. Good, good.

123:02 see. I have to think of name too because I have a,

123:05 spouse's name is Stephanie and my granddaughter's is Stephanie and my daughter's name is

123:14 . So you can see how I confused and that, that's what am

123:17 thinking of them for? They're not this room? All right. Uh

123:25 I talked about this. That's Oh OK. So this is a

123:32 slide from earlier now, shaded I've got a horizon and here's my

123:41 coming in, here's the normal if angle of incidence equals the angle of

123:48 view, that is specular reflection. is what you're going to have in

123:53 mirror. So, cars, how you say mirror in a spec?

124:01 . So specular means mirror in, Latin. OK. So what you

124:05 is exactly what you get out of angle. And then from this

124:10 it's more of a diffuse reflection. I see the sun coming through,

124:18 a little. So I see that coming down. It's a little shinier

124:22 , but it, it's a little blurred. Maybe you guys can see

124:25 the light is coming down as So it's more diffused. I'm still

124:29 a reflection but it's more diffuse. fact, that's how I see the

124:34 brown. Like what's the color of mirror? Well, well, I

124:37 know. And you don't see the of the mirror, you just see

124:41 else. All right. So in uh the commercial software and uh I'd

124:47 they all do it very well. does a nice job. Um You're

124:52 look at non specular reflection. So gonna have to right the F secular

125:10 , very poorly documented as to what do in the code in patrol.

125:17 we get that far, you have have a horizon picked first a

125:21 Uh, the choices you get are . Ok. I understand that.

125:35 , plastic, I don't understand Woody, I guess that's like the

125:42 and they might have another one. they're using these real soft words or

125:46 equation are they using? I have idea. OK. But I think

125:51 know what a plasticky surface looks like what a woody surface like and a

125:55 surface looks so you can play with . OK. So here is uh

126:02 picked horizons. I picked the top this uh pro gradation surface. I

126:08 the face of it here at the of the surface and I am looking

126:16 it from north to south and then moved to school and pare and I

126:30 look at it a different night as, as a musician. I

126:35 also look at it at different angles second. Ah, that one,

126:43 what the tool looks like. You this guy. Uh And now I'm

126:48 play it and it's a system from Texas. So north central Texas,

126:56 got cars collapse in it, pick surface. So you can see the

127:01 cheese holes and you can see what did here or what I did.

127:08 just moved this mouse around first looking aim you then uh changing the incident

127:16 the white and what it really It's an interactive film. It's pretty

127:22 , you know, it's a whole of fun. Uh Definitely picking the

127:26 is not a lot of fun. part, you know, you,

127:29 spend two weeks and then you have five minutes of pleasure, but that's

127:38 . All right. So conventional interpretation . Um One of the first papers

127:42 3D interpretation from uh Reich and Gilford uh Shell identify the horizon of

127:50 OK. Usually your boss or your of team will say because of seismic

127:56 photography, we wanna look at a stand and want you to pick that

128:00 or we are in uh the Johnno's . We want you to pick the

128:05 shale formation there or maybe the one filled with channels, et cetera.

128:10 So there's typically gonna be some focus what you're interpreting. Then you're gonna

128:17 a horizon on a grid of every 10 or 20 lines in line

128:21 cross line. There's a method to . You're gonna start with the bad

128:28 and then you're gonna quickly realize, I better use a more systematic method

128:36 ties the lines as I pick. I don't have to re pick them

128:41 do you don't wanna do all the lines first? Because then the cross

128:48 , they're not gonna tie. So have to kind of draw squares and

128:54 to make sure those squares tie and up confidence if you got a salt

128:59 or in, in our case, got a die up here or not

129:02 volcano in the middle. See if can kind of go around the darn

129:06 , don't try to go across it there's nothing to pick in the

129:10 OK. So this is the kind thing you learn by doing. And

129:15 and I notice even here, some you guys have quite a bit of

129:19 . You're helping the others you learn . You learn from your friends,

129:23 office mates, et cetera. I , that's how you learn.

129:29 Then you're gonna, you're gonna have grid and then you're gonna fill in

129:33 blanks between, let's say every 20th and you're going to use an auto

129:39 for that. Thanks extract horizon So time structure, amplitude extractions,

129:48 magnitude, dip Asmus combined, dip dip Asmus interactive sun shading like I

129:54 showed you horizon based curvature, those of uh horizon based. I would

130:04 one other term on here and maybe , I'll stick it in now.

130:10 the next time I do a class this, I have it.

130:17 I would apply the data conditioning first you'll notice that lab five, which

130:25 a couple of you got, did get to lab five? Maybe?

130:31 . Maybe during a week, whatever five is simple data conditioning. Not

130:37 to do. It's just pushing you're gonna find out that it,

130:42 helps the data. It includes, increases the vertical resolution and it definitely

130:47 the continuity. And by increasing the , it's going to make the horizons

130:54 to pick. And by increasing the of terminations at faults is gonna make

131:02 faults easier to pick. So I say data conditioning is, is

131:11 So maybe let me, let me put that in here. So the

131:15 time I remember and D and Ok. Ok. I'll make that

132:01 different color because that's not from, him. Ok. Fact,

132:23 Oh, somebody from Texas is calling 832. I moved from Houston 18

132:32 ago. This is my daughter's old number. Have to use the

132:38 anything from Texas that I get. not a name that I know it's

132:45 trying to sell me something uh for car that I bought in Queer Lake

132:52 years ago. My, my, know that car that I sold 15

132:56 ago, its warranty has run I get that over 65. Uh

133:04 of the calls are about Medicare and , stuff like that. And somehow

133:09 people know about my compromised romantic capabilities they're trying to sell me stuff for

133:17 too. Anyhow. Having the phone sounds like, you know, this

133:26 gonna be Partridge is good. All . So here's an example from central

133:31 platform of West Texas time structure Uh simple piece wise uh kind of

133:39 red down to blue. So red shallow and blue is deep. There's

133:46 dude plotted against the gray scale. got a reverse fault here. Reverse

133:54 there. This happens to be a slip fault that happened to be a

133:57 swp fault happened to be cars over picking it was hard to pick

134:02 So you can see Mard bad picks uh 1520 years ago when I did

134:07 . OK. In this room. right then. Oh, come on

134:15 . OK. That's my better But she doesn't know uh I got

134:23 , put it on. Oh Come mute. OK. That was

134:40 one of my Stephanie. OK. as mute. OK. Going around

134:45 color wheel. That's what, that's I think of it. This is

134:50 it looks like in the software. is done using Geof frame and then

134:55 OK. So now uh a paper Bruce got it. Uh things

135:05 let's say a carbonate. I'm gonna it. The fractures are gonna be

135:11 intense where or in this place where flexure is greatest. So here's his

135:22 form. Here's his line a a and uh more modern we would say

135:27 at the time he just used it . So here's a survey from uh

135:34 Colorado and he picked three horizons. ? And now you see this like

135:44 pink guy here. OK. I a fault here. Got a fault

135:51 and then up here it looks So the area is on that uh

136:01 hand picture and even here as well I have discrete discontinuities. Is that

136:09 seismic noise problem or is it geology ? I haven't picked on you

136:20 Do you think it's seismic noise or ? I mean, here I have

136:23 resolution. More glad, I don't how to undo that. I have

136:31 lateral resolution deeper in the data than shallow. What? That doesn't make

136:38 sense? Ok. That doesn't make sense. So, what, what's

136:43 on here party? You think it's ? Good. So, you're a

136:53 , right? Can't have one Give me three hypotheses as to why

136:59 is every geologist has to have three for anything. None of which they

137:05 all conflict. That's fine. So me one that you might think is

137:17 . Have you done any structural geology ? No? OK. Well,

137:22 of them I've got, this is , maybe not clear. But to

137:27 it's clear this is a reverse So, oh, maybe I got

137:31 fault then fold structure. So I'm down, I'm falling down deep and

137:43 it's folding and then it's just simply . Ok. That, that's real

137:52 for tectonics, like in the rocky . Certainly in Colombia you're gonna have

137:56 ben folds everywhere um down deeper than have more brittle rocks. Maybe very

138:07 rich brittle rocks and a shower. have more shale in the system.

138:15 the, the brittle rocks are breaking discreet faults and the shells are just

138:24 smearing. They're more ductile. More plastic or I'd have a single

138:33 down deep and then a sway fault above maybe five or 10 little falls

138:41 the shallower part of the data like the yellow and the red horizon

138:45 And seismically, I can't resolve that m offset on each fault, but

138:51 can certainly resolve the 25 m offset the one fault. OK. So

138:58 , so its geological, which one the opposite is true for seismic,

139:03 tend to have more resolution up shallow less resolution down deep. And the

139:10 is our resolution is coming from the that we can look at the

139:16 So if I've got just think of common spread, I've got more angles

139:23 uh up shallow and near parallel angles deep. Now, we have,

139:31 fix that a little bit with seismic , but the migration aperture up shallow

139:37 gonna be 100% and the migration aperture deep, we may not have data

139:42 enough out to get a good So anyhow, so then what he

139:50 is done 20 years ago now, it's still a good paper and he's

139:55 dip magnitude to production. So he's high production fier production. Oh It's

140:05 this flexure and then along this flexure here were the best one.

140:12 the flexor intersect, how, why that be? OK. And then

140:21 I just moderate production. Not nothing write home about. OK. Um

140:31 an outcrop from uh Lao de And we got a nice fold.

140:42 . OK. I curvature as the of the radius for a circle that

140:52 not only tangent to the surface but . OK. So I can have

140:59 ones that are tangent, but this fits it. And then I'm gonna

141:04 a dipping plane. A sin co decline a flat point and they purpose

141:16 I'm plotting. OK. So here going to say it for a planar

141:21 . Even if it's dipping, the is zero for a sin coin,

141:25 gonna negative for an anti cliental feature is positive and for a flat plane

141:32 is zero. Here's the equation. , that looks hard. Let's think

141:39 it this way, I defined it one old radius of the circle that

141:44 fits it. Now think of a I go around and I've got an

141:52 of two pip and I go around I have an art plank or circumference

141:59 two pi R two P over two R one over R. Let's take

142:06 little arc measured in radiance and an W measured in meters, take the

142:13 over the arc, W that's OK. So D the D uh

142:22 now I got DS. Well, , here's my surface and they're going

142:27 and down think topography. OK. , I don't wanna know the curvature

142:33 the surface. I wanna know the in the X direction or the Y

142:37 . I wanna put it on a time. So the, I'm

142:42 first of all have to change the axis or variable to A X to

142:49 yeah, S to X. And am I gonna do that? I'm

142:53 use the chain roll. So I to have a DS DX in

142:57 OK. So I'm gonna go from something DS D theta DS, I'm

143:02 put a DS DX spot. Not to do then. Oh I gotta

143:09 D theta DXD. How do I that? So I'm gonna go ask

143:14 who's much younger than me who did not too long ago, which is

143:24 . OK. You remember the OK. So the dip data,

143:33 the arc tangent of the height over distance, right, opposite over

143:43 right? All right. OK. that's simple. Now, I know

143:47 that is. What is the derivative of the arc tangent? OK.

144:00 remembers that? Nobody remembers that. why we got Google. That's why

144:06 have all textbooks. So you look up and guess what? You,

144:10 all studied this in school in the . We're gonna have a one plus

144:16 , that's the slope square to the half power. OK. That's,

144:23 what the derivative of the arc canon . And then, well, we've

144:28 another power of one of that term the denominator from the chain rule.

144:33 then we're gonna get D squared, squared and the numerator. So what

144:38 wanna get across here is curvature is the second derivative of elevation. It's

144:46 this correction term. OK. So I have a curve, sure,

144:53 curvature of this guy is the same of this as of this, of

144:58 , it's rotationally in bearing it. . That's the dip of the

145:08 Well, here's a, I got couple of little cartoons in here and

145:13 one picture is uh in red is topography and in blue is the

145:21 OK? So hopefully this works. . So I'm gonna put a,

145:25 circle tangent to it but not tangent it. OK. So positive.

145:35 . And here it's gonna be the circle and now the circle is gonna

145:39 a little bigger. All right. now it's gonna change orientation. So

145:52 gonna go from anti clal to syn . OK. So it becomes negative

145:58 then if we go along, it'll OK, it's gonna get bigger.

146:01 a big circle, big circle, small curvature. And then clearly the

146:09 who made this movie will, he an interactive thing maybe in MATLAB and

146:13 skin is not very, very steady he does. OK. And then

146:18 positive again. All right. And . So football season, I got

146:25 kinds of notes about not being able park on campus or whenever it

146:31 Uh So we're gonna have you got football, I'm gonna have curvature along

146:38 , thanks, the tightest part of football and I'm gonna have one perpendicular

146:45 , along the long side of the . So we were in, in

146:48 dimensions, we're gonna have two not like that one outcrop picture I

146:53 you and then we're gonna have an of the maximum and minimum curvature.

147:00 . So here's AAA cartoon from Hama he drew a, an image like

147:08 here is, and I don't want to spend much time on this

147:13 Here's my positive curvature and I here's something called, this is the

147:17 derivative and it's called K positive. , that's the um the crest of

147:29 topographic feature. But the hinge line is gonna bring into uh fractures is

147:36 be the most positive principle curvature. it's gonna be called K one and

147:42 hinge line of the most s inclined , the tightest negative curvature is going

147:49 be here. But the one that associated with the lowest part of the

147:56 actually has less curvature, it's less , it's less strained. OK.

148:02 we got a bunch of curvatures out . Um We have most positive principle

148:09 most negative. And this is what gonna use almost exclusively in this

148:15 Um There are others out there, mean minimum curvature, maximum curvature.

148:22 might show you curved ness which is sum of the squares of the two

148:27 . And yep, that's it. . So this is most bi most

148:38 one is biased towards and forms, other is biased towards scent forms.

148:43 is useful in machine learning classification. just wanna know what part of the

148:57 . Yeah, I mean mathematically good . But other than that these guys

149:05 , are less useful and cause too confusion because half of the literature is

149:11 with positive curvature. The maximum curvature you have a pencil. Good,

149:32 . OK. Just hold it, it. Here's my curved surface on

149:39 horizontal plane which direction shows the most of the structure you're showing up and

149:50 . No, but I mean in plane. So I want you to

149:52 like this way or that way. area W OK. She's saying this

149:58 that mathematically is the first eigenvector, eigenvectors and eigenvalues like when you're

150:10 Why? How am I ever gonna this? I never gonna use eigenvectors

150:13 eigenvalues. Why do I need to that? That was me.

150:17 That was me use eigenvectors and eigenvalues the time. But anyhow, that's

150:23 first eigenvector. What do you need know about an eigenvector is what it's

150:26 to measure, it's trying to measure direction best represents. In this

150:35 the most change in depth and it's way. So the maximum eigenvector is

150:43 have a negative side. OK? direction shows the least change in de

150:49 be parallel fact though, having a change, that's going to be the

150:56 curvature. Now, I got an , maximum curvature, minimum curvature.

151:02 ? So it's mathematically defined. Now say, oh, I'm a

151:06 Well, maximum's gotta be bigger than , right? So let's forget about

151:13 minimum curvature because it's hopelessly messed up half of the software. One

151:19 half of the software, the other , half of the publications, one

151:22 half of the publications, the other within the publication by Andy Roberts.

151:26 showed you a picture yesterday. I it was the first paper on horizon

151:30 curvature. Great paper. His figures curvature like eigenvectors and his text and

151:39 show curvature like a geophysicist would do . So in the same paper,

151:45 inconsistent. OK. Let's not do . OK? Just think, oh

151:52 a positive, you know, OK. Now, so here's the

151:58 of confusion, but I just captured and I'm gonna use a K one

152:06 the most positive principal curvature. K , the most negative principle curvature uh

152:13 . Why? Because they have eigenvalues eigenvectors or principal components if you

152:18 So K one is always gonna be than K two. Mhm.

152:23 But here he stop. Risk and ball stopped and you got the

152:47 We've got a school of differential Yeah. OK. I gotta update

152:57 do too. OK? Curvature picked outcrop in Wyoming in the US rocky

153:08 . So this fellow we, one the famous theologist of 19 nineties.

153:13 went out there, he liked his and then he got a yardstick or

153:19 meter stick and he measured how many per meter. OK. And he

153:25 fractures per meter to curvature. So Gaussian curvature, so Gaussian curvature,

153:33 lived uh in the 18 sixties, the other traits. OK. So

153:40 lived in the era in the 18 and he uh a lot of

153:46 one of his contributions to what's geology metallurgy today is the theory of thin

153:53 . So he said, yeah, I got a thin plate like

153:57 yeah, I'm gonna have a little on the bottom of the arch.

154:01 have a little extension on the But yeah, the average strange about

154:09 same on the top for a thin , for thick point is different for

154:12 point. So I'm not gonna have lot of open fractures instead, let's

154:19 that as a thin plate. Now I've got curvature in both

154:25 Ah So he's gonna multiply K one K two. That's what he

154:30 And uh you know, and that's there's cool, there's nothing wrong

154:34 that. And so here are the , OK. In terms of uh

154:43 practice for neuter. Uh So hi of fractures on this side, here's

154:49 curvature, high curvature on that So good visual correlation. OK.

154:56 one with the P. So this like doing this. But OK,

155:04 comfortable with the idea of a parent , right? So the true dip

155:09 this direction and the parent dip uh in that direction, we have the

155:13 thing with Kish, the true We got two principal curvatures this one

155:20 this, but we could have an curvature at that angle uh named after

155:26 . OK. So it's called Oiler . And in Petrella might be called

155:32 curvature. I don't know. But , and uh so the, it

155:43 thought, sure, here's my curved , here's my playing. I've got

155:52 strike and a dip. What is curvature in the direction of the striped

155:57 and in the dip direction? So idea is, and it's not that

156:02 of an idea early and you're gonna it, is that the rocky mountains

156:11 under compression. So any of the that are parallel to the rocky

156:24 those fractures, they're gonna be a of fractures, they're gonna be

156:29 they're, they're gonna be closed. ? Because the rocky mountains are under

156:34 in contrast parallel to that, they're be relatively tensile. So, ah

156:40 fractures I'm interested in are gonna be to the uh the transfer faults that

156:50 the folks in front of the rocky . But, and here he's working

156:55 the, in the rocky mountains and a structural geologist so he doesn't know

156:58 he's doing and he's got eight wells they were, they were locations and

157:09 his curvature anomaly from the surface and well, one and well, two

157:15 they are excellent producers at this horizon they communicate to each other. So

157:22 the simple explanation? Oh, I a lot of natural fractures in that

157:27 . OK. That's what he There's another one, this is down

157:31 the Maga Jess Maga Ji's basin there Southern Argentina and another horizon based

157:44 So here's a P horizon. I a little grob in here, a

157:49 grab in here. Structure map are , blue and purple are beat.

157:59 here on this time structure map, don't know what the real row

158:05 a good magnitudes. Oh, that's . And then here is his maximum

158:16 . Now he's using curvature the way just said it should be displayed.

158:20 like I said, half of the are one way, half of them

158:23 the other. So where it's that means it's Syn Kinal and where

158:30 positive, it's anti clal. So , we've got a feature that's kinda

158:42 kinda like that. OK. That of thing. So anti clal on

158:48 outer edges. Sin clal on the edges. And here's what it looks

158:54 in the vertical seismic. OK. you can map stratigraphy as well.

159:01 this is the Soto Canyon in the of Mexico. Here's an amplitude

159:05 I see this fine uh a time map. It's OK. I see

159:12 levy levy because Park Park O La Lede, Pasco Leve, right?

159:23 it's raised, raised, raised up Le Matin. I get up in

159:28 morning, I raise myself, my brush themselves, right? That's French

159:35 . Uh OK. Um We can dip as mute dip magnitude.

159:44 here I see the edges of the on the magnitude curvature. Wow.

159:52 see all these reworked edges of the due to the uh currents at the

159:58 and then has one. He calls . He doesn't apply. OK.

160:04 here, see the edges, they these notches notch. So here in

160:14 , you're not gonna see many notches , but uh go someplace where you

160:20 a road cut. So drive to or drive to New Mexico and you

160:26 through a road cut and here's the road cut and it's level on the

160:31 , but there was a heavy rainstorm there's this like triangular notch and all

160:37 dirt comes down and the walk. . So we have the backwards version

160:42 that submarine things are going in the , not the canyon, but down

160:47 channel in the Turbid flood stage. have a high flow, it cuts

160:54 and comes out. Where are the is gonna be at the cut bank

161:01 ? Ok. So uh Henry Postman , this guy, he's like the

161:08 of seismic geomorphology. So I did , not. Yeah. Yeah.

161:27 . OK. What the thing was you moved horizons along that fault during

161:35 time. So we've got the different . We know the top of the

161:40 division was a one time flat. know the top of the Cambrian was

161:46 time flat. The top of the was one time flat. So we're

161:50 have different thickness on different sides of fault of a normal fault if you

161:58 in a deep voice, Synon OK. That means you have deposition

162:06 the fault is moving. OK? then you want to put these

162:10 But now darn it and my fault like this no big deal, but

162:16 fault is like that it's corrugated and parts are quartz rich and more

162:24 sandy sandstone and other more ductal So when things are rubbing against

162:32 it's gonna cause fractures. So what did is she did a fine element

162:37 and measured strain and where are the that are going to be under most

162:44 during the geologic past? And then the well controlled, she correlated them

162:49 high fractures cool. Um so called and geom Mehan properties here, I've

162:59 three geom Mehan units. And this , he's got uh I guess these

163:07 shales and then he's got sand. he's gonna call it a competent

163:11 All sand. This one is almost all shale and this one is

163:17 sand and shale. He's gonna call a mixed mechanical unit. And you

163:22 see here, I have doctoral deformation . I have quite simple.

163:32 because a competent unit and in this it's something in between and noticed different

163:39 changes. So everybody here, who's geologist? You probably did, did

163:47 build sandcastles? Like you ever try build a sandcastle underwater? Doesn't work

163:54 well. OK. So you've got internal friction coefficients. You might have

164:03 studied about more circle. OK? uh coefficients of friction and so

164:12 So different rocks are gonna have, gonna more circle will say that depending

164:17 , you know, like cool coefficient that a rock is gonna break

164:23 60 degrees or 80 degrees or 45 . You can figure out what that

164:29 of weakness is. All right. you can go back to your uh

164:34 textbooks, but that means the the shape of the fault or

164:42 or the, the dip of the will change depending on what I now

164:48 gonna move things along this stuff. , I can't, if I'm gonna

164:53 along there, I'm gonna have aosis, gap, aosis, you're

164:57 have holes in there. How am gonna accommodate those gaps fracture?

165:03 So this is what your geology your structural geology teammates bring to the

165:08 and put together and what, what do as interpreters. Well, we

165:14 that darn fall and sometimes darn I wanna make that fall straight because

165:21 my preconception of a nice clean fall sometimes it's not that way,

165:30 So here uh same guy and here got the different falls, high

165:40 the wave green, then just wait how you OK. Uh The magazine

165:53 still in bye that we talked I don't, here's his folk.

166:00 is the word he's using. We a couple. Her name clearly wasn't

166:25 . It was Yo Deli. Olo Yomi. Anyhow. Good,

166:33 Nigerian name. Yeah. And she studied here. Uh So she

166:39 the top and the base of this based of this formation. Here,

166:45 the top, here's the bottom and can see uh it's a little higher

166:50 . So it may be a little . There's an in size channel here

166:54 size channel there, inside channel that go give me uh a second snap

167:02 thick. The middle one, this little less thick and this one the

167:09 it was picked, we really don't this little incise there. That could

167:12 over here someplace. Now, uh my, my line OK? Everything

167:20 up. Now, what? So , my attribute is bottom line,

167:27 top, let's do R MS So the, but some of the

167:34 of the amplitude in that zone divided the thickness and here it what?

167:41 . I've got low R MS Ir MS on the sides, fairly

167:48 R MS here. And this one see in R MS. So notice

167:55 thick part of the channel has low MS amplitude and the sides have high

167:59 MS amplitude. So why is, is that Newton? Why is

168:15 Let's see if Jessica Jessica, you there? Yes. Yeah. So

168:22 , why do I have high arms on the flanks of the channel and

168:27 in the middle? Mm uh I know. OK. Anybody want to

168:37 a guess. Well, we're gonna a little bit of a levy on

168:43 side. So we'll have a little filled levy. It is filled,

168:50 charged with gas and the size channel was just filled with shale.

168:57 So one is mapping the levy and other is mapping the channel axis which

169:02 us to the next slide. So here she is mapping other sands

169:08 the Gulf of Mexico where we have salt tectonics. OK. So we've

169:14 salt tectonics. Offshore Brazil, North Sea. Lots of places,

169:20 ones and other places like in, Libya. And that, so what

169:25 is the salt doesn't really push its up. It's the basin is building

169:33 So the Mississippi River is dumping dumping sediments, dumping sediments. So

169:37 pushing down, pushing down, pushing , the salt layer is being squeezed

169:44 comes up where it can't. So the basin is building down and

169:50 as the salt comes up, the the the mini basins fill.

169:55 we're forever having the mini basins building and the salt coming up, changing

170:02 topography. So what happens? I these little bitty mini basins and then

170:08 spill into the next knee base and fill that and I spill.

170:14 That would be great if it stayed but nothing staying still. Everything is

170:17 around. So what did the geologist this bill and spill? Right?

170:27 cool, doesn't it? So, and Spill. So here are three

170:32 sections through the data kind of ugly but still. So here is just

170:41 , here's a thickness map. So thicker here and then thinner. And

170:46 here is her interpretation of um the where she's got distributer the main

170:54 et cetera. And then here is data on the right thickness and here

171:06 a uh research uh fish tank filled colored sand. OK. So Strat

171:13 like to do these things. the fish tanks could be oh 10

171:20 by 10 m, might be a 5 m by 5 m. I

171:23 they're big. OK? Then maybe high and you put sand and different

171:28 sand and you add it and see does it go. How does it

171:31 , et cetera? I'll show you pictures uh next week on that.

171:35 notice the morphology very, very OK. Another one. And I

171:47 we're gonna stop there and see if can do a quick practice quiz,

171:55 ? You wanna show him how to it? Not any history?

172:38 Oh. Mhm. Yeah. So uh repeat the answer when my mic

180:53 off, this is the, this test counts for absolutely nothing other

180:58 for you to see the style of questions I ask. OK.

181:05 you know, typically you're gonna have or four pictures to choose from.

181:12 found that when I used to do tests by and I would pick like

181:26 of the questions with the synthetic, would pick bad answers that people had

181:32 drawn. The most, most common answers is drawn from here. And

181:37 would say the reliability is almost exactly same as drawing by hand, just

181:43 lot easier to grade. And for of you guys who like quick response

181:47 find out how well or poorly you immediately, pardon? You said?

181:58 , so I didn't have to. you don't, you don't have a

182:03 out. It's better that it's Oh, yeah. Yeah, you

182:10 . That's right. Yeah. because sometimes when you're making,

182:13 uh, the 80th copy the ink and some people get a bad

182:20 especially for color. If you got big class, you get good

182:24 good quality. Yeah. Pardon? , officially it's over. If we

182:41 , I'll go to 555 we'll I'll go quickly over the answer.

182:47 , you know why? And, , makes sense. Oh, except

182:53 might have, hopefully I didn't turn computer off. I have, we

183:04 quick. In fact, I couldn't out how to log off. How

183:14 you log off? Yes, for plan. Yeah. Yeah. How

183:24 you do that? There's no power or anything you need to, you

183:33 name? Oh, I gotta click name. Oh, and then it

183:37 , logs me off. Oh, see. Ok, cool. I'm

183:40 right with that. I don't know , OK. Ready to go over

185:33 . You don't have to finish But, so we'll go over

185:35 Let's do the first one. And got uh I've got four images that

185:41 instantaneous face and, well, and one is the best one?

185:48 So we can rule out, remember phase at 180 is the same as

185:53 phase at minus 180. So we to have a cyclical color bar and

185:59 is a rainbow color bar going from to red and this is the blue

186:05 , red, uh dual polarity color . So neither of these two are

186:12 in the upper right and the upper , the lower right. One is

186:18 cyclical color bar. So this is same color here is down there and

186:22 same color here is down there. one's OK, but here the interpolation

186:28 on the default. Hopefully you did in a lab exercise today and you

186:32 , it's got all these little artifacts in patrol. It shows up

186:37 the zero maps, the green in page color bar. It's got all

186:43 little green stripes here between the blue the red. I turn it

186:49 All that goes away. OK? you wanna use the one up here

186:55 in the upper left. The second you haven't started picking. So maybe

187:01 isn't quite that you need to know can figure this out. So if

187:07 ask it next week, you'll but we've got auto pickers. So

187:12 wanna like, oh I'm gonna pick , drop, drop, peak,

187:15 , peak, zero, crossing zero . If you are picking an angular

187:20 conformity, you're gonna have different reflection I'm sorry, you're gonna have different

187:27 coming up in an angle to let's a constant impeding of the shale

187:33 So sometimes you'll have a positive sometimes you'll have a negative reflection.

187:39 if I have a standing formation that to have the same impedance as a

187:45 formation, seismic doesn't care, you're have zero reflection. OK? So

187:51 can't pick peaks and troughs. And same thing is true. And this

187:55 why, um, Stephanie here hates photography because you can't use an auto

188:01 . You gotta pick everything by hand everything is on lamp and awful labs

188:05 you can't pick peaks and drops So, uh, you have to

188:11 turn auto picking and auto, turn picking off and then pick the terminations

188:19 hand. I mean, that's all can do. And it's pretty

188:25 Pardon? It would be eve it, it would be number E

188:38 in Edward, turn off the auto CND you can't do. So that

188:45 be a zero crossing. CND would a zero crossing. Uh Yeah,

188:52 doesn't, it doesn't matter. It's the reflectors aren't continuous. I'm

188:58 the reflection coefficient is not continuous. if you were to look carefully

189:04 you say, oh, here I've maybe I'll call that positive, then

189:06 changes, then the positive again, positive, negative, positive it

189:13 OK. You'll get comfortable with that you start picking. OK. Now

189:20 one takes a little bit of skill it, it doesn't require any understanding

189:25 geophysics and understands, requires more of . OK. So my geology guys

189:33 gonna be comfortable with that. All . So we're gonna pick,

189:38 this one kind of goes up. all right. And then it continues

189:41 go down. What about that What about that phone? What about

189:45 phone? Oh, I went up I went up. Ok. This

189:49 goes down, down the toilet. . This one goes down the

189:56 This is like my petroleum engineers would and this one says, oh,

190:01 got district faults and this block number explain everything on the computer.

190:12 Yeah. Yeah. Yeah. Sorry Jessica. You're quiet.

190:18 So, so this one kind of down the toilet. This one follows

190:25 blue troughs that goes down the This one tries to go up the

190:31 but doesn't do a perf a consistent the faults first. That would be

190:40 best way. Then you don't poke eye out. So you would pick

190:44 falls and you would say, aha are sliding them, the foot

190:51 I'm this is the foot wall and is the hanging wall. So the

190:56 wall is gonna slide down on top the, I'm sorry, the hanging

191:02 , the slide down on top of foot wall. So this layer is

191:07 to go down with respect to the on the other side and that's going

191:14 be consistent along. So this, block has slid down. This block

191:21 swayed down. This block has slid . This block, I slid down

191:27 both sides. So maybe this is the pick is and then you got

191:32 block here and this block so they directions a bit on you. But

191:37 I'm picking the same red, red pattern and trying to match the

191:43 across the fault as best as I by eye. OK. So what

191:49 need to do is when I, I was talking about reading the

191:54 you wanna honor the seismic. So , I'm always gonna pick a trough

191:57 this example consistently, but it needs be geologically reasonable. OK. So

192:05 got to integrate the two together. . This one comes from the book

192:10 Don Herron. Well, couple of asked, should I buy a book

192:13 you're gonna buy a book? This the book to buy. It's a

192:16 book to read, easy. Everything it is worth knowing. OK?

192:20 superfluous information. And he's got this of using an auto picker and what's

192:27 auto picker doing? It's connecting peaks troughs and it's cross correlating and he

192:32 right across there and maybe at this , it looks reasonable. But I

192:37 this guy up here that's clearly dropped here. It's dropped down. So

192:45 understanding of what's happening above where everything dropped down below everything is dropped

192:52 This guy should correlate to this negative in white. OK? And if

193:01 just use the picker and you don't it to stop at fault, how

193:06 you do that? Oh, you pick the fault in that line?

193:10 . But you can pick it and erase it and then start it

193:13 OK? Perfectly permissible if you uh it by itself is gonna pick right

193:20 there. And if and variant right at that level where the red pick

193:25 the variance would be zero, it not see a fault. OK.

193:31 . This is the more and you to think of reflection coefficients. The

193:37 thing, what's the polarity of the ? So I think on the first

193:41 I gave you the top reflection and have the uh impedances there. So

193:47 your head or on a piece of , you multiply 2.2 times 3.2 and

193:53 you multiply two by three. that's six, I can do that

193:56 my head. And uh so if going from high impinges to low

194:01 I have a negative reflection coefficient. means my source wavelength is zero

194:08 It's got a at that. Now, well, that's bigger than

194:19 times three. So I could have OK, that's good about to

194:36 I happened to the right one, can see correct one on the

195:01 No, that's not going from going high. It's one. I,

195:18 , I mean, because I there's some I should give zero reflection

195:23 thanks. And it's a kind of but it's not expensive. Definitely ask

195:34 a question just like this. Maybe was like, OK, this one

195:40 what we uh covered maybe this year uh direct hydrocarbon indicators. So here's

195:48 horizon. It's from the paper by , which I recommend you take a

195:52 at, I'll pick a picture from that for sure. On uh

195:58 Friday. So it's getting brighter as go structurally higher. When you are

196:05 structurally higher, they're getting much structurally or much higher. A much stronger

196:12 . So these are, they're just , they're simplest kind of bright

196:17 right. So that's kind of the I don't want anybody to be

196:22 like, oh, this guy's got or five pictures to look at your

196:27 , man, that really stressed them . They didn't like. And when

196:31 did it by hand, they I've never used colored pencils before.

196:39 , think engineering. Ok. um, you've got my email pretty

196:45 to find, um, and, , send me a note if you

196:52 a problem and uh, send, , you tie a note if you

196:58 a, a problem as well. , especially if you're in on the

197:03 and you get stuck at some You know, you come in,

197:05 commute, you get stuck on the . I know Stephanie is probably gonna

197:10 right after church tomorrow and tell her . Yeah, baby is still

197:14 You need to take care of take care of her. Um,

197:20 just, just send me an email , um, I'll see you next

197:24 . Ok.

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