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00:00 Did it in class. You got grade for the quiz that had class

00:09 and three where we had to OK. I took a point off

00:14 class three was not as flat as wanted it to, to show,

00:18 emphasize. Unfortunately, it was not my notes the way I thought it

00:25 , it's in the notes. It's the class that I'm giving today.

00:31 classes I gave this, I gave lecture and then gave him the quiz

00:37 again. But you were, you have benefits of this lecture. So

00:42 gave everybody a point for the class , flattening that I took off

00:48 So give it that, that makes a plus so far. OK.

00:55 . Ready. Oh, yeah. . Is there any questions you might

01:00 ? Right? Is that a somebody OK. Ready. And any

01:09 participation questions in here? Oh, got uh everybody in the audience.

01:19 . I have seven here but I have six. Yeah, but they

01:28 giving Stephanie, she won't be So is that the only person we

01:34 missing then Stephanie in here? I think he's, he's gone to

01:44 day. Yeah, because they asked the quizzes beforehand. Ok.

01:50 uh, let's see how disastrous I be in trying to get this slide

01:58 . Huh? We're gonna try. , ok. Let me see,

02:34 , back to the Zoom and I to go to share it, share

02:39 screen. So. Oh, I see. Ok. Can you

02:48 the slides out there in Wonderland? . OK. Classification of Avion anomalies

03:12 19 seventies, we had a technology bright spots. Does that relate to

03:16 VO are common midpoint gathers necessary for spot regimes? Should we request asses

03:25 to depth for new seismic acquisition is easy to determine for a particular A

03:34 class. Oh We're skipping over 35 that's the same as 23. It

03:47 uh I wanted to have the amplitudes both places and I did not give

03:56 section either. I skipped over it . Uh 35 is a lot of

04:03 and as I said, just showing equations for the anisotropy. Basically just

04:10 of it this way. When you anisotropy, you have different equations for

04:14 A bo it means that whatever angle shooting. If you're shooting, if

04:21 reflection angle changes, then so does amplitude that no longer obeys Zage,

04:30 obeys it halfway and you have to another term to the equation. And

04:36 if the asthma enters in it In words, if you're source and receiver

04:42 both in a north plain, a south plain, that's gonna be different

04:49 if your source and receiver are in east west plane vertical plane. So

04:56 adds another term to the reflection And it introduces 2 to 4 more

05:07 besides velocities. WW. When you done it, it, it,

05:13 all the anisotropy, there is nine you have right now. we think

05:21 P wave velocity, shear wave velocity density as the parameters that describe the

05:28 . But when you put in a M, you have to have two

05:32 wave velocities, two shear wave It adds up to be nine different

05:39 and only a few people really work that because the processing is exceptionally difficult

05:53 it's also very noisy. You have have exceptionally good quality data where you

06:01 it. It's usually the poorest data might need it in Saudi Arabia or

06:07 like that. And you got the seismic data you can imagine West Texas

06:11 it badly and they have awful seismic because up shallow in West Texas,

06:19 have the castile evaporates and then they into a really soft section and because

06:27 that large velocity inversion of shallow, got noise coming everywhere. OK.

06:37 look at a VO cla classification just show you that I like to be

06:44 hoarder of all things. This is book that was given everybody in 1973

06:53 was held at Exxon's Auditorium and it's lithology and direct detection of hydrocarbons using

07:02 methods. 1973. Well, this also called the Bright Spot here.

07:11 the DD I direct detection indicator. was at Mobile and in 1969 this

07:22 came to Mobile and I don't know exactly at Mobile did it uh brought

07:28 over, but shell said they had in the 19 sixties, 1966 they

07:35 using it. It's a pretty significant basically what it is in the Gulf

07:46 Mexico. Let's take there when you're for gas reserves, you get a

07:52 big high amplitude. I mean, , it's gonna rip right through your

07:56 section. That was the bright spot so bright spots became synonymous with gas

08:06 . I was at Mobile and so had it for about three years and

08:14 thought, well, I'll go to symposium but I know everything. All

08:19 . I mean, we have one of the first ones and I

08:24 to the symposium and lo and I thought we were above most of

08:29 folks surely in the United States. we found out that Russia had done

08:37 years before us, there were seven that were translated, there's six of

08:45 and it shows that they had to it at least five or six years

08:50 these published papers. And us, published anything yet. Then I got

08:56 thinking, yeah, but we have called four D. You ever hear

09:02 expression four D, four D means , you go out and shoot a

09:08 survey. You're successful, you get big field and it's big and

09:15 you start training it. Then after six years you wanna know,

09:22 how much is left in there. you shoot another 3d survey and you

09:30 your current 3D to the previous which was your baseline that's called four

09:38 because you had that. So, I, I thought us was the

09:43 one to do that. And in was a Russian paper in his

09:48 how they used it every year, they did as they had salt dos

09:55 they filled the salt domes full of during the summer. And then during

10:00 winter, they go ahead and drain salt domes to use as, as

10:06 as they needed. In about they would shoot a two D line

10:13 the Saldo to see what was the of the gas remaining in the sal

10:19 . And so every year they did . And I thought my gosh,

10:23 pure application of four D, it was a two D series but

10:30 a beautiful application way before the United . So Russia had a lot,

10:37 brilliant technology. They just didn't have equipment to go along with it

10:43 to give you an idea. Has been here of logging? Logging a

10:48 , is everybody ever been associated with ? Any mud loggers in the group

10:54 , somebody collects samples. One of problems that Russia had for a long

11:01 is determining the stretch that was on cable that they put into the

11:07 If they have something that's 4 m , that's a big damn cable.

11:12 gonna stretch the wire. How much it stretch? Well, it could

11:17 30 ft, you know, something that. Well, you're, if

11:22 trying to predict what depths the drill that, you gotta know close to

11:28 plus run is 30 ft. So is where something can be that you

11:33 believe, to make sure they didn't a target. They cleared the,

11:39 , sometimes the whole, well, would core, that's what Hungary did

11:44 years because the Russian technology was in . But computer room, their computer

11:53 were terrible compared to what United States in very small counties. But the

11:59 were educated beyond. Ok. Enough Great Russia. Here's the birth of

12:05 bright spot here. You see a section and they have on it,

12:10 called an automatic gain control, a where they bring in the seismic duration

12:16 try to make the amplitude average over certain window the same, take the

12:22 MS value and just keep on making . So every window has the same

12:27 this is what you get with a automatic gain control. Now you take

12:33 off and you process the seismic you get this. Now, where

12:38 you drill? Well, obviously this where you would drill. It

12:45 Now companies, when they recorded when he first started analog, they

12:52 an automatic gain control. Remember all had is paper records. They didn't

12:58 have tape. So what they put that paper record and it was a

13:04 record. These had a light beam across it and that's all how you

13:08 your seismic trace. They had eight beams going across wiggling as the electricity

13:16 in. So they had to have A GC auto game control. Then

13:23 start getting tapes, magnetic tapes, digital, still a animal. They

13:31 what they call program game. they could predict the gain that they

13:35 on there. OK. Enough of . So what was the technology?

13:44 spot technology, hydrocarbon indicators, We call them Hcis hydrocarbon HC indicator

13:53 brought the technology direct detection indicators. I and those of us who uh

14:00 had had the bright spot thesis oh, this is just the BS

14:05 . OK. I saw one Yeah. All right. Leave it

14:18 that. And to an extent it the presence of gas and to a

14:23 extent oil, oil with a high , oil ratio will change the reflection

14:30 significantly how the carbon indicators are lateral vertical changes in reflection continuity. There

14:40 auxiliary measurements or observations that indicate the or absence of hydro drugs. They're

14:48 only they're not absolute proof significant when several indicators are present. So for

14:58 , if you got a bright spot your seismic data, how about the

15:03 beneath it? Should they be a dimmer? And what if you had

15:07 flat reflection, you know, it's all over the place and you get

15:12 bright spot above it. Why is bright spot? Oh The velocity got

15:16 because you put gas instead of But what would that do? It

15:21 the reflectors beneath it down a little ? So you see a little

15:26 a little, I should say a , a little small section that became

15:33 down underneath. Here's the bright If you look at this right

15:43 that's something you could see. it's an anomaly. That's an

15:49 Now, if you come up here put your nose to the screen and

15:53 look sideways down the screen, you see that right here pretty flat.

16:02 fact, this, this almost intersects top. So there are two

16:09 two peaks, 12 and the bottom tends to come across an intersect way

16:18 here. This bottom limb is a face. It's a gas to water

16:28 . It's not a boundary from sand shale. It's a fluid upon fluid

16:33 is a big seismic indicator. Also hydrocarbons. It says you got a

16:40 surface. Why do you got a surface? Because gas and water have

16:45 different density gravity will make them settle to one flat surface. Gas above

16:52 below water below one or the Notice right underneath here, this right

17:01 there is the double depositional model. in the Gulf of Mexico. Anybody

17:11 cinema in college here, anybody took sections? Nobody, Tessa can I

17:19 you? We, we keep we keep our face on so we

17:25 sure everybody's still awake. See if , I have to scream and we

17:31 it likewise. Also, please. you. Has anybody taken cinema

17:38 Tessa has, she's Tessa has taken the courses in college. You know

17:43 the only anyone, everybody else is hide their face because they don't wanna

17:47 asked. OK. What is the depositional model and sediment sema? Isn't

17:53 one where if you have a gas , you always have another sand just

17:57 the, the same size. It's double depositional model. You always have

18:03 G in it. Didn't you ever that or is this another one of

18:10 black magic tricks that Fred's played? think it's a black magic trick then

18:17 is this? Because you see this and over again from the seismic data

18:22 the 19 sixties and 19 seventies. it is? It's a function of

18:31 air gun going off and leaving a , an air gun when it is

18:42 as a big pulse and then the starts to grow and then the bubble

18:51 and there's another pulse, the distance the original explosion to where the bubble

18:58 up and collapses. That's a function how much pressure you have in the

19:04 . When the air gun goes it's a function of how deep the

19:08 gun is, is flowing. How they get rid of it?

19:15 this has 200 cubic inches in but they also have another air gun

19:22 goes off and it only has 50 inches. So its bubble does not

19:30 in at the same time, but original shot comes in at the same

19:35 . And when you add all those guns together, it kind of gets

19:39 of the bubble right here. that was a later type of

19:47 various size of chambers. So the come in differently and you know,

19:53 20 air guns maybe being out That's a lot of air guns.

19:58 originally those air guns were very expensive only one person had them bull and

20:04 charged an arm and a leg and sued you in court if you try

20:09 make, make any. They also , I think I showed you one

20:17 cages where you could explode gas inside metal cage. And it would have

20:25 bubble as the explosions going off. the cage, which had a lot

20:30 holes in it who let the air but dispersed it. So it never

20:36 a bubble. And that was one . But at the same time,

20:41 heard many stories about the cage, get away from the, the Gulf

20:46 Mexico going across, say the Atlantic their site and all of a sudden

20:52 can't get any reflections, the amount energy just seemed to decrease. What

20:58 they do? They said bring that gun, bring that cage back,

21:03 it on board the ship, take cage off, just explode it.

21:06 leave it live with the bubble. gotta have some energy out there and

21:11 of a sudden you get reflections but get the bubble when you see the

21:16 down here, look up here. right there. There's another bubble a

21:21 smaller though, have to, that's bright spots you would notice that.

21:27 when you're interpreting the data, then of a sudden they find out

21:33 there were bright spots where they were to come. Here's a well that

21:38 driven and the amplitude decreases. What that? That's a carbonate play and

21:44 get fractured and the velocity get gets little lower and all of a sudden

21:50 velocity between slow here to the fast gets even slower. So you don't

21:58 as big as a plus reflection. decreases here. That was the

22:04 And then there were, there were areas where I'm thankful that the author

22:11 I copied this from, put a around this because if you look very

22:17 , you'll see the peak just above rib goes into a trough over

22:26 It's a phase reversal where here's the response and here's the gas, this

22:35 called the phase reversal. And then course, this is a beautiful one

22:39 had to put in literature. It a gas signature and you can see

22:46 interface between gas above and water below look how comes straight over and where

22:53 stops. That's kind of where the amplitude stops also. Now, that

23:05 1973. And in that discussion, was a gentleman by the name of

23:14 forget is his name Paige. page showed these two sections and he

23:24 , why? And basically it was the audience, why is it that

23:30 noticed on my far offset sections, can see the gas a lot better

23:37 I can on my near offset. never gave an answer that related

23:45 Yes, he related it to, , there's a bigger array effect and

23:51 smoothing the response more on the far and that's why the amplitude decayed.

23:57 it really was the first I can in literature showing a vo that on

24:03 far offsets big angles of incidents, gonna get a writer's amplitude. So

24:19 seventies that was the bright spot And geophysicists always like to be quantitative

24:29 here's the way they went ahead and , categorized and classified their amplitude

24:37 This is an axis or plus as . This is the normal incidence,

24:42 dash line that doesn't divide us into quadrants, that dash line. It's

24:49 to show you this is zero We'll start up at the top when

24:56 blue, that indicates a water When you have paint, the gas

25:03 the size of it indicates the So we start off with a limestone

25:13 it has a fast velocity compared to shell right up. So when you

25:20 a little bit of gas in, a limestone velocity decreases. But it's

25:27 when you have shell over limestone, if you put gas in this right

25:34 , this acoustic competes is still gonna greater than this shield. So your

25:39 decreases, but it's still a plus . So we're above zero. It's

25:44 plus ample. Then I'm gonna get here at the bottom and then we'll

25:48 the middle. Then there's the bright . You have a plastic rock and

25:54 might be positive when you're wet, might be slightly negative when you're

26:02 Brine Phil. But you add gas kazoo, your amplitude goes way down

26:10 becomes bright, unconsolidated sands. When put gas in them, you really

26:17 their velocity depending upon, of your depth as we learned.

26:24 there's those that you put gas in , it's positive it becomes negative or

26:34 could be slightly positive. You put in it, it's still negative,

26:39 it isn't a bright spot. It very far on the far traces.

26:44 gets a high amplitude. So we're have to take a look at those

26:49 the high amplitude is a negative I got, I had a question

26:56 that. Uh Can you go back a second? So yeah, I

27:02 a little confused by this. I this is from your your paper and

27:07 was confused based off of this compared Rutherford's paper where I thought he was

27:14 the dim out was when a phase happens because basically you have the positive

27:22 that get erased by the negative amplitudes you have the phase reversal and you

27:28 it is it might thinking about right? Or good, good point

27:34 , good point. This is the normal incidents. Ah So yeah,

27:40 not shifting in incidents, you Yeah, you see on we had

27:51 but here we had the angle theta talking about only on this axis right

27:59 normal. So you start positive, can go like this. That's Rutherford

28:05 Williams, this is the negative the reversal. But ours, if I

28:12 , if I become gas charged, gonna move down, right?

28:18 Yeah. So incidence isn't changing at . It's just the fluid that is

28:22 , it's just the fluid right Yes. OK. Thank you.

28:26 question. So that was the 19 class that was a 1970 classification.

28:35 come to the 19 nineties and here the Rutherford Williams paper and in

28:42 they showed class one, class two class three. Class one. They

28:49 with a high impede in the When they put gas in it,

28:54 went toward negative plus two. Your incidence is right around zero small amplitude

29:05 it decreases also when you put gas it. In class three, it

29:12 a big negative on the normal incidence it decreases also when you add gas

29:20 it. Now, one of the that was kind of uh interesting uh

29:29 , Steve Rutherford uh was a well use in Geophysical Society and he actually

29:36 , I didn't call that class He said, I told, I

29:40 , and this is section one of paper. This is section two of

29:43 paper. This is section three. blames that on me now. But

29:49 will stick with in class 12 of ex excellent paper. I loved

29:54 No, this is great. And see on the x axis it has

30:01 angle except once again, geophysicists are . They don't tell you what is

30:10 wet response. What if the wet lied right on top of the gas

30:17 wouldn't give you any help. So always wanna know what happens. Oh

30:22 four also by uh Ag and So here are classes 12 and

30:37 Mm. And this time I have it's wet and also when it's gas

30:47 , wet and gas charge for class . And finally class three.

30:55 it's a little bit too much is here. So let's only go out

31:00 about 30 degrees and summer right around . This is where offset between the

31:08 and receiver equals depth. So let's that back like that and analyze

31:17 And this right here is gonna be the quiz. I could tell you

31:25 it's look at class 12 and The black is class one. The

31:34 curve is gas, the lower excuse me, the upper curve is

31:40 . The lower curve is gas on these. You always go lower

31:48 No, remember the word amplitude means or minus magnitude is plus. So

32:00 said when you go from what? high to carbon charge, you always

32:07 more negative amplitude. Good quiz But magnitude might change magnitude might increase

32:19 offset when you add gas because we going always downward on this chart.

32:34 do you notice that's different between all ? Tell me something that is

32:41 that shit different but obvious. There's lot of things in here that's very

32:48 . The first thing you, you had, you had an experience

32:55 this when I gave you a wet and gas. And I told you

33:02 the simple Avio equation and compute the is four or five offsets every five

33:11 10 degrees and draw, draw the and you did that day one.

33:16 , and what did you get? , here's what I found out,

33:20 , I found out the wet response always above the gas. Yeah.

33:26 else did you see? Oh, zero, right around a normal

33:31 It's a flat curve on everything. coefficient doesn't change quickly around theta equals

33:39 . That means something. I when you're analyzing the data, oh

33:46 gosh, the wet and a they have parallel shapes. I bet

33:54 gonna be worth 10 points on the . I bet it is too because

34:00 about it if I gave you the shape for what? Listen carefully.

34:08 gave you the A O shape for and I says now here's the gas

34:14 but I don't give you a of . I just give you the normal

34:18 value. All of a sudden you draw the A vo for the gas

34:25 . Why? Because it's same as we, you just have to shift

34:29 down. That's very important cause a of times you don't have a,

34:37 lot of information, especially if you out to evaluate a prospect and somebody

34:43 showing you something, you can quickly at that as curs see if they're

34:49 and if they're not, something's wrong , what you're trying to tell me

34:55 not correct. This is not a prospect. Well, the first thing

35:00 gonna see is this, the gas is the same as the wet,

35:06 it's more negative. The difference between gas and the wet. See that

35:16 right there. Now, look at same difference between the blue, the

35:23 between the wet at the top and gas at the bottom. It's bigger

35:29 class two. Then class one, you get to class three. That's

35:35 biggest. So you have more separation wet and gas as you go from

35:42 one to class three. What does tell you? I don't like class

35:47 . It's gonna be hard to see class three is gonna be easy to

35:51 because there's a big difference between wet gas makes it easy to see.

36:00 , that's nice. The A VO becomes flatter from class 1 to

36:08 So class one up here, you're dipping but look down here at class

36:15 , you're kind of flat sitting in . Ok, let me, let

36:21 write this down. I add three to somebody's great. I add three

36:31 right now. You make sure I it all you gotta tell me is

36:37 all the curves in class three flatter nose in class one. Who wants

36:44 get three points. Raise your Oh, we got somebody's hand up

36:59 in the audience. Can you see ? No, we don't have anybody's

37:05 . I just said that to get excited. Sometimes somebody of the audience

37:11 raised their hand. OK. Not going for three. I got

37:22 operating and they were going through, through going number. Oh, take

37:24 for four. Anybody want to go four. Anybody want four points.

37:27 want to challenge it. Four points I go five. What if I

37:30 give you an a no, I'm gonna do that. Anybody want to

37:35 it. Newton says he's gonna try and he says the hell, I

37:40 I didn't say that. Ok, can offer some suggestion. Anybody.

37:50 . Let me lead a little Then which one of these has the

37:58 velocity? Which one of these 12 or three involve larger velocities plus

38:10 class? That's good. Class Uh I said three. So maybe

38:16 was wrong. That's OK. I one. Why? Why?

38:25 let's, let's think about it. during the rock physics, I said

38:31 you had a class, if you a rock that's around 8000 ft per

38:38 and you put gas in it, velocity drops. That was during the

38:44 an experiment, we said you add little bit of gas to unconsolidated rock

38:51 drops. But if you have a 18,000 ft per second and you had

38:55 to it, it just a, a little bit of draw, just

38:58 little bit. So the harder, consolidated the rock, the less it

39:06 on the poor float to change its . Consolidated hard rocks. They changed

39:14 velocity due to porosity fractures. It's unconsolidated rock that depends heavily on what's

39:23 the pores. So, up here class one, we have the consolidated

39:31 and they're a high velocity. Why is this dipping more? What

39:45 the dip? Well, Fred, a dip. So you ought to

39:49 everything. OK. I'll think of Reinhard Borel. Good old Reinhardt.

39:58 sat and we talked about him a bit and say what is so significant

40:04 Reinhardt's proxim Reinhardt? When you looked his approximation in amplitude section, his

40:13 term concerned fluids and only responded to . However, when we looked at

40:22 , the second term, it only to sheer away velocity. It says

40:29 larger the sheer wave velocity difference, larger the sheer wave velocity difference,

40:37 more you're going to change, the offset, the more that second term

40:41 gonna add. Now, what was sheer wave velocity of the shallow

40:49 Remember when we start looking at we said, hm, look at

40:55 , this sh this class three. we're looking at it, I said

41:01 looks like a fluid. It reacts a fluid, it has a low

41:07 wave velocity. There's not a large . So Don here we said those

41:15 , they act like a fluid, rocks do they have a low shear

41:21 velocity and therefore the differences in the wave blasi are gonna be small and

41:28 gonna have a flat curve. So have the high acoustic appearances below acoustic

41:38 on our curve ra where they fall flu discrimination resides in the normal

41:49 normal incident difference. Why do I that? How much is this upper

41:57 different from the lower curve? So I gave you the slope at any

42:05 towards you, just a slope, example, but the slope itself,

42:11 said you couldn't tell me if if it's a what or guess the

42:16 are the same. So that means slope doesn't give you, it's this

42:22 right up here where it's attached to normal in instances that tells us if

42:28 gas or if it's wet, that's big discriminator right there. The largest

42:37 that you're gonna get is on a three and I should say magnitude.

42:45 class three or two. What has largest magnitude? Uh which absolute value

42:55 gonna be the largest? It's gonna way out here for class two.

43:00 you're in an area that's class You see a big amplitude on the

43:05 offsets a big magnitude. I think most likely a hydro crop like that

43:13 here. You gonna say, oh , I'm gonna look for the slope

43:21 right here now. Oh, you're look at the difference between this and

43:28 fact is last night you remember that you read Michelle called stacked. That

43:35 one of the outputs that they They said look at the stack

43:40 That'll tell you what the fluid content . If you're in a class three

43:47 . How do we tell that? the interval? A lawsuit? I'll

43:51 you the range and I'll tell you you're in class three, here's the

44:00 . I, I have a quick going back to that last one.

44:07 class three, it looks like the and gas curves are not parallel.

44:14 that the case? Uh piggy picky? Yes. OK. But

44:19 , it's, they're not far OK. It's, if I,

44:24 you drew this, this is 2.6 that's three, you know that

44:31 you're not gonna really see it on data because you're within the air

44:36 Uh But see up here, there a big difference. Well, it's

44:42 related, always related to what happens the near trace. You're looking at

44:50 common midpoint gather and you're gonna see bright amplitude and this bright one not

44:57 , but you're not really. Oh , I got a big slope

45:01 A change it. No, you're big. You're big. But right

45:07 , that big is big because you're it against the trace that is at

45:11 offset and it's five times bigger. , that's what your eye sees

45:18 I look. Oh, I'm 4% . Uh That just doesn't click to

45:24 eye. All right. No, , thanks. Yeah, that's a

45:28 question about this. So you mentioned here uh but and is controlled by

45:39 source, right? So this, you say amplitude and if I tell

45:50 this, you're not gonna hold it be arrogant over anybody else now because

45:54 know more than they do. Just tease it, you can correct

46:00 . But when you say amplitude, means plus and minus exist, you

46:07 have a minus two and the plus , that's an amplitude difference. But

46:13 is the absolute value mag magnitude is an absolute value. So when you

46:23 you have a big magnitude on the of your data, it could be

46:28 negative reflection or it could be a reflection. But when you say a

46:33 amplitude, you're normally talking about a reflection, you're talking about being done

46:41 in a gas zone. OK? is the source energy, right?

46:51 OK, your amplitude comes from OK? It also comes from all

47:02 attenuation has to go through to reduce amplitude or magnitude amplitude is just a

47:18 that doesn't have to be related to . It could be an oscillation.

47:27 When you say that's a big that wave has a large amplitude,

47:34 actually you're going between trough and That's a magnitude. The amplitude would

47:44 . If you say that's a big , you don't say that in the

47:48 because you, you don't know where zero line is. But here on

47:54 data, we know where the zero is. You see this right

48:05 That's a big magnitude. Big Both. I mean that it's most

48:16 two oh OK. Over here, a plus value. That's a big

48:37 etude. That's a big magnitude over . You have a big magnitude but

48:50 smallest amplitude, that's the smallest amplitude you have because it's minus 0.3.

49:03 is only minus point 01, something that. If it is negative,

49:15 red lines are 1020 30 40 50 degrees. OK? Because why do

49:28 have notches in those angles? If have a velocity of 10 here and

49:40 velocity of seven here you come to boundary and you Google in like this

49:48 art like that. So the angle is 20. The angle here in

49:58 low velocity is five. If I back the angle here, what's it

50:14 ? Your angle was 20. But you get in the middle, it's

50:19 this right here, this right That's 0 1020. This is only

50:30 . The actual seismic you see the that you get right here is a

50:38 1020 30 degrees, 30 degrees is the heck out there on that

50:52 This trace in here above you might 30 degrees. This is only gonna

50:59 15 degrees. These are contour lines what they are. Oh my

51:14 Uh, you missed your break. go ahead. Take a break,

51:18 . About 10 minutes. I got minutes after nine. Let's come back

51:23 25 minutes. Jo 10 those of that are in the same time

51:39 you probably didn't hear that because well, that's hard to see.

51:56 . It's time to start again. . I thought for sure Taylor was

52:08 to quiz me again and say you it wrong again. Fred.

52:12 I hate to have to correct you the time. Fred. OK.

52:18 did I get it wrong this Well, you taught us something about

52:28 black curves being parallel. Look at blue. You said these are

52:34 that's the class two, right? then I come on to the next

52:40 and I'm tell I'm telling you that curves have the same slope also and

52:49 seem seem right. Does it going to, to this curve, the

52:57 between the upper and the lower kind remains the same? And yet when

53:06 look here, uh the amplitudes are S oh my God, Fred.

53:11 crazy man here. It looks like , they're the same right amplitude there

53:16 it is much different there. So wrong because I was wrong. They're

53:22 same magnitude, but they're not the amplitude. You see this is plus

53:35 right there. Take the peak here not the peak, it's the

53:42 That's the first gimme that's minus two a magnitude of four here at the

53:50 , far, this is zero, this is minus four. They have

53:57 same magnitude but the amplitude is OK. So when somebody says,

54:11 , this is the biggest amplitude, was it turns out that's the smallest

54:18 amplitude has a sign. But don't with them because we'll have a hard

54:22 discussing magnitude versus amplitude. But we to know the difference when we were

54:30 to say the difference. And these amplitudes is the same as the difference

54:36 the two amplitudes over here small point you happen to have a gas,

54:48 contact. So you have the same and the gas is lower velocity and

55:01 density, the that water sand. what does it say? It tells

55:07 the reflection coefficient and positive and it an increased of amplitude with offset.

55:15 other words, its slope is gonna up like that. Like this

55:29 this is the one of the better interfaces, fluid contact that you'll see

55:39 Sea nice flat event there. That's positive reflection. An example.

56:00 I'm gonna give you my definition of do you quantify class 12 and

56:09 How do you quantify that? And this is my attempt to show you

56:16 you quantify it? For instance, told me this seismic data that she

56:23 last week, most of most of zone of interest was a class

56:32 What does a class two look like it? Maybe your class two is

56:40 bright spot for me or maybe your two as a class one from

56:47 How can we be? Sure? we're gonna go ahead and look for

56:52 method to quantify the amplitudes that we . I'm gonna take a far offset

57:03 call it 30 degrees and I'm gonna notice this, I'm taking the absolute

57:12 of what I find on the amplitudes the far offset. And I'm gonna

57:20 that I want, I'm gonna call K times the normal incident. So

57:27 class two is now defined as take far offset if it is two times

57:37 than the normal incident. That's a two. No, if you

57:45 that's all, that's the only definition would really need there. So we're

57:53 look at the class two at 30 . This is the green, it's

58:01 degrees right here. You got an of minus two. Your normal incidents

58:11 one. So on your favorite one of your equations minus two is

58:19 to the normal incident, which happens be one plus 0.25 times the B

58:29 slope. Now 25 is the sine to 30 degrees sine of 30 degrees

58:36 0.5 square, that is 0.25. that's gonna give us B solve for

58:42 and it becomes minus 12. So and here is minus 12. Now

58:50 go for the other one. Let's the red curve right here. The

58:56 O is minus amplitude at the far is minus two. The normal incidence

59:03 minus one. So you have a B of minus four. Here's what

59:12 means. We plot normally plot the incident on the X axis in the

59:20 . On the why this green 0.1 more incidence than B that is this

59:29 right here. This point of minus and minus one is this value

59:39 Draw a line through this right in . And that happens to be one

59:46 the far absolute value is greater than times the absolute value of the normal

59:54 , everything within these bonds right So if you get a normal incidence

60:01 and you get a slope value and one value falls right here, you're

60:07 be a class two. If you're this side, it's a class three

60:12 this side, class one. And finally, this is something that has

60:17 slope that's positive. Most slopes on CD P gather that et slope is

60:26 be negative very few class fours. when we look at this data

60:39 we see that this is a class , this magnitude there is greater than

60:52 times that magnitude right there and so . Here's a little exercise that you

61:06 put on your computer. How many a Mac? How many, how

61:13 have a Windows ss start again How many have tips running? Who

61:19 tips running? One Jessica? Do have tips running? I don't,

61:29 I can move to a computer that , ok. Can you get,

61:34 you get to it on, P day? No. Carlos.

61:40 you have tips running for some I can't hear you. Carlos.

61:51 doesn't look like you're muted. Just your head. You have tips running

62:04 no, it's not, it's not properly. It's like there are some

62:09 . I don't know why is it windows environment? No, no,

62:13 in, it's in a Mac. on the Mac. Yeah. Do

62:18 have avail, do you have windows for the tips? You don't have

62:24 bill? No, no, sir. Ok. Where do you

62:28 ? Houston? No, sir. Colombia? You're in Colombia now?

62:33 , sir. Ok, I'm gonna you a plane ticket to come up

62:36 expensive cash. Ok, let's I can make it. Yeah.

62:43 . Would you like that to be class? Yeah. Yeah, that

62:47 be good too. Ok. I'm missing somebody here. Aren't.

62:52 , there's only four live. Yeah. Ok. Who in this

62:58 does not have tips on a You don't and you don't and you

63:09 three well, that kind of sty . The idea of having a,

63:21 all day type of, uh, think, uh, or ok,

63:34 have to change, change the game . What I was gonna say,

63:42 is a nice exercise to do to how you go from class 123 and

63:52 . What are points hot if you a class one anomaly. And you

63:58 if I give it a little bit gas, I'll get a class

64:03 Well, surprised you gotta go through two first. As it, as

64:07 increase the that amount of gas or lower the velocity, it doesn't jump

64:13 1 to 3 or 1 to And this little exercise shows that

64:24 So real data, class 123, is a show, this is two

64:37 data didn't have 3D. They I did uh you're looking at a

64:48 blue, the color bar, red negative, blue is positive. So

64:55 is a negative, positive. That that you have a negative, positive

65:03 acoustic impens means you're negative coming down like this. That happens to be

65:13 lower acoustic and bees than the surrounding trough peak. Likewise down here,

65:23 bright amplitudes sitting in there. These class three bright spots, deep water

65:29 of Mexico. Let's take a look the dotted rectangle and see how that

65:36 with incident angle, all the angles the amplitude changes 0 to 12 degrees

65:44 to 24 to 36 when I looked at the bottom and compare that to

65:52 immediately. You wanna say Fred, got bigger amplitude on the far

65:59 And Fred has to complain that Fred too smart when he did this because

66:06 is the company's software wasn't developed for VO And so when I brought this

66:15 section of the block, the program computes the background amplitude, the R

66:24 background. And then plus at 0.7 when it gets down here, the

66:33 amplitude is very low. So it you're gonna need a higher gain to

66:38 . And so it's hard to but this amplitude is the same as

66:46 if I apply the same gain Now, you can see that by

66:52 at the CD P gather right here is the CD P gather at the

67:00 site. Look right here near look at the trough almost the same

67:08 all the way across. Now, know what you're saying. Ah Look

67:13 this right here, Fred, that's the same amplitude. Well, what

67:18 got there is something that Fred wish there this data as what's called a

67:31 multiple suppression. And after you do move up, if you have

67:41 normally they are a slower velocity so when you normally move or correct a

67:47 using primary velocity, you normally have event that is parabolic like this.

67:57 So you search that isn't right, like it, you search for Parabolas

68:10 program or actually find that multiple and will design an operator that looks like

68:19 multiple and subtract it off, but subtracted it off at the zero offset

68:31 took the amplitude away and we don't that. So that's originally one of

68:37 downfalls of the original, the multiple radar is if you did have a

68:44 multiple there and there was a, another reflector like this, right?

68:50 just wipe it out at the near . And that's what happens over here

68:57 . Current processing doesn't do that. yes, the class three did have

69:01 aptitude that's consistent. I go don who will make the assumption that this

69:08 here is wet and I look at amplitude and I can see it,

69:13 amplitude is being compared to this amplitude depth. Is it direction zero?

69:26 what does the well cite if I a welder, I can make an

69:31 vo response for wet and gas at location, a tip type of a

69:38 . And we see the gas and wet both are essentially flat out to

69:45 40 degrees and the gas as about one to about three times bigger than

69:56 web. And that might be what seeing here, that amplitude is about

70:01 times bigger than that. So that's class three. And if we look

70:09 the summary gas zones or oil. you have a high G gas,

70:17 ratio, gas zones are bright on stack and all angle limited stacks,

70:25 angles. When I looked at this here, that was angles between zero

70:33 12 degrees, they were stacked Amplitude, gas, amplitude is constant

70:45 increases slightly with offset if you have great big change in amplitude with offset

70:57 you can't relate it to radon. that's another anomaly. It might be

71:02 limestone or a volcanic sitting there. wavelet is a trough peak on all

71:11 stacks. Hydrocarbon prediction is possible from stat. You can actually say,

71:19 that an oil, is it wet is it gas Peggy? How do

71:28 know you're in class three and bark the background interval velocity between 14,000 ft

71:35 second? Who's gonna work for oil gas exploration? Anybody in here wanted

71:45 get oil and gas? You all to be environmental. Judge J

71:52 is anybody else out in the other ? There gonna be uh oil and

71:57 industry? OK. The reason I'm that even if you think you're a

72:10 and won't get involved uh wrong because gonna be looking at seismic data more

72:17 the geophysicist is gonna be looking and gonna come back and have a responsibility

72:26 your data is gonna get processed. , they're gonna ask you what do

72:30 want and you're gonna have to tell what you want. You're gonna

72:37 well, I want the data process not enough. No, you have

72:43 say I want a stack and I want these angle stacks. And I

72:54 want the CDP gathers themselves right before stacked. But the biggie is in

73:02 red diner. You have to I want the background velocity field every

73:11 cds, they do at least a analysis. And you want that velocity

73:19 because you wanna know what is the , velocity in my zone of

73:26 Because it's, if it's 50 to , 50,000, what 5000 to 9000

73:33 per second, you're gonna say I be in bright spot regime and you're

73:38 expect to see all of these. have a question. We have,

73:45 have, can you hear me? have what a question? Uh

73:52 we have seen everything here that is . It's the seismic is intact,

73:57 ? But can we do the same depth? Absolutely. When they,

74:06 they do this in depth, they to make a velocity model a 3d

74:13 model. And you want that because want to know what was the interval

74:19 in your target interval? That's even because it's it is more accurately computed

74:27 they do a depth model. So . And you want the CD PS

74:37 time, I prefer time because if process isn't very good, the depth

74:43 look screwed up, but time is forgiving to the beginning processor.

75:00 Class two Avios. I really, wish I could take that little blue

75:10 and get rid of it right by . Well, because then I could

75:15 you, do you see any hydrocarbons this seismic se in other words,

75:22 don't see hydro carbs on a stack if it's class two and we need

75:30 know what velocity range it might be we'll, we'll give you that.

75:36 that tells you if you have class , you better have some type of

75:42 vo discriminator. What would that Just having three different offset ranges allows

75:49 to examine what the avia would So that's the minimum that you

75:56 Minimum. These are gas, let's at. So this whole section

76:05 I'm going to squeeze sideways. Remember you wanna get a good interpretation of

76:12 structure and you're having a diff difficult , squeeze it together, make it

76:18 horizontally. It helps your interpretation. , when I did that, we

76:24 down by the well, and we this is blue red, that's positive

76:31 negative. I didn't want that. thought that should be negative.

76:36 that hurts. OK. I have arrow for some reason pointing there.

76:44 would I put that there? I know. Let's look at the next

76:47 range right beside it. 00 Look iphone all of a sudden with

76:57 That blue, red is now a , blue and look beneath it.

77:03 multi red, blue, red, sitting down there ears. Oh.

77:09 , remember this? You didn't know we picked it. Look at it

77:13 . It has an amplitude. Let's right here. Oh, it's picking

77:22 an amplitude now, wasn't there? , let's go really far. I

77:30 hydrocarbons everywhere. Oh, my Bosses are gonna be so exciting.

77:36 even had hydrocarbons migrating down de no in the other world except on my

77:42 . Does the hydrocarbons go down dep . This makes it suspect Fred.

77:49 . Look at this. No, II I, any place that I

77:55 , I'm gonna find hydro cars. is just tremendous except for one thing

78:01 not gonna trust this. This is and normally that is one of the

78:12 risks in the Gulf of Mexico, water. And how was that?

78:20 100 companies list this as one of biggest risks. This is a clean

78:26 , a very clean sand and it I pros but the main thing is

78:33 clean and what happens then it can like a gas s what does the

78:39 see? Have a very high sheer velocity and it's going to give it

78:47 big poison ratio difference. So this here, Ashley is a clean

78:59 Let's look at someplace else that arrow we go to officer, it's

79:07 This right in here looks like the wasn't showing up on the normal

79:15 but it's getting bigger. It has amplitude increasing magnitude increasing. I come

79:24 here in the red zone and look it and say, hm, as

79:33 go from far, which has very reflections in there, the near,

79:39 get all kind of good reflections. . So what is this telling

79:46 Big hint, geologist geo scientist, hint going from here to here to

79:54 , we got a will. There's sand in here. There's no sense

80:03 all shall how does it, how it show itself? Look at the

80:07 offset, it loses amplitude with Oh my gosh. Does that may

80:14 ? I look at all those reflections there. Yeah, all of this

80:20 of looks like massive shall sitting in and you can draw it just by

80:27 fact look how the amplitude decreased with . Big clue. Remember on Ruther

80:38 William's chart, the slope was negative everything except one class war. That

80:48 the magnitude no has or has a of getting smaller it off. And

80:55 what you're seeing right in here. chill a sand starting operating here.

81:09 help. Really big help. If look at the stack section here is

81:19 where the reservoirs might have been. look at the CDP gathers this is

81:29 the field, this is off the over here. See that blue line

81:39 blue line is normally offset as equal depth. Normally, you don't see

81:48 data. Normally, you don't see . Normally you don't see that we're

82:00 out very far and we'll show you reason why. So that's a

82:06 that's a gas down there. I at the amplitude versus offset how it

82:15 and the wet sand ick is over it dies so you can start off

82:25 it does. The, yes, it starts off small. But when

82:34 gets way, way out here, is a monster. You compare this

82:41 that and it's so much bigger. you're seeing right here going across this

82:53 right here. Is that a gas ? Yeah. Well, look at

82:59 . Does it make it to the ? But there's nothing else, nothing

83:04 . But really this thing right Sean got a little another one down

83:09 . This is your clean sand. clean sand doesn't have anything on the

83:14 offset. Now, the biggie don't down here. Some of you are

83:26 as it don't look. Ok. is a very special volume special because

83:33 has something very unusual. This is is equal to depth. Notice how

83:39 events are flat here and then they upward. In other words, the

83:47 our correction was wrong. We over . That is known as the hockey

83:54 effect. It looks like a hockey . You hit the puck with this

84:00 right here and so you don't like , you rather that they be flat

84:11 this prior to 1991. This is we lived with actually a little earlier

84:21 that, but around that time and this. No leaning back and let

84:33 tell you about a young phd by name of Brian Duvall. And around

84:42 Brian was getting his phd at Colorado of Mines and he gave me a

84:48 call. His dad is a well Geophysics in Houston. It says,

84:54 , can I come down to your and process some seismic data? He

84:59 I have nine components. I have phones too. A vertical phone.

85:06 had vibrators that came out shook horizontally two directions and vertically. That's nine

85:13 now. And we don't have enough power for me to process it here

85:18 the school of mines. I OK, bring it down. So

85:26 brought it down to Houston. He , well, I'm here,

85:30 I'd like to do some interpretation because processing takes a fairly large time and

85:37 only run it when it's none of year jobs. The company G is

85:42 Corporation was running jobs is OK. said you're just lucky. We got

85:49 , a 3D volume that's nine square . It's an offshore block and we're

85:58 it for free because we don't have 3D that we can show people that

86:04 can process it. We don't own . And I, I can't get

86:08 off the company that's shooting it. he says I found a count in

86:12 oryx that said, yes, they'll it. And I told him

86:15 I'll show him everything. I won't back. I said, II,

86:18 don't think it's right. You're taking and I'm gonna wanna release some of

86:24 . So we start processing for them I want to show you something we

86:32 for Brian F. He, we down to the work room and there

86:37 13 piles. Each one of them a different wall location. We had

86:43 the modeling done, all the processing stack sections, the CD P gatherers

86:50 angle stacks. And he comes down says, Fred, we're gonna have

86:55 get these normal move by corrections. gonna have to correct for them.

87:00 just, oh I says, I says, well, why?

87:04 said this is the sign of hydrocarbons you go ahead and you get those

87:14 , which is thing here. He , look at the far offset.

87:19 do you, if you stack what's gonna happen, you're gonna get

87:23 stack here here and down here, get something to stack here here and

87:31 . Every one of these that I drew, but that's the only energy

87:35 gonna get from the far offsets to right of the red line. They're

87:41 hydrocarbon reserves. This is the the only events on this far offset

87:49 the hydrocarbons. Whoa. So I we better go ahead and look in

87:55 literature and find out how to do is. Oh no. He says

87:59 is due to anisotropy as it will that, that was published by Leon

88:06 . Professor Eric Mines the most read paper in the SCG history by the

88:15 . And I said, well, we better go find out how to

88:17 that. He said that's ok. School of mines published an article about

88:23 to apply that. So don't people it? He says most people don't

88:28 the data that you have. You field data from Fairfield and this is

88:34 unusual data. Most people get seismic that goes to the offset is equal

88:41 the depth of interest. He says have offsets that are 15 miles away

88:50 Fairfield laid a line from the coast then go out 15 miles and then

88:56 shoot in between two lines, no . The cables are ocean bomb sensors

89:02 just so they got this tremendous offset you got all of them. So

89:07 able to go 2 to 34 times depth of your offset. It's

89:13 So we processed that we solve Brian did not. And when we

89:18 done, the data looked like this was that CD P gather and then

89:26 anisotropy as a new parameter, it very nicely. Look at the stretch

89:32 you see up here when you don't or correct them as much, they

89:37 have that stretch. This is a right here. Look at that.

89:44 is that this does a real good right in here. That's a pretty

89:48 match on the data. And sometimes go ahead and bring a overlay and

90:00 it on top of this. And you don't see this section and

90:06 where are the hydrocarbons? If you see them on this day, it's

90:11 . And I said, OK, , where, where are all the

90:22 ? Oh There are sands up Yeah, you can't see them all

90:27 you can see are the hydro chromes that's the resistivity sitting right there.

90:33 same with the field data. All see are the hydro carbs.

90:40 this leads to something that looks like . This is your conventional stack.

90:47 you find four hydrocarbon zones on Would you drill any of that?

90:56 , look at that. Would you any of that? Well, they

91:01 look good. Well, as it out each one of those locations here

91:09 , here, here all have No. What, what is the

91:23 between these? This is only the far traces only this data, only

91:41 data on A S was added together inside data right here that who's this

91:54 take? Only the very far? this is actually called officer, the

92:01 , the officer E equal twice the that's all harder comes in. Now

92:13 gonna watch for my audience participation. want you to look at this and

92:21 me reflectors. OK? You see that is. Let's go back.

92:32 kind of like right there. what's different one has reflectors? The

92:45 one doesn't one has reflectors and the one does it. These are the

92:56 far offsets. These are the near . Now, this is a class

93:07 . Remember what I said about shall shale. What happens when Shiel upon

93:16 , you go to the far off , shell on top of shell,

93:23 no reflections, shell upon shell on near offset. Ah But you got

93:33 . What the heck is all this ? This comes about by something in

93:40 photography. If you go back to 1976 Pete Vale at Exxon said seismic

93:55 come from Chrono Strat democratic boundaries. does that mean? Can a geologist

94:02 me what a Chrono stratigraphic boundary Halley said she cant Galley puts a

94:09 Stratigraphic boundary? Carlos I think he what it is. He's just keeping

94:21 . 00, we got an answer the audience. What is it

94:27 Yes. Chrono stratigraphic is a time boundary. What makes it significant?

94:34 a flooding surface. So what we're at are boundaries that are really quote

94:43 surfaces. That's what Deville had to . Now, remember something else that

94:52 about during the 19 sixties, that all very short offset type of

95:01 Now, they also said something They said something besides chrono stratigraphic

95:08 What were the other type of boundaries they talked about? Lithos, Strat

95:14 boundaries, lithos, Strat democratic boundaries those that occur because it's shall upon

95:25 interstate. Where do we see Mostly? Let me think,

95:30 let me think. I remember yesterday showed Ralph Chewy's plot, what which

95:42 was that you took? And you 0 to 15 degrees A CD P

95:49 and then 15 to 30 then 30 90. And in the middle,

95:55 he went 15 to 30 degrees, saw all these reflections but none

96:01 near offset just on the far in examine and lo and behold, they

96:07 all sand reflections and shale. So responded to voice songs ratio. Where

96:18 Poisson's ratio and the only equation, know, the farther offsets,

96:25 voice on ratios. Lithology and mythology in the father of them. So

96:31 have litho Strat Democratic reflections. Where the litho Strat Democratic reflections occur in

96:39 far offsets? So these are Chronos Democratic and they can include sand over

96:47 or shell upon shell, shell upon . You can have two different types

96:51 shell, but this one says it's shell. There's no change in

97:01 You can have all those different reflections the normal incident. But shell upon

97:06 is your litho strato? So here have now another feature, the litho

97:12 reflections that's coming up. So class , what does that give us?

97:21 we take a break at 10 I think we did, didn't

97:25 Oh, we'll do a break it around 1030 or so. Right.

97:30 think that was it. Um Let finish this and we'll take a

97:34 Ok. There's no indication of gas the near Englestad, very small normal

97:45 , reflection class two. Remember Rutherford Steinman gas amplitude increases with offset negative

97:58 event may or may not be event the stack section. Interesting. That

98:04 Rutherford Williams paper. What wavelet may may not be a trough peak on

98:12 stack section, but the waver is draft peak on the far angle stack

98:19 class two. Now the encouraging this is where interpreters take hold and

98:27 making a little advances. Inferences of are apparent when comparing near the far

98:35 stacks inferences such as what happens when go into overpressure and you get a

98:44 spot. Should you drill it? at the far off? Sets a

98:50 alone without calibration cannot distinguish a clean sand from a gas sand. Big

99:00 . This is why clean sands are as one of the biggest risks for

99:07 type of drilling. And if your interval velocity is between 23,000 ft per

99:20 , expect to be in class to . Somebody asked, well, how

99:25 if we have depth sections? if you have depth sections, the

99:30 beauty it is because you have a detailed interval velocity model that's required to

99:37 a depth migration. And you can where is the 9 to 14,000.

99:42 could say when I get at this , I'm in class two, pay

99:46 my different environment, different type of signature. A VO was invented for

99:58 two anomalies class three. We find look at the stack section, class

100:10 , we're going to have some type an Avio feature. We gotta have

100:14 different angle stacks to look at the P gathers something has to be

100:22 OK? I have a question real . I I don't quite understand how

100:27 distinguish that clean sand that starts you start to see those bright spots

100:34 increasing amplitude and it can be a sand and it can be a pitfall

100:39 how, how do you determine that is a clean sand? Um That's

100:49 this right here comes in Avio alone calibration cannot distinguish a clean sand from

100:59 gas sand, right? So what do you need to? We can

101:03 some inversion work. Look at see we see any significant difference in sheer

101:09 velocity from the o other ones because sheer wave velocity increases when you get

101:15 a limited uh clay content. Um songs ra or sheer wave used to

101:28 something that they would run in the for the petroleum engineers because it gave

101:35 an indication of the clay content. version. So anything that gives us

101:41 indication of the clay content and one be the sheer wave velocity. That's

101:49 uh we could put that into some then to see how that would go

101:55 a normal instance to the far But you need calibration, well controlled

102:02 to help. Maybe somebody else has magic wand. I don't have

102:10 You'll see that when I talk about analysis, this is Pete Rose in

102:17 consortium. I don't know how many they had probably over 100 1

102:22 But have you gone through 203 100 prospects? And it keeps coming out

102:29 . Sin. Bit me. When drilled this, I can't give you

102:36 positive answer. I don't know who it. OK. Yeah.

102:41 fair enough. I just didn't know I missed it. Um So nothing

102:54 . Let's take about a 10 minute . I got uh 28 after let's

103:01 back around uh 10, 38 and half missing, missing one from uh

103:20 America Carlos. It might be the zone. The internet shuts off.

103:41 . Any questions? It's OK. . Hang with me. We're way

103:55 there and I don't know how to down there without screwing everything up.

104:08 . Wrong class one. A bo righty. Um I, I do

104:17 a story to tell about Brian He's the one that led us to

104:23 the very, very far offsets. in the upper and mid night scene

104:30 class two, they were absolutely I mean, you, you got

104:36 sections and all that was on the sections were reflection from hydrocarbon beds.

104:42 else disappeared. You couldn't ask for more. And when we discovered that

104:50 did, I went back to the company that gave us the 3D data

104:56 we could show. And I told that this is what happened. And

105:04 said, nobody else knows this. said, but as soon as we

105:07 processing data for somebody, it's gonna leaked out. Somebody at the bar

105:13 gonna listen to his buddy that's with company and it, it's gone.

105:17 said to him, it's not gonna a genius. I said,

105:22 we're not as smart as a lot those guys out there. They'll get

105:25 real quick. So I said, we do have a time that you

105:30 make a, a AAA good deal money off of this and all the

105:35 sales for the next six months, the Gulf of Mexico Lial, you

105:40 be able to go ahead and bid lot better than you've been bidding on

105:46 transition zone, this Miocene uh type trend. And I told that to

105:55 uh oil company or X. And said, OK, let us think

105:59 it. And, and what they is they immediately went over to Western

106:04 and also PGS and they showed him work and said, can you do

106:09 but only cheaper than what the, company wanted to charge him? And

106:17 never heard back from them. I heard that from my friends at Western

106:21 . They called up, hey, guys are doing good work over

106:25 Thank you. So we went down another company and it's called Zilka.

106:30 I tell you who Zilka was? ? Mister Zoka made his money fortune

106:39 motherhood, a store. I think was, it was in the United

106:43 and it was a store for providing and baby support issues. Uh And

106:51 had it throughout the United Kingdom. sold that and he wanted to be

106:54 movie producer. So he went to and bought Sony movies and that didn't

107:03 out too good. So he sold . He came to Houston and

107:07 son-in-law, you're 26 years old. got a GE geology degree. You're

107:14 new exploration manager. I'm gonna form oil company. So he formed an

107:18 comic and he went to Fairfield Geophysical said, I want all the seismic

107:25 you shot or they shot all all the very shallow water and add

107:32 about 100 and 50 ft water depths they had it all up in Texas

107:37 the way across Louisiana. Also my . And he said, what we

107:46 is you give us this data And if we find something, we

107:52 drill, we'll come to you and you, we'll either give you a

107:57 amount of money, 102 105 $100,000 up front or you can wait till

108:04 start producing it and then you can a certain percentage of the uh output

108:10 we get. It's a good deal Fairfield didn't cost them anything. And

108:17 Mr Zoka came to us and ok, don't tell anybody else about

108:23 week later. He says we'll provide enough data to for you to process

108:29 that way you'll make money on it we'll pay the initial price you

108:35 We're not squabbling, it was very , it was three times ordinary

108:42 And uh so this is fine. , they provide us a lot of

108:47 and they had a processing center and would prepare the data for us and

108:52 just had to put it through the processes. We made a lot of

108:57 by a lot, meaning that we giving bonuses that were a year's salary

109:03 some even more. And uh iii hate to tell you that our profits

109:12 like 75% of our revenue. It just unseen Mr Zilka, his old

109:20 after being a year and a half . He sold it. Remember he

109:24 have anything. He sold it for 1.5, about $1.75 billion for a

109:32 that just started. And they would him, how do you, what

109:38 your success? Every hole you drill successful. You don't drill dry

109:43 Mobile. They Exxon, they tried duplicate the processing but they didn't have

109:48 very, very far offset data that have. So he was able to

109:53 go ahead and keep going and get these good holes. Made a good

110:00 . Anyhow, we didn't care if Zucker made all that money. We

110:05 good. Funny too. That was . Ok. Let's look at a

110:08 this is the very unusual deepwater It's offshore Texas and you can see

110:15 dipping beds, how all of a they're counteracted. Look at them,

110:19 all dipped on to the right, all dipped on to the left and

110:25 drill the, well, it's a blade. They have a, they

110:29 a cable that's 31,000 ft long and going at a zone that's 16,000 ft

110:37 . So they have acquisition out to the depth that they're gonna have.

110:43 at this section here. I see that makes me say drill here.

110:50 this is Elf Alcoa sitting there. so we looked at the three angle

110:57 , 0 to 1212 to 2424 to . And I, I draw your

111:03 to this right here. We, , picking that peak and as I

111:10 down to the far offsets, it like I misplaced that little arrow in

111:17 , but it's not, the peak disappears as we get the far offset

111:23 that's gonna be critical because you're gonna Rother Fred and Williams. So,

111:32 is the conventional. Well, and Depp, we're gonna assume it's

111:36 Don dip and I will show you CD P together. Now, I

111:41 to ask you a favor and please look at the seismic D No,

111:49 look. I see you're peeking. , you weren't working. You

111:55 you weren't awake a couple of minutes . As soon as I said,

111:58 look. OK. Now you can . I compare the CD together.

112:04 Depp, the CD P gather at well site. So both of

112:12 here's the zone of interest. The decays with offset. Same here.

112:17 amplitude decays with off. I, don't see anything about the near trace

112:23 here and the near trace amplitude here make me jump up and down with

112:29 and the fact that the amplitude is with offset, it makes me feel

112:34 they're the same, you know, not gonna be able to measure

112:37 this small difference. But what do see when a takeaway? Don't

112:42 see. Now, what do you about the upper one all of a

112:47 looking at this, we see the does decrease its offset right there.

112:55 , excuse me, you got a reversal, it goes from trough to

113:06 . Come over here, you don't any amplitude at all. Ouch,

113:13 is what Rutherford and Williams were talking and of course, they did not

113:18 to go out to this far of all. If I look at separatist

113:24 , what do they show? They that the wet, which is this

113:27 de the amplitude decreases, but it goes through the zero amplitude on the

113:35 far offset. However, for the charge right here, the amplitude decreased

113:43 offset and it became negative. So direct detection indicator for this is,

113:50 they find where this goes negative sitting there that remember Rother Fred and

113:59 they said we're drilling the hard What we do is we follow this

114:04 . There's a big amplitude. We don't drill, don't drill, don't

114:07 all of a sudden the amplitude disappears we say drill hard to say s

114:14 to sell to management, especially if have a gap in your coverage like

114:20 do right there. But when you at the Hartshorn that they showed you

114:25 the article, you'll notice where they a peak at one little small line

114:31 in the middle of my red it's a trough, it goes right

114:35 against the peak now all of these there is a peak right above all

114:42 way across a peak, all the across. How did I do

114:47 Because I was trying to show that peak, the trough, it's really

114:53 . We have isolated it like a above and below to say I didn't

114:59 up the normal mover. That's And, but being able to say

115:06 that's another requirement that makes you believe is really a truly an amplitude going

115:12 zero reversing polarity and having any well be able to make that plot goes

115:21 and reduces the risk for you, you feel very secure and drilling.

115:29 class one, a vo gas in wet sand amplitude decreases with offset may

115:36 phase and may be if it does on the right hand side, that's

115:42 good thing to note that becomes your detection indicator. A lot of times

115:47 go into an area not knowing what gonna see. Gas vent is smaller

115:55 than wet on the stack section. , the gas is reducing the amplitude

116:00 like refer Williams mentioned, the wave a peak rough on a near

116:06 It might be hm tropic on a we don't know. But when you

116:13 a sand velocity, if it's above ft per second, expect the class

116:20 because if it's sitting up against the very seldom do you have a shell

116:26 gonna be 14,000 ft per second. it is, it's different. So

116:33 when you put gas into this, that's not gonna go for it,

116:38 might get down to 13,100 ft per . That's a consolidated rough. It's

116:43 depend upon the ferocity and any So what, what, what did

116:48 learn now from this? Class one class two avi both of them required

116:59 that were greater than one times the they required very far offset. Say

117:05 another way they require angles at the 40 50 degrees. And Marie,

117:15 isn't, I will say too bad you can put nodes on the ocean

117:20 and use your boat to go to far far offsets in order to record

117:26 on land. This is tough because land, you gotta permit people and

117:34 gotta see what the activity is in area. So your area, it

117:39 become twice as big, becomes four as big. And that's what makes

117:46 getting the very far offsets of land little bit difficult culture. Evaluation of

117:54 P gathers often necessary for class one vo the, the nice thing is

118:03 as you get the farther offsets, get rid of the ground rule and

118:08 , which really kills you when you uh for signal to noise.

118:16 properties of Avio anomalies how the carbon makes reflections more negative. Can I

118:24 a question real quick. Yes. uh so the class one, you

118:30 the phase reversal and I guess you call that a dim out. Is

118:34 , that's correct? Or you you can, you might have a

118:38 reversal might have. Ok. And if you do have a phase

118:44 that's a really great, great sign cla for class two. If your

118:53 incident starts positive, it could potentially a phase reversal as well.

118:59 That's correct. So could it also a demo could also have what?

119:06 ? Well on class two, if want a, if if you wanted

119:18 classify it as a class two, can have small positive or small negative

119:26 incidence. The ref the normal incidence is below plus or minus 0.03.

119:34 when you get then remember it, you slope is negative. So if

119:44 negative, it's gonna get more negative comparing the far offset to the near

119:50 got, you got more negative and when you have a slightly positive number

119:58 you have the A VO class what happens is, yeah, you're

120:04 get a phase reversal but the far is not going to look as big

120:10 it did if you started negative on normal incidence. That's the main

120:16 Uh can you have a crossover? , they called those AVO two class

120:23 and that was Dan, that was Ross and Dan Kinman published an article

120:29 that back in the, I don't um early eighties. Oh, any

120:40 question, ah gas reservoirs have the magnitude of far offsets for class two

120:54 three. So again, it's pointing the importance to note, am I

120:59 class two or class three regimes? do we use? The velocity?

121:06 ? The velocity profile processors? Have ask for your two D data,

121:11 for it if you're three, once 3d depth, make sure you get

121:16 interval velocity volume. Normally they always depth because that's your QC. In

121:23 depth migration is updating that interval velocity and over again. Class three hydro

121:33 have large amplitude on all offsets. one and two can have direct hydrocarbon

121:40 on offsets greater than depth. They start to really show themselves until they

121:46 way out there. And that's on two. That was the Zilka.

121:52 When you come to Euston, there's concert hall with his name on it

121:58 that he donated some of his He used to class one though.

122:03 the one that Taylor was asking about gonna have AAA demo or phase reversal

122:09 a very far off set past we're looking for bright amplitude, bright

122:17 class two AVI interpretation works best because near offset amplitude is small. It's

122:24 relative comparison. If you look at far versus the near it's a death

122:29 . Hate going for small to B easy to see. Class one and

122:37 four A vo require good signal to ratio to discriminate hydrocarbon from brine

122:45 I, I did have a class that I would normally go over,

122:51 I'm not really proud of it. I can't find a real good class

122:56 in literature. Uh People say, I got one and you look at

123:02 and I, I even question it the processing correct that they really process

123:07 correctly. Class four requires an abnormally shall velocity. That's one of the

123:16 get it high. It has to , I don't know about 20%.

123:23 shell velocity has to be about 20% than the sand. In order to

123:28 to class four hydrocarbon and risk indicators the book from 1973 I kind of

123:46 various high to carbon indicators from the papers and Bob Sheriff uh iterate them

123:57 his encyclopedia dictionary. One of Of course, there's a newer

124:05 Amplitude changes bright spots. The amplitude in the Edwards play limestone dey,

124:20 gonna be pros fractures that are Hydrocarbons would be there change in the

124:28 parent. This is when you have gas and you're drilling for it,

124:34 can get bright spot and it just back and forth up and down and

124:39 multiples throughout the whole seismic section velocity . When you go through the hydrocarbon

124:51 , you get a lower velocity. , the lower velocity doesn't in the

124:58 chromes doesn't necessarily say when you do velocity analysis, you're gonna be able

125:02 see it, but there should be time sag underneath the hydrocarbon zone.

125:10 it's a un unconsolidated s it could the velocity drop significantly and you can

125:17 deeper reflectors and, and it deeper could be even dipping, but you

125:22 see going down and then a little and back up coming again. And

125:27 can see that sometimes when you look the stacking velocity at the edge of

125:39 and you're looking beneath, you're looking a bed beneath the gas zone.

125:47 happens is you might have a gas right in here and here is your

125:56 reflector and this is depth going You can have a CD P gather

126:06 your near traces are here, but trace goes through the CD P gather

126:17 goes through the gas zone or it be one where I didn't do that

126:31 good. You give uh you can the near traces here, go through

126:41 gas zone too. Each one of will each one of these considerations.

126:49 right here will give an enormous stacking because of delay here. Now,

126:55 have three delays, that'll give an velocity analysis. In other words,

127:01 of being a nice hyperbole like where time is going down, where

127:08 have one that comes out, right there and then you have a

127:13 So you try to fit the best to this one with a little bit

127:17 delay. That was those type of analysis and changes were done a lot

127:25 we had just two D data. right here you can actually predict the

127:29 of the zone of interest. Oh there are other velocity variations too.

127:38 Tom Davis, former professor at school mines, retired uh when he was

127:45 Amaco, he wrote a kind of interesting paper. He showed that in

127:51 , something like 75% 75% of all reservoirs had a velocity anomaly above the

128:02 . Of course, he said most these were on structure. If you

128:08 structure, you're gonna have a relief tension on the top of the reservoir

128:13 all the beds above you. So beds above they're on the peak,

128:18 could have a lower velocity just because structure wave, the changes polarity reversals

128:28 you associate them with the right a that we have, they occur at

128:33 edges. Burma is a classic example where they have multiple pay and a

128:43 , you have multiple pays and there's reservoir and she, it almost looks

129:05 you have a fault coming down here what it is, it's just m

129:11 of reservoirs that have a phase reversal from the gas to the wet and

129:22 of them seems like just all Burma. Ok. This is for

129:35 recent current graduate students who's a, taking the regular program, you tell

129:42 a regular graduate, you're a regular student. Have you had, who's

129:47 advisor? Doctor who? Joe Doctor Harry Joe, is that

129:55 Ok. Ok. Your advisor Rob . Ok. Anybody have Yin

130:04 Ok. You've taken Doctor Kagan's haven't you? Have you taken doctor

130:13 study? Doesn't he advocate the frequency below the reservoir? Here, this

130:20 right here, lower or frequency beneath reservoir because of attenuation, doesn't he

130:28 hydro reservoirs say lower frequent have an of a lower frequency? Five years

130:41 , five years ago, five we've just had a gentleman in our

130:47 in real life who just announced, can't remember a class of five years

130:54 . He barely remembers who taught Not bad, you know, and

130:59 thought I was bad with my Oh, that's OK. He's only

131:06 years old. It, hey, , I'm 50 years older than he

131:11 60 years older. I still can't the guy's name, but that's

131:17 There is a group of folks that that when you go through a gas

131:30 , it will attenuate the signal. there are groups that said yes,

131:37 not for the reason that you're And so this as not a large

131:46 but a following that like to prove one way or the other whenever you

131:55 a gas zone, you can have right in here. What then beneath

132:08 you got the wet too high up . Let's go. Let's put gas

132:20 , interface this and this is what here. And we have a low

132:29 10%. And down here it's all sw water saturation equal to one.

132:40 in this zone, right in you can have a water saturation that

132:46 is like 0.4 there's a residual gas here. 60% of this is still

132:53 , not economic. That might be little bit too. It's 2.5 50%

133:00 , 50%. We it might not economic to drill it vertically but

133:05 Yes. And so a sort of presence right in here could be something

133:13 the order of 40 ft, 50 . If you have a porosity of

133:22 then this thickness right in here might six inches and this is the capital

133:31 pressure uh that does this puts a still in here and then you get

133:36 here and you're into an all water when you get into residual gas

133:45 Remember what we said, a little of gas, like 15% to 15%

133:52 20% that gives you bubbles and bubbles to attenuate the signal. If you

134:00 one big bubble that's not gonna you need many, many bubbles.

134:06 this is the article that Ed White pointing out when you get millions of

134:11 , it'll just wipe the energy all . So it's still up in the

134:19 if you have residual gas saturation and a thick section. Yes, the

134:26 frequency is expected but not in the gas section. OK. Mylo Backus

134:36 at the University of Texas for many since passed away was a big advocate

134:41 flat spot. He was one of founders of the digital technology. Back

134:47 the early sixties, he worked for Services Incorporated G SI G si then

134:56 Texas instruments, one of the big makers. But at G SI Milo

135:04 on the digital technology and he always that there are horizontal reflections produced at

135:13 fluid interface and we just don't look them enough. And so he developed

135:19 at the UT in order to look fluid interfaces. You know what a

135:26 effect is. I showed you a effect, Lake Geneva, anybody ever

135:31 there guys? You gotta make enough to go there. OK.

135:38 it's called the Arab Playground where the men go there and they don't have

135:45 wear all the white gowns and that they could bring out their gold necklaces

135:52 even have a beer or drink wine hard drinks there. Chimney effect,

136:01 gas can deteriorate all your reflections underneath energy does not go through the shallow

136:11 sands. It tends to go Well, that's good news and that's

136:16 news. The good news is there was hydrocarbons here. The bad

136:20 is, is there any left in reservoir? And so that, that's

136:25 thing. Now Malaysia, they have chimney effects all over the place and

136:32 have big reservoirs. There was a by the name of Fred Alzada who

136:39 have analyzed, I don't know, chimney effects and he could tell the

136:46 . Was there an, was there reservoir gas level? He now is

136:52 professor over at uh Southern California. , hydrocarbon indicators is a gas and

137:00 high gas oil reservoir reservoirs exhibit a two A VL. No, the

137:13 and this one is one you better into your mind. And I think

137:19 you join a company, they'll tell that if you have a structural reservoir

137:26 you think its hyder combs in the hydrocarbon reflection should be different than

137:32 wet. And when you map, you map your reservoir, you can

137:41 a structural conforming put over top of , the amplitude contours as a

137:50 the amplitude contours should conform to the contours. They should have the same

138:00 water contact all the way around. is I would say the primary risk

138:11 that's done on all structural type of . And that's the first thing that

138:18 asks for, show me the structural to the amplitude. And if you

138:24 show that you, you, you a good chance. You, you

138:28 sold the prospect, but they're gonna for it. The last one right

138:40 is one, as I said, came from Bob Sheriff, but this

138:44 came from Tom Lee and Tom Lafa to teach, uh, continue education

138:51 here for the U OF H and was a gravity person and he was

139:01 apt on gravity mapping, contouring et cetera. It was very,

139:08 good. But all of a sudden said, when the computer came around

139:15 in the pot seventies, going into eighties making maps for the regional

139:25 What's the gravity of the regional So you could subtract the regional charging

139:34 gravity from the regional geology. You to subtract from that, that you

139:41 to give you what's enormous observe. he saw these maps, he

139:47 coming out of the companies where they to apply some constraint and they replied

139:56 , what was it though? Third , fifth order, seventh order polynomial

140:05 to the data, the higher the you get, the more enormous smaller

140:11 got. And they just kept piling up automatic contour maps. And Tom

140:20 it. Amplitude interpretation must make geologically apply less principles of least squares

140:31 more principle of least astonishment. In words, look at what you're saying

140:39 the answer and look at the person you and they are they saying,

140:45 know, I'd be astonished if that geologically. It just is impossible.

140:52 of course, the least squares is upon maps based on the square contouring

140:59 more on doing it geologically. that means not 3D. This used

141:08 be two D where you didn't have data in between contour line in between

141:15 to the seismic data. And you to say what was the structure in

141:21 and how to use a little geological . And of course, a lot

141:28 new folks would do. You'd have clients every mile apart. North and

141:35 . And the young person getting on P A big high. You right

141:38 the middle of where there's no seismic out there. Hey. Oh,

141:53 . This is a article 2009 by Road. Ro Rocky is a

142:02 It's all by himself. He lives Center Texas. Do you know where

142:08 Texas is? Center Texas is, famous for a grocery store in that

142:16 store makes sandwiches all galore. But also has the largest selection of uh

142:29 beef, jerky camel, jerky, , jerky, sheep, jerky dried

142:39 . All selection you love. And is, you're going from Dallas,

142:47 to Dallas is exactly half white. why it's called Center Texas between Houston

142:53 Texas. People. Good place to , good drinks, good beef

142:58 great sandwiches that they make. Rocky there. And he has a cattle

143:05 , but he's a very well known and manager and they used to drive

143:12 distance 100 miles to work every day then have his home that he went

143:19 and he was part of this. he said we have over 200 prospects

143:27 that's 12 years ago. And he most of them, however, 90%

143:33 tertiary, most of them here are Gulf of Mexico or the deep

143:39 It's a major portion And here are of this classification, primary DH O

143:54 don dip amplitude contours. Over you see a structural map by the

144:03 line by the single black lines. is where the amplitude was above a

144:11 value. And so the amplitude was . The amplitude map does not conform

144:18 the structure map over here. This been better, excellent, almost perfect

144:24 and that got the highest grade So what is this great threat?

144:30 and associate? Have a computer And they're gonna ask you a series

144:37 100 questions and you're gonna get graded each question. So if your

144:46 that's what it's grading your prospect. it has this, that's a great

144:53 , you're gonna probably get 20 That's, that's one of them.

145:01 other thing is what's the amplitude consistence the mapped area? So here it

145:11 the consistency or her just random type thing where the amplitudes go inside.

145:17 again, that's grade five, but not worth 20 points that's only gonna

145:25 maybe eight points because that was the and so forth. So here are

145:34 most important direct hydro chrome indicators for . Structural Amplitude on the Don dip

145:43 . Does it conform where you have , the gas water contact is it

145:53 both on structure and on the amplitude . Now, here's one here phase

146:03 character change at Don dip anomaly In other words, did the gas

146:09 a negative reflection? And what the on the stat, that's what it's

146:17 d flat spots. And then we the Avio attributes, various ones.

146:27 , Rocky gives him a nice and came from 2014 paper, Rocky gives

146:33 nice presentation on this and he points when they wrote the first program and

146:42 join their consortium, they give you program so you can grade your prospects

146:50 they first wrote all the questions. were geological omens. How co how

146:59 is your prospect to another? that's proven productive is your sin in

147:09 same reservoir as the most productive be you? Are you up dip or

147:19 dip from the last productive will? they had a series and they got

147:25 score. The, how they evaluate escort every prospect before it's thrill.

147:33 after it's drilled, they had plots say, how successful are we?

147:40 many do we say drill and turned to be dry? Hos they would

147:46 , they evaluated that. They said were 60% successful. So that's

147:57 It used to be 25% 25% of walls were successful. But by our

148:04 analysis, we lowered the cost of drilling dry holes as soon as they

148:10 amplitude. All of a sudden it like from 60% successful to 90%.

148:18 was the main emphasis getting amplitude, one amplitude conformance structure, then an

148:28 vo then bright spot, all the like that. No, these also

148:37 upon what clash are in the top . If you're in a class

148:44 a down dip structural conform most then if you're a class two,

148:54 second is C amplitude consistency and mapped . Now on class two, it's

149:04 be the far offset that you have the near or not the staff.

149:10 you gotta watch offset, you you would expect the stack to be

149:16 because it could be positive and But the A vo the first one

149:24 get there Avio observations and gathers or stacks. Now there are certain warnings

149:42 DH I and such a thing as you have watch tuning? And I

149:54 you an example of that where I proven flattened the hot and there's a

150:01 bright spot, bright spot with brighter and it's up to it up de

150:08 it was productive. But just on other side, there was another one

150:13 like it, it turned out it the tuning effect of the wedge.

150:18 was not the hydrocar reservoir thin The bald structure doesn't continue. Velocity

150:31 can affect conformance to closure interpretation. you have a thick velocity, a

150:40 reservoir in the reservoir is like this , you're gonna have a velocity delay

150:54 than on this side right in here it's thicker reservoir and over here.

151:00 underneath, right in here, you're have something that goes like this.

151:06 tilts, this is your gas water , but it's tilted because of the

151:15 velocity. Sitting over here. Oh dang. You always have to put

151:32 in something that doesn't work. Strat democratic traps are tough because they

151:39 necessarily have reservoir don dip conformance. as it shows heresy changes across the

151:51 and yet stratigraphic traps, one of biggest, biggest oil produced birds in

151:58 world and they have the biggest Major reason for dry holes, low

152:06 saturation, thick wet sand, hard volcanoes. Last two I porosity,

152:19 sands. I think that's it. . OK. Any questions that would

152:34 to uh entertain audience here, put in far, far land,

152:49 Anybody going to the rodeo this weekend rodeo playing. I keep seeing something

152:56 the entertainment. Does anybody know here's rodeo going on? What's that?

153:08 , and of the p and the , they're, they're advertising all the

153:14 . They're gonna be at the Rodeo the people entertainment, top names.

153:21 didn't make it again this year. for Rodeo. My singing.

153:27 anything else? Ok. I uh, 1130. We come back

153:35 1230. That the name of the . 1230. We'll see you

153:42 folks. Bye

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