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00:10 Oh good. I'm getting another, on my home computer right now,

00:19 it's asked me to lodge the meeting I'm just gonna quickly try this.

00:24 . Oh, there we go. just see here. Okay, Can

00:57 see that guy? Yes. Okay, well you might not be

01:11 . You probably had breakfast already, uh somehow it came across this a

01:19 back. I thought it was kind funny to put it together.

01:27 so we've been uh, we were about location and drilling and making measurements

01:34 and core and a bit about making situ or some surface into the material

01:43 . And just a reminder on us how cora's recovered. And here's,

01:48 one technique uh recovery of core is common in the mining world, in

01:58 hard rock world. So it's generally to the surface of course for

02:04 but they often use slant rigs as , the ones shown here. And

02:09 you can see the, the drill also, um the barrel in core

02:18 then uh, that's recovered. And in the hard rock world, the

02:23 , the full record of course is often recovered. And then you'll see

02:28 often displayed um in, in the like this. Typically the, the

02:36 is cut in half and half would to an archive or some kind of

02:44 and then the other half is, tested and and maybe maybe destroyed in

02:50 test. So invasive invasive testing You can see a couple of recovered

02:55 from two of our very common shale the marcellus shale on the East coast

03:02 the lower Eagle ford in south So now we've got, now we've

03:09 some core and again how they, just showed the over barreling technique but

03:22 also sidewall core and there are a of different ways that sidewall car can

03:26 recovered. And here's the, the method or an impact method where actually

03:33 tool is lowered into the well and tool just has steel cups that are

03:40 actually are blasted right into the side . And so these are, these

03:45 sort of cylindrical bullets and um, fired in and the cup or the

03:54 itself is on a tether and so goes into the formation, grabs a

03:58 of rock and then it's actually pulled into the end of the tool.

04:04 this is a, this is another simple way to, to gather some

04:10 rock. Then we could be a bit more sophisticated uh, rather than

04:20 the bullets into the side of the , we could actually have a tool

04:26 a coring tool called a sidewall coring . And you can see the

04:30 the little bit that sticks out the of the tool. It's like a

04:36 her wheel or some of the hubcaps cars that are around my neck of

04:42 woods here so that it rotates a drill bit and recovers a recovers the

04:50 . So that would drill into the of the borehole and you can see

05:02 kind of course that would be recovered this case this is an over barrel

05:05 of 3.5 inch quarter so and we've sliced off part of it then

05:10 filled it in with plexiglas so that can do some more experiments with

05:15 Um And here's another card. This to be from the Canadian oil sands

05:23 it's a it's a chunk of But you can see as I mentioned

05:26 , the sand is unconsolidated and it's fully saturated with bitumen. Actually,

05:33 love the smell of it shouldn't smell much but it's got a great great

05:39 . But what's done up there is is injected into the formation. So

05:44 play is that well, only a 100 ft deep and then horizontal wells

05:53 drilled in pairs. It's called sag . Steam assisted gravity drag drive.

06:02 the steam is injected in the top , it melts all the victim and

06:06 goes falls down into the bottom well then it's produced at the bottom

06:10 So uh in this part of the , horizontal drilling has been used for

06:16 decades and and mainly to get this . So you can see that after

06:23 steam has been passed through the oil , the sand is completely clean and

06:31 unconsolidated. So there's an example again an unconventional resource. The permeability is

06:37 high but the viscosity is extremely high . So it needs to be treated

06:45 , some people would say that this oil sand with almost 200 billion barrels

06:50 oil. There is mother nature's biggest spill and it's just all sitting there

06:55 to the surface and we're cleaning it steam and cleaning it and extracting the

07:02 . So here's some other other some rock samples from drill core.

07:09 we had done a lot of work um very assault. We're interested in

07:19 for a few reasons. Number it's, it's used itself just sodium

07:24 . There's a huge industry built around compounds. PVC polyvinyl chloride. So

07:33 the plastics use chlorine, chlorine in . So we're interested in getting the

07:40 , the chlorine out of the Uh also the salt domes make structural

07:48 for great oil traps beside them, talked about spindletop a little bit and

07:54 here, this has been the source a lot of the economy. And

07:57 of course right now the assault is for storage. So we've got these

08:05 salt domes that are thousands of feet . They're uh largely impermeable and so

08:12 can be etched. And what you is you drill a hole into the

08:16 and then start circulating fresh water. fresh water easily dissolves the salt in

08:21 brine. Then you pump the brine and then you etch or dissolve a

08:27 , making a cavern and you have do as the whole dissolves. Then

08:34 do repeat sonar surveys to see how it is and then keep on etching

08:39 dissolving the well to make these enormous and those can be used for petroleum

08:47 natural gas liquids. Some people have talked making them into sort of a

08:52 that you inject high pressure air when is cheap. And then this high

09:00 air can be blown back out through to generate electricity when electricity is

09:06 So it's a that can be used all kinds of different purposes. So

09:11 some beautiful salts. Um These are where we've operated Hockley at match before

09:17 I'll show you Stephanie, I'll show some of the, some of the

09:22 that I just got a couple of ago. That might be another interesting

09:26 for you. As I mentioned, guys are putting together a story where

09:31 want to raise some money and drill side of Hockley by premium of them

09:38 got the riches of mine. I down into a long time ago in

09:41 just not too far from Detroit, to cross the river from Detroit.

09:46 it was the big one of the salt mines in the world. And

09:50 Akira is one of the classic minds um Columbia, coarse salt was used

10:00 . It was the basis of You probably know that the word salary

10:04 from Sao or salt and roman soldiers paid in salt was so expensive,

10:10 valuable, salacious salud. All of words come from salt which means

10:17 healthy. Oh so so it's been for a long time. We regard

10:23 as just cheap and abundant. But most of history salt was very expensive

10:27 really valuable and we need it. some salt samples once again once we've

10:35 the sample this is not so much world, but in the in the

10:39 world, in the thin section the mineralogy world, they would take

10:44 samples and do a lot of stuff is ancillary. So as you know

10:49 X rays are shown on a on crystal we can shine x rays in

10:53 crystal. And if we had pure . A C. L. There's

10:57 diffraction patterns with angle that that So pure salt, the X ray

11:07 with result of angle looks like So that's kind of our template

11:14 I would like this. So if wanted to do machine learning this,

11:18 would be your template. The beautiful that you're looking for. Um We

11:27 at different salts out. Here's the sample from Hockley and you can see

11:31 it's almost pure beautiful salt N. . C. L. When we

11:37 down to Godrich the the Detroit It's pretty close to just pure

11:45 Then we go into zip Akira in and you can see that it has

11:50 lot of other stuff in there. you can imagine an algorithm that's what's

11:56 an algorithm that goes in and tries match templates to all this and then

12:01 out how much of each component is there. And when you re match

12:05 templates and there we find that it's it's probably about 90% N A C

12:10 . Salt. But you can see there's calcium sulfate, a bit of

12:14 courts and also some limestone calcium Anyway that's that's uh there'd be all

12:23 of geologic analysis done like this with core now that we've got the

12:30 So we also were involved this is bit ancillary just for interest. But

12:38 were also early on in presenting So creating our own core out of

12:46 D. Printing materials. And the D. Printing materials can be plastic

12:51 even even metals. And so there's lot there's a lot of interest of

12:56 now in the last 10 years on a design and not having to millet

13:01 manufacture it or put it into a . But just to print it.

13:11 we were doing a bunch of that here's one of our favorite guys getting

13:17 D. Printed. So we were were actually making rocks making our own

13:26 so we could give it certain velocities structure and everything. And then we

13:30 testing that. So here's an example making making our own core With three

13:36 . models, you can put porosity it And you can see on a

13:41 scale actually how these how 3D printing . It just lays down a little

13:48 in orthogonal directions. And then when , when you tell it to

13:52 it doesn't put the fiber down that a hole. And so you can

13:55 any shape by just programming the machine different shapes. And then it'll just

14:02 down the shape with these little little . So we were putting various cracks

14:10 porosity and making all kinds of different of rock that we're going to investigate

14:16 different pore saturates and then find the acoustic properties. So you can make

14:23 kinds of cool um kinds of pseudo or like rocks. And that's what

14:29 did. And then um and then can propagate seismic waves through them to

14:33 at their properties. So once what side, what's done with the

14:39 that comes out of the uh this And you can see that a lot

14:44 it stored for example in in Austin over half a million boxes of

14:53 So if you were working on a anywhere, um that's one of the

14:59 that the state has. So you go into and examine this this corner

15:07 just actually look at the rocks So the stories there, uh and

15:13 what kind of, what can you with that car? Well, as

15:16 geologist, you go in and just at it and describe it the the

15:21 of the shape, the length, grain size, all that kind of

15:26 . And then you can actually run various kind of harry potter wands over

15:31 top of this um to measure the Gamarra and make some of these other

15:39 too. All of these guys can done with the largely uh nondestructive

15:47 So we'll make all kinds of measurements the court to get its rock properties

15:51 how saturates would would behave in Ok, Another, another classic thing

16:02 gonna do with core is just try get another value. This is a

16:08 simple one. This is just a measurement. And in fact, I'm

16:12 show you mike Myers and Laurie Hawkins , did did you get over to

16:16 Stephanie in petroleum engineering? Did we you there? Um No, I

16:24 think so. I don't think Either. I took my class there

16:28 week but yeah, we might, put that on the schedule one of

16:35 days or I'm gonna actually say this another project. I'll give you three

16:40 four ideas for projects that may interest and then depending which one you want

16:46 select or somebody else is. But of the projects were just starting a

16:51 physics project with petroleum engineering in in this lab and I'm gonna show

16:56 . But here's one of the instruments they have. And it's a really

16:59 and it just measures the hardness of rock and how it works is there's

17:05 an inventor that goes down hits the and then just measures the diameter of

17:14 indentation. And then you can plot that diameter. That diameter relates to

17:22 an index or a number you can from it. And that number of

17:26 would plot against depth and properties and a log out of it. And

17:34 this number or strength is related to pressure at which the material breaks.

17:43 it's a hardness number but it relates how the material breaks. Why do

17:48 care well, because we're going to fracture the material, we need to

17:53 it's the forest or the pressure is to break it. So here's a

17:58 a number that gives us an idea what kind of pressure is going to

18:01 required to hydraulically fracture or break this . So just one example of what

18:07 can do with current. Now we also non invasively put an ultrasonic transducer

18:16 the top of the corner, one the bottom. And then just measure

18:18 transit time. So the upper transducer a little vibration and then we have

18:27 transducer that records the vibration. Sometimes can do the reflection measurement or the

18:34 measurement. So with with this ultrasonic , we do both in this case

18:39 can do a transmission just one way through the right through the material and

18:46 that's just measure the distance that the of flight picked the train travel time

18:51 . So we get maybe five centimeters by 20 microseconds. And that gives

18:58 the velocity of 2000 m per second something like that. So we can

19:02 that with a P wave, the vibrates up and down. Or we

19:07 have the transducer vibrate back and And that gives us a shear

19:12 We can pick the sheer weight of , Thickness L over the share wave

19:16 . 40 microseconds gives us say 1100 per second. Then in the classic

19:30 we always do in petro physics or logging or anything. We're gonna do

19:35 plots. And so for example we take that hardness number, the ball

19:41 number and plot that through against shear velocity and find that there's a direct

19:52 . So that's interesting. And then course the shear wave rigidity. We

19:58 that that's directly related to break ability the rigidity is a big number in

20:05 hydraulic fracturing equation. So um this again two measurements. We can make

20:09 ultrasonic velocity of material and the hardness platform. That can tell us something

20:15 how how hard we have to whack rock to break it. Okay now

20:30 again, just as an example, rocks are not pure. It's nice

20:34 we do get pure rock. So all the times we talk about rock

20:38 and logs and everything. Usually the are mixed and so everything we talk

20:43 is gonna be for mixed rock. even the simple salts typically have some

20:47 of mixture and here's some of the of the salts that other people have

20:53 on. You can see primarily salt lots of different beautiful character. So

21:04 Stephanie with dr Castano's course you probably a bunch of rock physics.

21:12 Yes sir. Yeah. Okay so show a few things but we won't

21:16 much time on on rock physics but would have showed also the the mixing

21:23 . If we take um Say two rocks maybe and then hydrate and and

21:32 carbonate or something else. Then we them in this case they salt,

21:36 hydrate, so we take 100% salt then introduce more and more and hydrate

21:42 it. Then the rock properties start vary and there are two numbers that

21:52 use for rock properties. One is the void and that is the rice

21:58 and that's just whether we're dealing with geometric or a harmonic average of the

22:03 . So do we deal with to the final velocity is the final velocity

22:07 one over B. Is equal to times one over B. A.

22:11 one B. One over B. . And the likewise the rice is

22:16 standard average. So and people generally that those two numbers reflect an assemblage

22:30 the of the material, whether it's stiff material or a softer material.

22:36 then those provide the bounds for how two materials would be put together.

22:45 just just to remember to about our types, of course we make a

22:49 and this is an elastic wave And uh if one of the ways

22:56 will propagate in virtually any material, wave is just our compression all wave

23:03 that particle motion is in line with direction of propagation. So this is

23:07 sound and air like right now or fluids or solids. We get this

23:14 of wave, we have to have the compressibility and a rigidity this guy

23:21 . And then as you know, can we can disturb the material

23:26 And then a wave just like shaking slinky up and down. The particle

23:31 up and down with the waves propagating the slinky as opposed to whacking the

23:35 on the end and the wave is in the direction of propagation. So

23:41 get our share waves and R. waves. And in the in the

23:44 or in the more hall we can these make these waves and measure them

23:50 they tell us about the rock Now as you know the when we

23:58 at the compression wave, that disturbance the material squishes the material. And

24:06 the uh the wave propagates with the depending on how hard it is to

24:11 the material. And so because we're the volume of the material, the

24:18 wave is a delta V. Over . It's a it's a change in

24:21 volume. It changes the shape. you can imagine that the that what's

24:27 the porosity or inside this network of matrix makes a big difference. So

24:38 I had a gas in this a gas in the porosity, how

24:45 is it to compress gas gasses? hard to compress gas. Right?

25:06 , uh it's not not relative. mean, think of compressing. Think

25:15 trying to compress water water, but you actually try to to put that

25:21 in a box and compress its It's extremely in compressible. Yeah.

25:27 always like kind of thinking in my , Yeah, like rock. If

25:32 if you try to squeeze a that's pretty hard to change its hit

25:38 . But if you have a you could take the balloon and squeeze

25:43 if you could do it without, squishing out. But gasses are pretty

25:48 to compress. So, because they're to compress, they don't provide much

25:59 to compression. And so the sound the wave itself is kind of sloppy

26:04 it propagates through. And typically it's slow. So the the the classic

26:14 for sound propagation? Just sound and is you remember that just how fast

26:26 p waves, how fast the sound in the air. Um I was

26:38 , like one point, I don't , I want to say like

26:43 but I don't think that's right. it's uh the number. And you'll

26:49 to again remember numbers in both of units, but it's 3 32 m

26:54 second, so just over 300 m second. So it's around 1100 ft

27:00 second. Okay. No, But that's a practical number, you can

27:10 . I I use it all the sitting up here in the 22nd floor

27:15 the city because especially when there's bad that comes in, there's lightning all

27:20 time. And so I'm always trying compute how far away the lightning

27:27 So again, when lightning strikes, see it, we see the the

27:35 immediately right. And then sometime later hear the thunder. So the thunder

27:44 from the lightning, ionizing the blowing up the air basically and creating

27:49 shockwave. And then the sound from lightning propagates. But of course the

28:00 propagating at three times 10 to the km/s. sound is propagating at .3

28:14 . So the lightning arrives, the arrives instantaneously the sound takes, um

28:21 going at 1000 ft per second. if you see the lightning and then

28:27 thunder arrives three seconds later, how away is the lightning? 3000

28:35 That's it. So I think that a good little number. So all

28:40 time when I'm sitting here and should we go play golf or when

28:44 are playing golf and you uh see lightning, just count how long it

28:52 the sound to arrive. And if Under 10 seconds then the lightning

29:01 You know, a couple of miles at 10 seconds. So that means

29:05 gonna have to get out of So lightning then the thunder under 10

29:13 . You better go a lot of if it's really close, you actually

29:18 it's pretty close cause it's loud, It might be, it might be

29:25 ft away, five seconds. Boom . Then we hear it. Or

29:34 Alameda Road, just up the A few years ago, two Bar

29:39 were having a dispute by the turkey hut. The two owners were having

29:47 dispute. And then one morning, is, I think five years ago

29:51 so, four or five years it was four o'clock in the morning

29:55 there was an enormous explosion, enormous that woke me up and everybody around

30:04 so I was actually testing one of seismometers here in, in my condo

30:12 the explosion, you could see it on the seismometer, which was

30:18 But it turned out that one bar was mad at the other bar

30:21 So the person got a bunch of to go in and pour gasoline on

30:26 guy's bar and blow it up. just, it's shocking that nobody

30:33 well, maybe somebody did die, knows the video saw the show people

30:39 away. But the problem was when poured gasoline all over this guy's bar

30:44 detonated it, they weren't too smart they didn't realize that their gasoline fumes

30:51 . And so the guys who did were probably burned anyway. It was

30:56 crazy thing. But it shut down whole, shut down the whole

31:00 There was wooden buildings all over the . We don't know of anybody who

31:03 hurt, but I'm sure people did . On my seismometer, I recorded

31:10 air blast, But before the air there was actually a ground way arrival

31:17 even on the 22nd floor, I in the seismometer. So the blast

31:22 a refraction in the ground that propagated Alameda Road hit the building and shook

31:31 building and it's slightly before the air . So it's kind of interesting.

31:36 must have been really mad at the guy. I'll tell you what,

31:45 really mad and really dumb. that was quite a thing.

31:55 that's really not the way that you to resolve disputes. But nonetheless,

32:00 some interesting seismology. Okay, so just talked about sound propagating through air

32:08 332 m/s. That's how I remember . But you could convert that two

32:12 per second somewhere around 1100. and immediately useful. I use it

32:18 the time when outdoors, if we're field camps or doing field work or

32:22 , there actually are laws when you to really shut down people working in

32:26 outdoors if there's lightning and typically it's about five miles away. So I

32:34 need to shut down crews and everything there's lightning in the area. And

32:39 find there's probably some golf courses up the woodlands. If there's a storm

32:43 a storm coming, you'll likely hear golf courses blow a horn. I

32:48 know whether there any golf course is around where you are, but some

32:52 . No, there was one, they closed it down, but we're

32:58 close enough to hear it. I think. Okay because normally they've got

33:03 big horn that blows. It says the golfers you get off the golf

33:08 . It turns out that the believe it or not, there are

33:11 lot of people who hit by lightning year in the US. And

33:17 The statistics, I saw some time that 30% of the fatalities of lightning

33:23 were actually men on the golf So it, you know, the

33:31 courses are often flat, There's nothing on the fairway. You're the highest

33:37 . What the lightning wants to do just connect the easiest way. So

33:40 got a huge battery up here on ground and it's trying to connect to

33:46 so it's gonna discharge in the easiest possible. And if you are carrying

33:50 bunch of lightning rod golf clubs in middle of the fairway, that that

33:57 un good. So, um, , that's one of the big

34:05 the record. There's a guy who's struck by lightning seven times that's in

34:09 Guinness Book records, I think he's most struck guy in the world who's

34:13 around. He's a he's a ranger the up in colorado, one of

34:20 mountain ranges. And of course he's there all the time. He's lightning

34:24 the time. And he gets caught myself as with some guys scrambling in

34:30 Iraqis and we're close to the Beautiful day. But we could see

34:34 weather coming in and we started to funny, Your skin starts to feel

34:39 of funny and then the hair starts kind of stand up and then we

34:46 , oh we wanted to get to summit but it's getting kind of funky

34:52 then we could hear things clicking, could hear our packs kind of

34:56 Well maybe it's just the, the melting in the rocks. But then

35:00 would go like this and little sparks go between your fingers. Seriously.

35:06 when that started to happen, we , you know what we're gonna have

35:09 bail and get out of here. , so because there's been a professor

35:15 electrical engineering that had actually been unfortunately from the university University of Calgary.

35:20 I thought you know, I teach safety and if I get killed it

35:25 be really embarrassing. That would be , really embarrassing and hypocritical. So

35:32 very very hypocritical. So I better die this way or try not

35:37 So we bailed off the mountain and enough, a big storm did come

35:41 but that is this battery inducing a . And if that field gets strong

35:48 , of course lightning connects. There's spark. You want to be in

35:52 way. So back to our a . Um If there's fluid in the

36:00 then it's hard to compress the If there's gas in the rock,

36:03 easy to compress the rock and that the velocity. So you can see

36:09 that just our standard parameters. This kind of the compressibility of the rock

36:14 here's the rigidity of the rock, was shear wave as the shear waves

36:25 through the material. It's just changing shape of the material, not the

36:34 . So in some ways the shear is easier. It's just starting the

36:41 now because it's starting to shape as can see uh if I start the

36:47 . So I get this triangle and the triangle over there. The shape

36:51 different but the volume is not. the shear wave doesn't distort the volume

36:58 it doesn't distort the volume. It largely feels the matrix. It doesn't

37:05 feel what's inside the porosity. Unless in the porosity is extremely viscous,

37:13 which case shearing it is felt. you can imagine if there's fluid in

37:18 and I change the shape just like talking about if I've got fluid in

37:21 balloon I can easily change the shape the balloon. I can't change its

37:25 size but I can change the shape . So it offers no resistance to

37:30 change. So the fluid and the do very very little to the rigidity

37:37 the matrix. So the shear wave really feel what's in the pores because

37:44 has no rigidity. So there's the wave velocity just depends on the rigidity

37:51 the whole material. And because the and gas, if they're in a

37:57 have any rigidity, they don't make change now, where they do change

38:03 a little bit is you can imagine the density of the material. So

38:11 back to Tanya's fluid substitution, if put gas in the rock that will

38:20 the density fluid of course makes it dense gas makes it less sense.

38:26 surprisingly, you can see here if put gas in the rock according to

38:31 density. Do you expect the shear velocity to go up or down?

38:37 we replace fluid with gas, would expect the shear wave velocity to go

38:42 or down? Just from the equation , I'm like thinking um it would

38:53 down. No go up. So if we're replacing fluid with

39:05 we're making the material less dense. surprisingly, it puts less dense in

39:14 terms, the shear wave velocity goes . So if we go back

39:34 we might say that the p wave should behave in the same way.

39:39 if we replace fluid with gas and density goes down, the p wave

39:44 should go up, but it Why is that? Um Just for

40:08 equation, we said, this is smaller, density is getting smaller.

40:12 in principle you'd say, well that make this get bigger. We said

40:17 the rigidity doesn't really depend on the because it has no rigidity.

40:25 our observation is that when we put in Iraq, he goes down,

40:31 said this term should be driving it . So the only thing that can

40:35 is this term sort of the compressibility the rock. So when we put

40:44 in, we said, gas is to compress. So if I squeeze

40:51 rock, it's actually easy to squeeze rock with gas in it. That

40:56 that Lamaze goes way down. So is getting smaller and is driving the

41:06 up, but only a little little compressibility is going way down. Lamaze

41:14 . The primers going way down because easier to compress the rock of gas

41:19 it. This is going way down the velocity drops so this guy is

41:25 smaller but this guy is getting way so it wins. Okay.

41:35 something that I've struggled with so far this program being by myself, I'm

41:40 bad in the spot and I am spot. So it's been it's been

41:47 hard for me because I'm not I'm dumb. It just takes me a

41:54 . No, it's really easy when asking the questions, it's way harder

41:57 you have to answer the questions. , very much so. Yeah.

42:06 Yeah, well no, there were any enormous hurry so take your

42:11 It's really just to um to interact make sure that you're not getting overwhelmed

42:17 the stuff that you've got some time think about it and um yeah,

42:23 hard to be flat on all the too. No, I find it's

42:35 same thing. Even when lecturing or , if you are being asked questions

42:40 , you're kind of in the same that you've got to think fast as

42:45 as you can on your feet but it comes to doing calculations um I'll

42:50 right to the board and do the simple basic calculations because most of us

42:55 do calculations on our feet fast and . So I'm gonna write down distance

43:02 time distances. Do do it seems , but I'm trying to do this

43:07 real time and I don't want to it up for sure. Good.

43:15 , so that's just some again, mental aerobics for the morning. Just

43:20 remember a little bit about the rock and when we do log analysis and

43:27 talked about saturation. Of course this all the story. So once

43:32 just to to think about the simple of the ultra sonics that we can

43:37 on these core, whether they are core or actual core, we're just

43:44 the ultrasonic transducers. The let me if I can put this on a

43:52 different screen. Love me. You what? I'm gonna maybe do that

43:59 the break. Um So once you can see that there's just a

44:07 created transmits. Now if we measure kind of material, the vertical or

44:14 P wave arrives pretty fast, but can polarize or if I'm generating a

44:19 wave, I can have it in direction or another direction. And it

44:23 out with these materials, if they're ice, a tropic are not the

44:27 in every direction, then the arrivals slightly different. So if I'm shaking

44:33 material up across the betting or parallel betting the waves travel in a different

44:43 . So the shear wave velocity is dependent on how we vibrate the material

44:49 that's called anisotropy the very simple way think about that is imagine a set

44:56 bad springs. And for every node one bed spring that's like the springs

45:06 a car that's very stiff. And in the other direction I have another

45:10 spring, that's kind of a soft . Then the other direction they have

45:13 bed spring that's kind of intermediate So you can imagine those bad springs

45:18 a node altogether have different values. when I whack it this way and

45:25 wave goes through, you can imagine different springs it travels faster the softer

45:33 when I whack it, the wave through but it's traveling a bit slower

45:37 this is really the basic concept of Satrapi in Iraq that it's we imagine

45:46 rocks just all these nodes and springs put together and you whack it and

45:49 just waves that go through it. the P wave depending on the

45:53 will go one speed depending on the strength. The sheer wave same

45:58 it's going to depend on the strength the spring as the wave propagates

46:01 And so that is what we find real materials rocks. So if we

46:06 a P wave through this way or way or this way um the velocity

46:15 a little bit because in fact the or the mechanical properties of the rock

46:20 slightly different. So that that's the it did to understand and I Saki

46:24 me, it's just different spring strength that's easy to think about. And

46:29 the wave going through those different spring travels a slightly different velocity. So

46:39 again in a in a real lab , we've got the transducers and we've

46:45 a rock sample. I'm just gonna the transit time through it. It's

46:49 pretty basic measurement, but it's the . We need to calibrate our sonic

46:55 and our seismic because that's what our waves do. So this is just

47:03 up a core barrel transducer, one transducer, another rock sample, and

47:09 this is going to be put inside tube that can be pressurized. That's

47:16 all the seals are here for. that we can put fluid into the

47:21 and we can also put pressure on rock to simulate the reservoir conditions.

47:29 , here's an ancient photo. we've put the rock inside this pressure

47:37 or pressure bomb this vessel, we introduce fluid into the corner to saturate

47:43 core and then we can pressurize outside core to simulate the depth of the

47:51 reservoir. So, in the what you're typically trying to do is

47:55 something fairly simple, but then try make it perform at its actual reservoir

48:05 . So we talked about temperature if down 10,000 ft 3000 m, that

48:11 the rock is gonna be boiling So if we want to find out

48:18 the rock is like reservoir conditions in lab, I have to be able

48:23 boil this the inside of this pressure which we do and then we have

48:29 pressurize it up to thousands of S. I. Pounds per square

48:37 . And we said that Down at ft if the fluids at a.

48:46 . S. I. Per foot were up and around £10,000 per square

48:52 . 10,000 P. S. Well what does that mean? Have

49:00 ever put air in your car I mean I make my husband do

49:05 . But yes I'm sorry I'm not all sexist. But that's a guy

49:13 . I do things for him. does things for me. Um So

49:19 he's probably and you probably helped him first time to make sure that the

49:23 could do the work. You're pressurizing tires somewhere around 30 or 32 40

49:33 . S. I. Pounds per inch. That's sort of a

49:37 like women's within a bicycle. Uh is gonna want their bicycle tires pumped

49:43 one of these days. And so gonna pump that tire up to around

49:46 or 60 P. S. A scuba tank. If you're gonna

49:52 diving underwater, might be 1500 high air. And then as we

49:57 the reservoir deeper reservoir is gonna be . So you can imagine that that's

50:06 hundreds of times higher pressure than your your car tire. So the the

50:17 are really really high. Here's another modern setup so we can have the

50:24 the core under reservoir conditions, high high pressure and then be measuring the

50:31 of the core permeability. Um Maybe of the magnetic properties. Dielectric

50:37 So all these things than in our . You know we can measure just

50:45 the bench top what's called if we're doing everything at at standard atmospheric conditions

50:52 called bench top bench top measurements. we're just under atmospheric pressure atmospheric temperatures

50:59 we can do that. Or if go over to the petroleum engineering they

51:02 this huge lab where again we can reservoir conditions. And this was us

51:14 days ago visiting the petroleum engineering lab they've got a bunch of these pressure

51:22 . You can see the pressure vessels here where they put rock samples,

51:27 them to reservoir conditions, temperature pressure then they can saturate those with fluids

51:32 gasses and then measure the acoustic The P. And S. Wave

51:41 . So they're they're actively doing that now. What are interested in is

51:46 current experiment is to put CO two dioxide in the rocks to simulate um

51:53 which a lot of the companies are in. Of course there's uh for

51:57 last 20 years we've been hearing a about C. 02. So we

52:01 want to store it in rocks and best way to do that is probably

52:09 depleted reservoirs or saline deeper formations. people have been talking about storing co

52:20 in in salt domes too and that's of what we want to look

52:27 Uh The volumes have to be really but it's conceivable in some of the

52:34 domes you could store C. 02 pretty high pressures and store a lot

52:39 it. So that's that's one of ideas. Uh We'll be lucky at

52:44 . So here's Mike Myers and Laurie and his wife, they both they

52:49 have various instruments there. So what we do? We've uh we're gonna

52:57 the rock in. This happens just be some of the happens to be

53:00 of the core. We're working on core and then most of the time

53:04 put it in you put higher pressure can see we're going up to 4000

53:08 . S. I hear and then look at how the velocities change.

53:14 that's a classic measure. Oh Well we've been almost an hour so

53:21 don't we take 10 give it a break and then come back at around

53:26 , 10 or so. Okay great . We'll see you shortly. See

53:32 tie we'll see you in a Okay we were going over some of

54:28 tests which are really just personally for how the how the measurements were made

54:36 what they give us and for with salt, you can see we're

54:42 the salt under pressure in the lab measuring the transit time of waves across

54:48 , knowing the length of that transit , we get the velocity. So

54:52 we've got the velocity of salt in lab as a function of pressure,

54:58 . And again, once uh we do the same thing with temperature in

55:03 case, we're heating up the rock and measuring the shear wave transit time

55:11 it. And you can see as get the material hotter and hotter.

55:14 takes the waves longer and longer to through it and then we pick those

55:18 then look at the velocity as a of temperature. Now in these oil

55:28 , the reason we want to know is because we're going to be injecting

55:32 into them in the field and we to get the oil sands up to

55:39 pretty high temperature to melt the bitumen to produce it. So we'd like

55:44 know when we inject the steam, hot is all the settlements. So

55:48 going to be doing surveys on top to extract the velocity and from the

55:54 if we get a velocity of the , then we're going to say that

55:57 corresponds to a certain temperature and then gonna create a temperature map of the

56:04 . So you can see that all is really based on lab measurements and

56:08 how does this material behave that sitting and temperatures in this case temperature and

56:14 we're going to make a seismic measurements the surface um which ideally is is

56:20 . We can't drill the hole We're gonna measure from the surface and

56:23 where the steam has gone and then how to produce the vitamin. So

56:29 an example of where these measurements would useful. Then we measure the p

56:36 velocity, the shear wave velocity. it turns out that that maps two

56:43 rock types. So now we can a measurement and then map that to

56:49 that we want, which is typically type. So in other words,

56:54 world doesn't really care that much what shear wave velocity of and hydrate

56:59 But we do care about making a that's inexpensive. That gives me a

57:04 . That is useful. So I a velocity number that's got a value

57:12 that value means something about Iraq. that's good. Um We're mapping our

57:18 to a property of interest and you see that for example, there are

57:31 of all kinds of different rocks and properties as a function of temporary

57:36 But here's an example, say just salt. It it has a velocity

57:42 4600 m per second. So 13 ft per second for the people the

57:48 , it's very light. For you probably remember that most courts the

57:58 zero porosity courts just pure silicon dioxide 2.65. So if we've got a

58:08 primarily courts, it's gonna be 2.65 per cc. When we introduced ferocity

58:18 that granite. So break it make it into a sandstone and then

58:25 with gas or water. The or , the velocity decreases a lot and

58:32 density too. Okay, you can that just down the road of

58:43 oil is generally less dense than water . So it's like if you if

59:00 have a solid and you wash the and the lettuce still has a bit

59:05 water on it and then you put oil and vinegar dressing on it.

59:11 your favorite dressing Stephanie actually do like balsamic, like oil and vinegar.

59:18 you go. So I don't want ruin it for you, but I

59:22 help. But when the, when lettuce has been wet, you just

59:25 it or you're making the salad, you boil, pour your balsamic vinegar

59:30 top. Does it go to the or does it float on the

59:35 I mean usually the lettuce just doesn't like balsamic because it's too wet so

59:39 just lets go of everything. It's at the bottom, it's at the

59:44 . But if you look at the on the bottom of the plate is

59:48 is the dressing underneath the water? it float on top of the

59:52 Can you see that? Yeah. that, to me is the first

59:58 , you always know that oil floats water. It's from salad and pouring

60:03 favorite dressing on it. So you , you can maybe try and put

60:08 water on a plate and then pour balsamic vinaigrette and just watch it float

60:13 then you'll never have trouble remembering what density is. So generally are 32

60:22 A. P. I will talk the smart generally the oils that is

60:26 oil, 30 40 degree api nice light crude floats. Its density

60:33 1.85 g per CC. And so , the oil floats on water.

60:43 oils can actually sink some of some of them are more dense than

60:51 . But those are, again, are the vitamins in Canada or Venezuela

60:56 some other kind of degraded soils. they are, they're tari, they

61:01 are thick heavy oils in this, this case it's more like the oil

61:08 you'll see on tarmacs when, when roads are being paved, there's sticky

61:18 that's in the, in the asphalt the asphalt themselves. The asphalt teens

61:23 actually very heavy. So the mix that asphalt is probably slightly heavier than

61:32 . So asphalt would would sink. Okay, so just again, getting

61:45 rock properties in mind. Now, we, what we think about the

61:50 , a very simple way we think the rocks, especially geophysicist. Um

61:56 depending on your background, you probably a fair amount of geology. Many

62:00 have not had that much geology and also Petrakis is the, well loggers

62:08 of the rock in some ways, fairly simple terms because if we think

62:12 it in the way the reel rock in a thin section, then it's

62:17 to get anywhere to describe it. we're gonna simplify it and the simplifications

62:24 correspond to our measurements. So we're going to make the rock as complicated

62:29 really we can measure it. So thinking kind of from the way of

62:34 got to make a measurement in this . What's the model that can explain

62:38 measurements? And those models are often simple. They're not as complicated as

62:42 real rock but for our purposes they it to a degree. I don't

62:50 care what the rocks like. I want to get something from it.

62:54 that's the economic you. So um the here's the standard rock model that

63:02 a geophysicist or a Petro physicist or well longer you'd be thinking of.

63:07 imagine that was of course the matrix and that can be composed of a

63:10 of stuff and a lot of different types. We've got porosity inside that

63:17 got or space that has no matrix and in that poor space we imagine

63:25 there are fluids or gas and then you might remember what's the most in

63:37 whole sedimentary column. We've got rock , we've got carbonates, we've got

63:44 and we've got clay materials, mud in the whole world, in the

63:49 column. More or less. What's composition of the of all of our

63:56 ? Do you happen to remember um just of the sedimentary rocks like do

64:07 mean like sandstone, sand stones or or mud stones shells, which is

64:13 most popular? What's what's the percentage the of the sedimentary column? What

64:21 ? Carbonate sands or shale play I I don't remember but I want

64:29 say it was more more of the . I'm not mistaken. You

64:35 in terms of in terms of a lot of the reservoirs are actually

64:41 , reservoirs, petroleum. But it out that about two thirds of all

64:47 sedimentary rocks on earth are mud their sales or something she'll like.

65:01 it turns out that 60 65% somewhere there, all of the sediments on

65:11 , our mud stones, so And we've got a lot of Sandstone,

65:18 another 20% or so. And then a little bit of salt and then

65:22 carbonates. So mud stones, sands carbonates and then some salt, some

65:37 , but because there's so much clay mud stone that we kind of assume

65:46 there's a little bit of clay, stone shell in all rocks and so

65:53 it's kind of part of the, imagined simplified rock, we've got a

66:00 carbon age, sandstone or whatever, we've got a little bit of shale

66:04 there someplace or play and then we've the ferocity. So that that's kind

66:14 the thinking the simple model of the most rocks are expected to be.

66:21 that's our little model. Um It's straightforward, but it also leads us

66:26 all the log analysis because now when imagine the models that way we make

66:31 these measurements and we try to understand measurements, we're gonna understand the measurements

66:36 that kind of thinking, with that of model in mind. So once

66:42 we imagine that we've got the rock the matrix, carbonate and hydrate,

66:48 , whatever it is and then I've some holes in it, I've got

66:51 ferocity, some voids, Those voids going to be full of clay or

66:58 , gas, food. So that's simple idea. Um then in the

67:08 itself or in the porosity it could connected or not connected. And so

67:14 are a lot of different definitions, you're a Petro physicist, a geologist

67:18 about what's effective for our purposes, effective porosity is connected or floatable

67:30 You know, if it's got clay it and the water or the fluid

67:34 attached to the matrix then in a , I I'm not interested in it

67:40 I can't get it. So two . That's that's our that's our rock

67:52 . This is kind of the basis almost everything we do in in applied

67:57 . It's this idea. And then remember that when we're trying to calculate

68:06 , we can have an even simpler . We can just imagine that all

68:10 matrix material is, say spheres and we put all those spheres together and

68:17 the least contact that we can have all the spheres if they're in contact

68:24 to just have have them touching this , not to be packed, but

68:29 is the most ferocity we could have spheres that are touching. And if

68:33 do the calculation just with the sphere being 4/3 pi r cubed. And

68:40 the porosity is what's left. You see that the the void or the

68:47 the volume between the spheres in a cube Turns out to be about

68:55 So with this really simple, extremely sphere pack, we can have that

69:03 voids are almost half of the total . And we imagine that with with

69:11 matrix that's actually continuous or in contact about as porous as it gets.

69:17 we tried to make it more for , then we'd have a suspension.

69:21 spheres would be in a fluid hanging the fluid and not in contact with

69:25 other, which is a suspension. that could, in a sense,

69:30 greater ferocity. But now we're really a fluid with floating spheres or with

69:35 spheres. So that's not really a . So once again, the with

69:42 very, very simple material with a that's continuous. It could have up

69:47 something like 48% porosity. That's the highest we can imagine. So,

70:01 again, real rocks, a Sandstone have 30% porosity carbonate, which is

70:06 going to be less, maybe 10% . And once again, in the

70:13 schematics here, we can imagine that got sand grains, some kind of

70:19 carbonate of some kinds of holding the together and then we have the interconnected

70:25 the floatable connected porosity, which we'll effective in this case. And then

70:32 or clay stuck ferocity that we can't the fluids in and out. So

70:37 can see the total porosity is 30% this case Usable interconnected or effective porosity

70:44 save 25%. The, the isolated the non connected or the clay bound

70:56 stuff might be a few percent. reason that we separate these is that

71:04 of the measurements are gonna give us porosity and some are gonna give us

71:08 effective porosity and when we're calculating we want to know what's our usable

71:14 effective porosity mm, they're not gonna too different. This is a bit

71:20 a detail. So imagine we're just with ferocity in general, but there's

71:25 different characteristics of that ferocity. And we can have really, really serious

71:34 uh in carbonates. The one the of the left happens to be in

71:40 carbonate that has had some glacial And so they're they're rivers that have

71:47 through the carbonate, they dissolve This is kind of car stick,

71:50 called karst topography where fresh water dissolves the carbonate. And the uh the

71:59 in red was our guide actually, had been formally one of our geology

72:04 , but then she went full time a as a spill geologist, as

72:10 as a caving tour guide instructor. we were down and repelling into one

72:18 these caves. Incidentally was kind of , it was a mixed group with

72:22 . There was half guys and girls in, but it was fairly challenging

72:27 . You had to repel down some and then there were tubes to go

72:30 one called the birth canal, which , you're probably familiar with the poor

72:35 babies trying to get through that. this is actually uh actually a rock

72:40 you got through. So we were a cavern having gone through this and

72:47 were about four guys who came in different group after us and they were

72:51 freaked out. They were not happy being in that cave and going through

72:54 canal because they were they were pretty guys. And it turned out that

73:00 were s a s they were british forces guys and they were training to

73:07 shipped off at the time to And these guys were all brits.

73:12 never been in caves before and they learning how to get through caves and

73:18 able to operate in caves and they freaked out. But they did

73:26 So we I think we Liven them because when they got through this canal

73:29 were there was a mixed group there we were all having fun and they

73:35 felt better to be not so freaked because uh if we could do it

73:39 could do it. They were supposed be tough guys. So that was

73:43 . There are lots of caves, might have been in some of the

73:46 in texas. Have you Stephanie? Yeah actually for my honeymoon me and

73:52 husband we did like a whole like of like the hill country. So

73:56 took him to Long Horn cavern and stayed at the what is the Eagles

74:03 of the Eagles or whatever. Um Burnett. So it was really

74:06 But yes I've been a longhorn like or six times at this point I

74:11 . Yeah. Nice. Have you to, there are a couple other

74:15 that are pretty nice with the natural caverns. It's near, yes I

74:20 it's been years but my grandfather would me when I was a kid.

74:25 it's a it's a beauty um where we recently? Oh yeah we just

74:35 down to, we're down just south Cancun near to loom and of course

74:40 the yucatan peninsula is a big limestone . We went into one of the

74:47 , we've been in some of those before. But this cenote, you

74:51 go in and it was half full water and you could wade swim inside

75:00 , inside the cavern. It was was really beautiful and especially when you've

75:04 just flashlights and the water was just clear and you could you could see

75:08 was really pretty. So. Oh . Yeah so you've been in some

75:12 these caverns, Major porosity. Yeah longer is nice because they're they're really

75:22 friendly there and they we did one the field camps there too and they

75:28 us make measurements, we scanned inside cavern and uh did all kinds of

75:34 , we simulated the tie kids You remember were those, that was

75:40 soccer team, the kids were in cave in Thailand and they were trying

75:49 figure out how to get these poor out of there that had flooded?

75:53 they went in and then it flooded couldn't get the kids out. It

75:58 interesting on a couple of counts. been over there many years ago and

76:01 up the geophysics program in the university Chiang mai up in northern Thailand so

76:05 were kind of familiar with some of areas and and then it became a

76:12 of a geophysical thing. Where do do you, how do you locate

76:15 they were? So when we were this longer and cavern, we tried

76:20 same things, we tried setting a seismic array on top of the cavern

76:26 then we had people thump the side the cavern to see if we could

76:30 them and we could we could see to a degree. But it's a

76:37 a pretty challenging problem to locate people the subsurface. So anyway, but

76:45 a ferocity. So we imagine that porosity for our purposes in the rock

76:53 full of some fluid and gas. again very simply we imagine that there's

76:59 or water, gas and oil and sums up to 100% or 1.0 depending

77:06 using fractions or percentages. So that's simple model. Now again with the

77:16 the water itself, freshwater or drinkable has a lower amount of dissolved solids

77:26 or salt brackish water is typically a of saltwater, marine water and fresh

77:33 . So in estuaries and other river that are going into the ocean or

77:38 gulf and then saline water is really type water and then we get into

77:47 that are in the subsurface. And imagine that everything in the subsurface is

77:52 saturated in general, maybe not in top couple the top little bit,

77:58 everything deeper is full of water or special cases. What? So we

78:08 those special cases, but this is the, the saturation And you can

78:22 when you get brines that have 100,000 per million. That means if uh

78:29 I had this cup, which I don't know, maybe 200 I'd

78:38 putting in um a bunch of cubes salt, like two or three cubes

78:46 salt into this cup. And that be brian, extremely salty. It's

78:57 if you're a wine drinker, there's , there's a number that's a little

79:01 associated wines are generally given a number a very, very dry wine or

79:07 , very unsweetened wine is a there's effectively no sweetness or no

79:12 a very sweet wine that you might had like Moscato or some something would

79:20 be a five. So five is pretty sweet wine or some some of

79:31 really, really sweet red wines, a four or five, that's a

79:36 sweet wine. But what does that mean? Um we've had ice

79:41 I was in an ice wine vineyard and ice wines come from when the

79:45 freezes and when it freezes it it kind of becomes like a raisin

79:50 then after three nights of a full . The rule is you get to

79:55 the grape and then you ferment those , but the sugar gets really,

80:00 concentrated when the grape freezes. So pick those, you ferment them and

80:06 becomes a very very sweet wine. wine. I love it called ice

80:12 . Ice wines are really delicious before have to try that. Yeah,

80:19 some ice wine, others. So you like wine there's it's really really

80:24 . You know, they sometimes go the name of dessert wines. A

80:30 ice wine has to have had the frozen hard for three days. Dessert

80:34 can just be really sweet. But true ice wine, there's a kind

80:38 quality control like champagne or V. or different control. So you have

80:44 hard freeze it for three days and it's picked and fermented but it's so

80:51 . Uh So from upper new york , lower Ontario also. Um far

80:59 , maybe California, California doesn't do many because it doesn't freeze that

81:02 But there might be some ice wine California, british Columbia. And Canada

81:06 the has a lot of ice wines . But there Their rating is around

81:16 . So they are so sweet, just you just want a little little

81:21 almost like a shot glass of ice . It's so sweet and it's so

81:25 , so good. But it's rated 25. And what does that

81:30 That means that there are 25 g sugar per 100. Oh wow.

81:39 you think that a normal and typically wine comes in a smaller bottle,

81:43 in a thin bottle. So our bottle of wine is 750 mils,

81:51 . Ice wine usually comes in a about a third that size around 200

81:56 because you don't drink very much, it's just so sweet. But what

82:00 number means is the number of grams sugar per 100 millimeters. So you're

82:08 dry red wine of one or two two g of sugar per 100

82:14 So you've got something like 10 or g and a full bottle, a

82:20 bottle of ice wine, you've got g of sugar. So 25 cubes

82:25 sugar per 100 millimeters. And this cup is maybe 200 millimeters.

82:31 this would have 40 40 sugar cubes it. So, but it is

82:40 delicious, you just want a little of it and it's very satisfying.

82:44 , but for us, it's one of those measurements, like groundwater

82:50 , it's the number of grams of mint in a certain amount of

82:57 So ice wine would be 25 250 g/l. So yeah, ice

83:14 is to wine and sugar and wine the same as brine is to

83:21 So ah, if there was a and there is a brightness rating.

83:29 not sure what it is, but would be something like the sweetness for

83:33 . But you can see that brian 100 g per liter. So that

83:41 10 g per 100 ml. so in a sense, ice wine

83:49 twice as sweet as brine is We'll have to remember that. I've

83:58 done that before. So that's um bright is very, very salty and

84:10 we, we've been through this before you just want to remember all

84:14 all these conversions just so that you kind of banding these around um when

84:19 working in the, in the industry I'm sure in your chemistry there are

84:23 lot of different numbers that get bandied . But in the oil world these

84:28 go back and forth. Um An friend of mine was actually a natural

84:35 trader. And ah in a sense might think, well that's, that's

84:43 of the marketing fluffy end of, the oil industry. But I think

84:49 made more money than all of us together. So I don't know where

84:55 fluff is. But because what happens of course people are, we're finding

85:02 oil and gas then of course it cleaned up a bit and put in

85:10 and then sold. But often like , it's the actual person who makes

85:15 transaction, the seller who makes the money. It's a little bit like

85:23 realtor, you know, in in a sense, you may have

85:30 your place up in the Woodlands. you end up renting or buying a

85:34 up there, Stefan, we actually in with my parents to get help

85:39 the baby while I'm in this But we'll say I'm renting.

85:45 Well your parents would have bought the . How long have they lived

85:50 They've lived in this house for about years. Okay, well they may

85:56 bought it in which case they may bought it from a friend or something

86:01 they knew. But if they bought through a realtor, do you know

86:04 the realtors charge to? My mom actually a realtor. So I know

86:09 like It's like 6%, but then actually 3% because it's divided here.

86:15 then it's less than that because it everywhere else. So, so in

86:21 sense now it might only be one of 10 contacts that she actually ends

86:28 closing a deal on. Yes, very difficult and it's pretty difficult.

86:32 so of course you have to wait in when you do close the deal

86:36 you get 6% in the 1st 100,000 or something like that or whatever it

86:41 . And then there's a bit often gradation scale. So Maybe on the

86:46 few 100,000 bucks, it's 3% or . However it is. But,

86:51 still you can see that the trader a sense, the realtor, if

86:55 sale is easy, it's pretty good . Um, a lot of sales

87:02 easy and there's a lot of disappointments from the realtors point, a couple

87:05 good friends of either realtors, they do work for their money. But

87:11 you make a sale it can be pretty good sale. If you sell

87:13 million dollar house, that's pretty, a pretty nice day. So likewise

87:22 trading oil and gas futures and anything like that that the traders can make

87:30 fair amount of cash. And but where we're going is they need

87:36 , they bandy about it have to exactly the units and they're working in

87:42 fractions to sell big contracts. So what people talk about there is 1000

87:48 feet of gas. That is a quantity, but it has an energy

87:55 which is a G J or a jewel. Then way back again.

88:01 the units that we talked about. , the roman numerals, 1000 cubic

88:09 . In the old roman numeral way the capital, M. C.

88:12 . 1000 cubic feet or a million thermal units. Mm BTUs. So

88:20 are all these units in the metric , they're probably going to trade in

88:24 . J. S or meter cubed oil or tons But be a little

88:30 careful because a us ton is £2,000. metric ton is 1000 kg. What's

88:43 kilogram in pounds, isn't it around , it's like two point two or

88:55 . Yeah, that's exactly right, one. So if you go to

88:59 market in your I don't know, would have I don't know in Mexico

89:06 you were buying food in Mexico, you know, are they, would

89:11 sell vegetables or fruit by the kilogram by the pound? I honestly have

89:18 idea. I think they probably I Mexico is fully metric. So Kennedy

89:29 if you were buying fruit or something Canada, you would be buying it

89:32 the kilo kilogram. Um It says uses the metric system. Yeah.

89:42 I'm sure in the markets you're buying does too. So it's still a

89:49 bit mixed, people are still gonna to buy a pound of butter and

89:54 probably how it's sold. But we sold as .45 kg or something like

90:01 . So you can see the The here for us, a barrel of

90:09 is energy equivalent to about 6000 cubic of gas. So These trade differently

90:20 buy energy equivalent oils, 80 so I think what did the clothes yesterday

90:28 ? But oil is traded actually all time. So I'll have to look

90:31 my my phone, but it's somewhere I think 7 75 bucks a barrel

90:35 now and that'll be West texas intermediate that probably sold at the Oklahoma hub

90:47 that's the price for next month's barrel oil. Mhm. Um So oil

91:02 out 75 bucks I think, I gas is, I don't know,

91:06 bucks an M. C. So Multiplied by six. You

91:12 gas is trading at maybe 20 bucks barrel and oils at $75 a

91:16 So for energy equivalent gas is really . That leads to all kinds of

91:23 things. # one, it gives us a big advantage for manufacturing because

91:30 is cheap and you can use it heating for materials, for hydrogen for

91:35 kinds of stuff. And so when gas is plentiful, it's way cheaper

91:40 oil. And so that's that's a thing for gas producers. Incidentally in

91:46 political sphere, we think, it's great for the US to develop

91:51 terminals, liquefied natural gas to So the U. S. Is

91:54 of the biggest exporters of natural gas . But that had to change the

92:01 lot of the laws because going back the oil embargos in the 70s,

92:06 us put in laws that it couldn't oil and gas was to keep the

92:12 market supplied. But of course, domestic market, the US started producing

92:18 oil and gas than it sort of , at least in certain areas.

92:22 it was a big big logjam to be able to export. That was

92:27 course, in our opinion, my , very bad for the country because

92:32 U. S. Could not export and gas. Well, the law

92:36 a few years ago and allowed the to export natural gas and oil.

92:41 so now the big complexes like seniors the saving passed not too far from

92:46 . Freeport the U. S. building big L. N.

92:50 Terminals to expert, which is But believe it or not, there

92:56 a lot of the big chemical companies the US that fought against allowing the

93:02 to export. Why would they do ? Mm. I'm sure they probably

93:16 money in it somewhere else or I'm not sure. Yeah.

93:22 the idea was that the chemical companies cheap gas coming into manufacturer, that's

93:29 input cost. So they wanted it be kept plentiful and cheap. And

93:37 exploration and upstream companies could export, thinking was that's going to make the

93:44 more expensive because there's another market for . There are other buyers bidding for

93:49 . And so a few years ago actually tried to shut down. Not

93:54 experts in my opinion. This is bad and it's false economics because when

94:05 allow more exports, you get more , we can employ more geophysicists and

94:10 looking for oil and gas and producing . And when you allow the

94:13 ultimately, your building in surplus, will supply the domestic market. So

94:19 thought they were victims too very bad thinking. They thought it was in

94:25 interest to restrict experts. But it's really. So when you allow

94:31 it stimulates activity and when you stimulate , you make more fines. When

94:34 make more fines, you've got more , so allow experts. Okay,

94:42 that was a big deal. the, that I think more appropriate

94:47 thinking one and exports are allowed. especially right now with the poor Europeans

94:54 are struggling with no gas because rightly restricted Russian gas. The U.

95:00 . Has come to the, to salvation by having excess experts. So

95:08 stimulating the oil and gas industry, allowed us to supply our friends in

95:16 . So that had to be because were allowed. Okay, so here's

95:22 of the numbers. The background for . The other aspect is that,

95:28 know, we're proponents of science for of all kinds of energy. I

95:31 am, but you've got to be to that. Oil is such a

95:36 energy source. It's just hard to it. Its energy density is way

95:40 than batteries. It's uh, energy weight for volume for anything is way

95:45 than almost anything else outside uranium. you can see that even a one

95:52 wind turbine, which is a modern winter line is equivalent to about five

96:00 of oil per day, which is small. That's a stripper.

96:04 so a big honking wind turbine is very, very small stripper, man

96:12 well, So when you want to up wind turbines say, an offshore

96:23 in the Gulf of Mexico might be 50,000 barrels of oil per day.

96:29 need 10,000 wind turbines to be equal one offshore platform. Well, I

96:35 wind turbines. I invest in wind , but uh 10,000 wind turbines hasn't

96:42 been done before And nobody wants 10,000 turbines anywhere near their property. So

96:51 have to be realistic about energy sources that there's a lot of discussion all

96:56 time. People say, we'll just in a bunch of wind turbines.

96:58 , you can, but they aren't to service Houston, You know,

97:05 , a megawatt wind turbine is something probably maybe, I don't know,

97:17 households. So if you want to Houston's two million households, you need

97:27 and thousands of wind turbines. So are okay, but not that

97:36 So we, we need this saturday . Okay, um let's just do

97:42 couple more minutes and then we'll take little break. Um we talked about

97:47 density, so the oil is often as a P. I.

97:52 It's again, a P. I the american Petroleum Institute, it's one

97:58 the calibrating or regulating our standards bodies represents all things with hydrocarbon. So

98:11 , they wanted a number to be to just quickly talk about what kind

98:15 crude oil it was. And this just kind of grabs, it directly

98:21 how dense the oil is. But um it indirectly says what's the what's

98:27 content of the petroleum? How easy it to be made into a few

98:33 them? So it's it's a it's weird it's a weird number. But

98:38 water. What's the specific gravity of or the specific density of water?

98:48 , one that's it. So if just put one in there, then

98:53 45/1 minus 1 31 gives you So the api gravity of water is

99:02 . That kind of divides again, heavy oils from lighter oils and it

99:07 what jurisdiction and everything. But anything than water is heavy as far as

99:12 goes. Again, some of the of the areas, even west texas

99:21 very light, nice, nice 30 to 40 degrees ap i it's

99:26 light by light means just density is . But that typically means that there

99:32 smaller length hydrocarbons in it and the the length CH four is just one

99:41 When we get into the Athens and pentagons and hexagons and everything goes get

99:47 to six hydrocarbon chains. And that is getting heavier and heavier all the

99:54 . So the uh that means that hydrocarbon chain is longer and more complicated

100:01 maybe a bit harder to break and with. So we want fuels that

100:08 pretty simple and easy to burn and have a lot of other stuff in

100:12 like nitrogen and sulfur and all So CH four, that's why natural

100:20 is so clean burning. It's very . You just, you know,

100:24 oxygen, you get carbon dioxide and and it's a very simple reaction.

100:29 burning methane CH four is really very clean, very simple. And

100:35 that's why people call it the cleanest the hydrocarbon burning fuels. Very simple

100:40 can be very pure. So um gas is quite good and that's what's

100:45 for heating all over the place. you start burning oil oil, it

100:51 longer hydrocarbon chains. It typically has lot of other stuff in it.

100:57 Again nitrogen and the sulfur Z. all kinds of trace minerals and metals

101:03 everything. And so burning oil per itself is a bit messy. That's

101:11 of course it's refined to try to it into a simpler material. So

101:19 like higher grade crudes because they're simple they're they burn well and that here's

101:27 a again, a set of basically 10 degrees A. P.

101:32 . Is going to be heavier, heavy, Then we get up into

101:37 40s and 50s, that's light crude we like that around .8 g per

101:53 . So if we if we really at again, just some of the

101:56 just kind of it as an example viscosity. You can see that the

102:04 yellow slide on the left, this be a high viscosity oil and you

102:08 see that's pouring kind of like So oil can be that thick,

102:13 would be uh fairly, fairly heavy . Um but when you heat it

102:20 the discussed these drops and that's why with these heavier crudes, you heat

102:25 up, the disgusting gets lower, you can produce them. So just

102:30 example that some fluids do have viscosity in fact, we can propagate a

102:37 wave through this fluid because it's so , it actually has a bit of

102:41 and it will support a shear Is that kind of like what the

102:47 the tar sands, oil at a would look like that. Super viscous

102:53 . Yeah. And even even more than this. Oh, wow,

102:58 , this has been, this has , this is uh this is victim

103:04 or oil sand, but this has heated to and and treated a little

103:09 . It's even more viscous than wow. So that's a little bit

103:24 oil, that's the fluid or the can get so viscous that they almost

103:31 a solid. And in fact, you cool this stuff down, it

103:39 is is is solid. If you , if you freeze the this oil

103:46 become solid. But when we think the natural gas, you can see

103:53 a saying the top part of the . If this is a gas

103:56 you can see what it is, largely methane. So maybe 80 or

104:01 methane, maybe a classic reservoir. then you can see that there's some

104:06 the higher order hydrocarbons that are still , the ethane, propane and

104:12 But if we pressurize them they can fluids and that's what's done with LNG

104:21 natural gas, it's going to be and then pressurized and that's what the

104:28 say in the saving pass not far here, just south of Beaumont that

104:32 the shinier plant, huge plant. an LNG terminal. So the cool

104:37 pressurize the natural gas put in these Dolman ships and send it off to

104:43 or south Korea or someplace incidentally in , off to europe, in place

104:48 Russia or South Korea. You I don't know what it trades for

104:54 now. But typically in Asia, . N. G. Might be

104:59 or four times the cost of the . S. Because of course you

105:03 to transport it there. But that's good market. And even right now

105:09 are lots of contracts being signed. probably saw in the paper the last

105:12 of days there are a couple of LNG facilities that are going to be

105:18 and they already have big contracts to their product. So here's what's in

105:24 reservoir and more to what you're doing that you can see that in a

105:30 natural gas reservoir, there might be sulfide in the reservoir, We actually

105:36 standards for like all of that. we do like methanol, we do

105:40 , propane, all benzene, like , all of that. So this

105:45 cool. I've never been able to like tie in what my company makes

105:50 anything. So this is interesting. , that's great. So this,

105:55 know, this stuff coming out of formation right out of the rock,

106:01 really important to characterize this because of the just for health and safety is

106:08 much hydrogen sulfide is in there and how much carbon dioxide is in

106:15 you know that all this stuff, the hydrogen sulfide especially, but there's

106:22 different price on all of these For example, propane, you're gonna

106:29 to your local gas station if you to do have a barbecue, you

106:34 , there's gonna be a propane tank or something or something like that.

106:37 going to fill it up, there be a certain price for propane,

106:40 be different from the price of And of course when the, When

106:48 filling up those propane tanks, you've to have standards there that says this

106:53 99% propane or whatever, the you should look up the stand,

106:57 be curious to see what your standards for various things. Um, but

107:02 out of Europe, this is the we get and then they're just multiple

107:07 built around all of those products, aviation fuel, how much butane is

107:13 in or your butane lighters? because from, from my understanding like

107:20 we do is like, like let's a company request uh a sulfur like

107:27 and methanol set, They'll want it like zero PPm to like 50

107:31 So they use what we make to their instruments to be able to use

107:35 out in the field. So are making the gasses or the instruments?

107:41 make the gasses and the oils. we do we do we do mostly

107:46 , we do like sulfur mineral oil do like chlorine, mineral oils,

107:51 of the different elements. So like gonna metallics with like calcium,

107:56 um everything really. So it's I just I'm not like super interested

108:04 it. Like we all make like gasoline standards, arsenic, gasoline,

108:09 stuff like that. So it's Yeah. You know what, I'd

108:15 curious to see all of those numbers in a sense they relate to exactly

108:22 we're finding. And then, you , in a sense we're on the

108:26 end that's producing this raw stuff and that that's gonna get fed into the

108:33 stream and the downstream areas, it's get separated purified and then you're it

108:38 like you make the standards to compare probably upstream products with what the downstream

108:46 . Yeah, I think so, you ever want to come visit the

108:49 , You're more than welcome. we tours all the time. Okay,

108:52 that yeah, that would be great get on the, get on the

108:56 . I'd like, I'd like to it. It's really nice to know

108:58 your products end up. We're exploring this stuff and we make recommendations.

109:05 don't even usually get to see where , whether it's drilled and produced or

109:08 . You know, you're as an , you're onto the next one.

109:13 that's why some people like working for companies because you get to drill

109:18 you get to see it go into pipeline and then ultimately, you know

109:21 the pipeline goes. So it's kind fun being in a small company to

109:25 get all the way from assembling the to organizing the drilling to getting it

109:32 the pipeline. Yeah, because we products all over the world. I

109:39 we do business with china Turkey and like Turkey, they request a lot

109:45 like chlorine and water standards for whatever or they'll do like solid, So

109:52 do like poly poly ethylene, like things with like mercury and whatever in

109:58 . Um but we like I'm the XRF technician, so I handle the

110:03 rays, but then we also have instruments and stuff like that. So

110:07 interesting. It's cool. I think , it's all first of all,

110:11 just interesting, but it's all good experience to knowing how to handle

110:16 knowing how to handle the measurements, data what they what they don't mean

110:22 because earlier when you were explaining with chlorine and like the different like the

110:28 fractions like that's what that's what my my machine does. It shoots it

110:35 the crystal and it measures like where rays are going to see what it

110:40 . No and then there'll be all standards that you compare it to.

110:44 you can say this is what the of the material is. Well we

110:48 know so we already know what it . So like the customer wants like

110:53 0.5 weight percent calcium mineral oil or that I I test it to make

111:02 it's within a standard that we can into the customer for their calibration.

111:08 that's that's great. So yeah again providing the calibration standards themselves. So

111:15 companies are going to compare whatever they're or using to your standard.

111:23 Oh good. Well um let's take couple minutes just as a break and

111:28 um okay get our brains reset, your legs so let's let's take five

111:34 then come back in a few minutes we'll go up to around noon.

111:39 sounds good. Okay great Stephanie. great continue on. And yeah normally

111:51 some of this composition stuff is a bit outside what we would normally be

111:55 about as geophysicists but you're right in thick of this So this is this

112:01 up your avenue. Yeah. I've been there for three months now so

112:11 don't know like a lot but it's . So yeah. Well you'll you'll

112:17 it maybe you'll hopefully we'll get back doing geophysics but you'll be probably better

112:23 about the product that most officers are to find than other than other

112:29 Yeah. Most people don't have that kind of standard. So I think

112:35 I think it's really really useful giving a different perspective than most would

112:43 So again, with these properties you see that and you will be dealing

112:47 some of this with with your Um Because they're gasses and standards,

112:52 have all these different properties at different and pressures. So you can see

113:00 of course that room temperature or slightly most of these methane, ethane,

113:06 and butane are still gasses. The order hydrocarbons of course are more

113:16 And our liquids at room temperature instead room temperature is is that's probably a

113:26 bit high. Room temperature is usually 20 degrees C or 68 70 degrees

113:32 . And um that's just the temperature which humans behave the best. That's

113:41 kind of the definition when we get little bit colder than colder than

113:45 we start to perform. We get and when we're hotter than around 72°

113:52 performance actually starts to fall off. I put this all together once and

113:58 up all kinds of statistics on how behave at different temperatures, so we

114:02 differently too. Of course when we hot we start to get irritable and

114:08 systems don't work very well. And we get cold we start to freeze

114:12 shut down. So the really operates operating conditions for us around 70

114:21 So, and we are largely not too much gassy at room

114:32 So here's the here's this definition of for you that condensate is when you're

114:37 the gas reservoir or an oil As noted, you've got gasses say

114:44 room temperature, but you've also got of these other liquids that we

114:47 the hexagons and things like that that liquid. So, coming out of

114:53 reservoir will be a great richness potentially products and and so those will be

115:06 and separated. And that's part of kind of the midstream or the midstream

115:11 to separate these fluids because they will different purposes for different industries and different

115:21 . Then, as we said, gas is uh more than 1% H

115:27 s. So you can see that saw that reservoirs could maybe be up

115:35 5%, that would be a heavy of H2S, for example, and

115:40 would be uh be tough and you're have to have a lot of special

115:45 and you can see that, that sulfur gets stripped off. And

115:50 once again, if you go down Galveston's, you'll see often huge piles

115:54 elemental sulfur just sitting there, great piles of sulfur that are getting

115:59 So a lot of that sulfur will from stripping it off natural gas.

116:07 then it's got to use because we're put that sulfur in fertilizers and there

116:10 a lot of products that actually need . So, just again,

116:26 some of the definitions that we use standard temperature and pressure, which has

116:33 kinds of different definitions. What standard one community is not standard to another

116:38 as we know. So we have be a little bit careful. Um

116:42 , we would use STP with the of the natural gas standard here,

116:50 is pressure at sea level, one . So 14.7 p. s.

116:57 . And then somewhere around room So that's what I would call standard

117:02 and pressure. You know, you see in other communities, they're gonna

117:06 different different standards. And that's what company is all about. This is

117:12 standard that we're using. So what's game with a lot of these

117:20 they're just so many different units that used. And we need to know

117:27 most of them. Ultimately, if working in this area, the the

117:34 . I. Units are the metric typically are pascal's for pressure. And

117:41 pascal's is one atmosphere. But a of these just come from evolution,

117:49 know, hundreds of years ago, were using one measurement. They could

117:52 could measure the height of the mercury and that gave pressure. So that's

117:55 you define pressure millimeters of mercury. think, well, why would you

118:00 that? Well, that's how they pressure was with just a U.

118:04 mercury column. So that's what it . Um And again, we use

118:12 atmospheres or pascal's or P. I. But the weatherman is going

118:18 be using mercury or something like Great. Okay, we talked a

118:27 bit about viscosity, but technically viscosity when I when I stress the material

118:34 put pressure across it somehow. How does it strain or move? And

118:39 really the definition of viscosity. You , in a perfect gas or a

118:47 fluid. I could I could rub hand across it and it would be

118:55 no resistance. And in a infinite strain. So, I would

119:00 put my head across it. It moves with any sheer pressure stress at

119:08 . And solve That gives me zero . And here, you can see

119:22 some of the viscosity of standard things that we would be accustomed

119:29 So water say you can see the these very low, we get into

119:35 . The viscosity is many orders many bigger. By the time you're into

119:41 lava, it's very hibiscus. And we're looking at rock, you can

119:48 that the rock, we wouldn't even of it as being viscous. It

119:51 viscous, but just extremely viscous. viscous that it appears to be completely

119:59 and unmovable. Okay. So we've a bit about fluids but a bit

120:10 . There's some nice exhibits. You have been to the museum here.

120:15 we ever go? Have you been the museum? The Energy? The

120:19 energy center at the museum. I went was it for your, I

120:25 for sure. I went for dr when I took him for the

120:31 Rocks, rocks and minerals class. I think we were going to for

120:34 class within covid kind of ruined So. Yeah. Yeah. So

120:40 you go as part of this? master's class? Did you go over

120:45 No? I took rocks and minerals in like 20's 2019 or something.

120:53 I have seen the new the new . Um, yeah. Good.

121:02 know what? It's um, it's worth repeat visits. I've been there

121:05 few times. In fact, we them when they were setting it

121:08 We helped Qc and write some of verb It for him. The the

121:15 reached out to the G. H. Was a side of Houston

121:18 said we are putting up all the and we're looking for a whole set

121:24 volunteers to to go through the writing the materials and make sure it's all

121:29 . And so there was a whole of people who helped with with some

121:33 the some of the uh annotations and signage and stop there. But

121:41 yeah, that's that's great. They've got some just excellent displays and uh

121:48 I mentioned, it's changing. I there about a month or so ago

121:52 they've got new stuff. So it's really worth a visit. Um

121:59 one of the things they've got, I really like a lot is just

122:02 may have seen this. They've got turning wheel. Let me uh I

122:35 that Are you seeing that? We're seeing that I could see it

122:51 Mhm. Let me uh ah This some reason, this uh presentation rotates

123:07 . Mhm. Let me try See which orientation makes the most

123:32 Let's try the last orientation. uh this is actually a sphere pack

124:16 fluids. You can maybe see that little bit better on the upper

124:24 there's oil that's draining from a large pack. And on the lower one

124:28 oil draining from a small spear Can you kind of see that?

124:36 . And you can see that the oil goes into the big sphere pack

124:50 faster than the small sphere pack. it's really an indicator of um ferocity

125:11 normally they have Remember we with the packs. We did that the that

125:15 small sphere pack has the same ferocity the large sphere pack but has much

125:21 surface area. So normally porosity and go together. So higher porosity,

125:28 permeability and that's general. However these , these have the are the same

125:36 the permeability is are quite different. permeability really relates to area. Let's

125:44 see if we can get back here when we talk about flow, that's

125:57 lot. So if we put a pressure across this, say pipe that's

126:03 of a material, we have a differential across it then depending on how

126:10 the material is and the area and disgusting the fluid that determines the

126:19 So flow is naturally how much goes . This is naturally directly proportional to

126:24 porosity is the change in pressure. pressure we're putting on it and it's

126:30 proportional to the viscosity of the So high viscosity as we'd expect,

126:36 low flow. And we see And then of course the permeability.

126:40 permeability gets high flow and low permeability low flow but it's the amount that

126:48 get out of the rock, depends the pressure that we apply to

126:52 The permeability of the material, how we're trying to flow it and then

126:58 viscosity of the fluid that we're trying get out. So that all kind

127:02 makes sense. And that's darcy's lock we're interested of course, in how

127:11 different kinds of fluids flow, we be trying to produce oil or

127:16 we want to know how they flow water. How does the water

127:22 On the other hand, we might trying to inject fluids, we might

127:24 trying to put fluids like SEO to CO two. So we're trying to

127:29 a fluid and the CO two might be in a hyper critical state or

127:36 largely fluid state. So when we to the reservoir engineering, we need

127:44 know these kinds of factors, how is material. Uh how far are

127:52 trying to put it in? What the viscosity of the fluid? And

127:56 ultimately, the reservoir simulators need all stuff. And they're gonna model via

128:02 Law, they're going to model fluid and how much we can recover or

128:05 into the formations. Okay, So might just ask a few little questions

128:21 such as are there differences between oil gas wells and generally in the construction

128:26 the well, not too much different general. Both wells are going to

128:33 producing some fluids and we even the , we talked about there being um

128:42 natural gas liquids, even in a well, and certainly in producing an

128:48 reservoir, there's probably dissolved gas in oil. So, when we recovered

128:53 lower the pressure a little bit the will come out. That's why often

129:00 quoted when we look at the actual oil in place, we have to

129:10 that a bit smaller because when we the pressure on the oil, the

129:14 comes out of the oil and the shrinks and volume. So We've got

129:21 amount of oil with dissolved gas under . When we bring it to the

129:26 , the gas comes out and the of the amount of fluid is a

129:30 smaller. So the oil has a shrinkage factor or something like that.

129:36 in terms of the wells, the are gonna be pretty similar. Um

129:40 we were drilling gas wells again, gas has lowered viscosity in general than

129:46 , we could space the wells further because they'll flow more. And of

129:58 , gas wells, we haven't got this. But Stephanie, probably in

130:02 of your petroleum geology background or gasses generated at higher temperatures and pressures.

130:11 the gas window is lower than where oil is made in the kitchen,

130:16 underground kitchen. So, if you're for gas, often it's a bit

130:24 . Oil is a bit more And then if gas has evolved,

130:31 can lead to a lot higher formation , it's also more mobile. So

130:40 can move faster. So we're always uh about gas effects because again,

130:46 can be pressurized more and it can faster. So we're we're always worried

130:55 high, high formation gas pressure because can blow out easier in some

131:02 So, just some notes about oil gas. Now, we've we've talked

131:09 bunch about fluids, but we're also in the matrix properties. So now

131:19 talked a bit about porosity, we've a bunch about fluids and now about

131:23 rock itself. And we were looking where can oil and gas b and

131:30 the east coast of Canada, just of Maine and massachusetts, there,

131:36 are a lot of basins along the of the coast and along the margins

131:41 the east coast of the US. , just generally speaking, there are

131:46 of moratoria on exploring, not to drilling off the east coast.

131:57 most of the states along the East have restricted exploration and drilling. They're

132:06 perspective, it's just that you're not to really do anything. They're off

132:10 east coast of Canada Nova Scotia and . There are a lot of perspective

132:17 and and some production. So, the east coast of Nova Scotia,

132:24 good gas production, and then fairly production off the coast of Newfoundland,

132:34 hostile place. But you were asking some of the production platforms and their

132:42 production platforms off Newfoundland there in about ft of water, 300 ft of

132:48 . And they are some they have legs, they're huge platforms that were

132:53 out, then turned and sunk down these are concrete legs and in

133:00 they store the oil in the oil the legs of the platform and they'll

133:05 producing maybe 100 couple 100,000 barrels of per day, pretty big production.

133:16 again for us and this would be stuff that we're looking at in in

133:20 rock physics course we want to have estimator something that measurement we can make

133:29 that tells us about the rock And so we know know that if

133:35 have the P. And S. velocity that we can extract from seismic

133:39 we can plot that and say something the rock type and its porosity.

133:45 here are a few kind of related . So you can see that if

133:56 P wave velocity was say 3000 m second and the shear wave velocity was

134:05 m per second. What kind of is it? So P. Wave

134:12 shear wave 1500. What kind of isn't 21,500? Is that gonna be

134:23 cretaceous? No. What's orange, the orange whatever oranges. Yeah it's

134:35 gonna be something like a cretaceous shale again probably too. Um one of

134:45 younger mud stones are semi consolidated So if we if we knew that

134:59 say now that we've got both those a. V. P.

135:01 S. Of two which is fairly then suppose we knew that then we

135:09 down to the next bottom sort of . P. B. S.

135:11 two and it's a shale that I go across and say okay well suppose

135:21 was a cretaceous shale Then I could across make some of these other measurements

135:26 figure out well it probably has a of about 12% or something like that

135:30 13%. So again the situation here you say well okay but if we

135:38 get V. P. And S. From making seismic measurements remotely

135:45 in the borehole then I can tell something about the ferocity. And again

135:52 be kind of rude or direct, don't really care about B.

135:55 B. S. But I do about ferocity. So if I can

135:59 V. P. D. Which I happen to personally like but

136:03 for porosity that's what we really want that gets down to the dollars how

136:08 hydrocarbon could be in this rock then can use those measurements. The seismic

136:15 to infer values be PBS and use B. P. B.

136:19 To infer ferocity which gets down to to the money. So that's what

136:26 trying to do now you could say some of these rocks we can um

136:34 we mentioned quartz is very very It's rigid to the point of being

136:43 . And so that's our glass and course we drop a nice glass on

136:48 floor. We know what happens, shatters and that's the courts having a

136:57 high rigidity and a very high brittleness in a sense. Who cares about

137:05 ? Well we we care about it if we're going to hydraulically fracture Iraq

137:11 I know that courts breaks. So I'm looking for an interval to break

137:23 gonna look for quartz and when we at a lot of the plays the

137:30 and shale a lot of these plays shale itself is a little bit harder

137:35 break because you can see that clay a low shear modulates its ductile and

137:43 it's d for mobile and it means it's not brittle. We like shale

137:50 the unconventional world because it can contain organics. So we like shale because

137:56 got a lot of organics in We don't like shell because it's hard

138:00 break. So what we're gonna do we're gonna try to explore for an

138:08 that has the highest T. C. Total organic content. So

138:17 Shelly but that also has the highest . So I've got the goodies,

138:24 organics but I've got it breakable so can get them we need both And

138:32 as the organics go down the courts up so we're looking for a place

138:38 has the most courts and the most or we're looking for a sandwich like

138:44 bacon that has the shale in proximity a carbonate or sand and I'm going

138:53 go in with the horizontal and break sand and the hydraulic fracture can propagate

138:58 into the shale and break the shale I can access the shale and produce

139:03 from the sand. Good. So that's part of the reason that we're

139:15 for all this stuff. An example why we're looking for a map,

139:20 can make of rigidity as well as map. I can make abducted city

139:25 viscosity. So all these maps have purposes. And then this is really

139:32 for your records, the we want start to get to know what what

139:37 velocities all mean. And so you've these in the back in your back

139:44 to a degree. We know you , you want to know that some

139:47 the numbers, for example, a sand Is gonna have a lowest velocity

139:56 around 2000 m/s. So we want know generally that's a wet sand

140:04 If we get up to a generally a much higher velocity and generally

140:12 higher density. These are the common that we deal with. Um And

140:18 the Dolomites again very generally higher velocity quite a high density also and

140:25 fast, high density. So those the kind of rocks we want to

140:31 to get to know their properties so you've got these immediately. You don't

140:37 to look them up and you know or less if it's high velocity like

140:40 m per second and high density like 2.7, then we know know that

140:46 not a sandstone, it's not a , it's not a shale, it

140:51 to be an evaporator of carbonate. , so we start to get to

141:01 to be friends with these numbers. you've done a bunch of this,

141:04 is just a compendium from matt hall again this is just sort of for

141:11 records with with all these different bounds different little equations and we want to

141:21 to know these these are all of classic equations for rock physics. So

141:26 we step through them, we could the bulk modulation as a function of

141:29 for different kinds of rocks. And have different bounds whether they're the rice

141:34 the or the other bounds. And go by hash instructing bounds in other

141:41 , depending on how the rock is or how how diet genocides that

141:48 And then we plotted B P B , which we can plot versus composition

141:52 ferocity and then our classic little density as a function of porosity,

141:58 july and then this is the workhorse most traditional rock physics. The fluid

142:06 in which we make some measurements of rock with a dry frame, find

142:11 what his composition is and then put sections into the ferocity and then we

142:20 what that's gonna do to the Now it turns out that Matt Hall

142:28 a bunch of books on 52 things should know about rock physics and about

142:37 . So have a look at matt , he is also the honoree of

142:43 Gs Hs symposium this year. So you get a chance to attend some

142:50 that that would be good for both and Stephanie and that I think Utah

142:57 brought this up a little while It's what's the date for that?

143:07 was just looking here G. H. Symposium is uh April 19

143:19 20th. So April 19 and The G. S. H.

143:26 matt hall and all his work. they're gonna have a bunch of python

143:37 because that's been his big thing, and matt matt lab coating. So

143:42 you're interested in some of that coating I think there's gonna be some ancillary

143:45 sessions with the regular symposium. Now an overwhelming graph. Just so you

143:54 it in your records. Um We all of these, we talked about

144:01 these parameters in rock physics the young's asse, which is just when I

144:06 a strain on the rock, how can I or stress, how far

144:11 I stranded bosons ratio will drive it I squish the rock in one

144:18 How much does expanding the other Sure modulates when I stress the rock

144:23 way. How much does it deformed and of course velocities we understand.

144:30 all these are kind of the elastic that we use in just a nice

144:35 tropic standard rock. And you can a whole pile of measurements here.

144:40 this is really just for your But this is all the stuff that

144:43 into what we observe. Generally our or p wave velocity, shear wave

144:48 and maybe density and then maybe the . P. V. S

144:52 So these are our elastic wave numbers and we only need three of them

144:57 we can derive any of the rest them. So once again, rock

145:06 and that you would have been through john it's really the sort of the

145:15 between rock properties and especially seismic How do seismic waves interact with the

145:22 and how do the rock properties affect seismic waves? And we ultimately want

145:26 know that because we're going to use waves to create the structure and in

145:30 the rock properties. Seismic waves are cheap to make evaluating rock properties is

145:39 expensive via drilling and core characterization. , so there's just a bunch of

145:51 for rock physics. Once again, do a lot of this in the

145:56 Hall because we're we're measuring more of rock properties and surface measurements. And

146:01 we're trying to to relate those rock to what we measured? And there

146:09 just a bunch of definitions that you see here and read. I'll give

146:13 just a second to read those and can see that generally, we're just

146:34 to relate the actual physical properties of rock to some measurement that we make

146:40 the rock, whether in the borehole the lab or in the surface.

146:44 so we're going to go back and . We've got the rock properties.

146:47 should that look like in the measurement we've got the measurement which that look

146:52 . What's that infer about the rock . So once the forward problem,

146:55 the inverse problem and we're doing both them to try to characterize the

147:03 Once again, here's another description from and you can see that this is

147:10 they put rock physics between the geology all these properties and between the values

147:16 we have. And then in a , the geophysicist is over here,

147:30 seismic person trying to infer this And then the rock physicist is trying

147:35 infer this stuff and then we get into the Petro physicist and the geologists

147:40 to get right back to the geology the rocks. So john might have

147:49 you this slide Stephanie, Did he something like this? Probably Yeah,

147:55 . So you're familiar with this and that's kind of the seismic type of

148:03 . Great, okay, so what rock physics? It's just data versus

148:12 the rock property. Yeah, it's the the geophysical measurement we make

148:18 And how does that relate back and to the rock properties. And what

148:22 the physical laws in that interaction? a little slightly trickier one. What's

148:33 gauge pressure 10 m underwater? You kind of talking about this yesterday?

148:40 one atmosphere. Yeah. So that's basically. What atmosphere Or 14.7

148:54 s. i. Mhm. And what is In Fahrenheit? What's 28°C.

149:05 82.4. There you go. So I like that one because it's

149:12 palindrome Oh yeah for negative 40°F Well both so 28 c. is

149:22 f. So you can always remember because it's just background. So now

149:29 never forget that 28 C just put backwards and that's f. So I

149:35 to use that all the time. most of the family, my family's

149:38 Canada. And so if I tell in a sense it's 82°, they say

149:47 ? So I have to say it's seat Because 82° C is almost

149:54 That's not. Likewise we always talk being cold so -40 c. is

150:02 lucky Because that's -40 f. So happen to be the same. So

150:13 are two peg points that you can an F. That are that are

150:19 to remember. 28 C. Is F palindrome, It's backwards like radar

150:24 forward and backward the same. This exactly a palindrome but it's just backwards

150:33 Different than -40 c. is -40 . So that's a nice one to

150:39 to, if you're in Alaska, it's minus 40 degrees F. And

150:44 you're across the border in the Yukon minus 40 degrees C. It's the

150:48 temperature. So those are two that , that are easy to remember

150:57 Um this gets a bit more but we can also take gas mains

151:07 which were for an ice, a material and extend them to an anti

151:11 tropic material. And a former student iris long, long long was a

151:16 strong quantitative student and he extended Gaston's to anticipate tropic materials, which was

151:24 really nice piece of work. And published this and a really nice piece

151:28 work. He's now working with Shell he's done, he's done very nicely

151:37 . Incidentally, it shows how things change and you've all seen about

151:44 but Several students have had to suffer periods of unemployment, including long when

151:52 couldn't get a job, he was , very strong, but he couldn't

151:54 a job and he was all depressed then all of a sudden things turned

151:59 and he got an excellent job, . Likewise, another student done his

152:03 did a great job, 15 months and then all of a sudden things

152:10 around and he called me and he in one weekend, he got three

152:13 offers, this was a couple years . So uh that lifted his spirits

152:21 then a couple of other of our just about a year and a half

152:26 and both been unemployed. And then was at a G. S.

152:29 . Luncheon and one of the employers up and said what do you think

152:31 these two people? And I said they're they're both excellent workers, they've

152:35 great great backgrounds and boom both of got job offers. So it Can

152:41 pretty fast or it can happen pretty . The 15 months being unemployed was

152:46 bit of a drag. But that turned out in the end okay.

152:51 this was long and he did a job in his thesis and that was

152:54 of his stuff. We have talked the permeability versus porosity generally. Again

153:02 rock properties. We think that permeability increases with ferocity but it can be

153:10 little bit funky. In other words not necessarily a straight correlation depending on

153:19 content and and other factors. I that is getting a little bit beyond

153:30 we need to be right now. it's just about noon. We've got

153:37 going to start to get into logging next. So Stephanie was normally and

153:47 talk normally an hour for lunch or . And Yes so usually have a

153:53 lunch break on junior. Well great we are we finished lecture four and

154:03 take a break for an hour and come back with at one o'clock and

154:10 continue on until just about 4 I know you're a little under the

154:14 Stephanie, and so it won't be too badly today. Well,

154:20 Great. Well, we'll see, see everybody back here at one o'clock

154:25 then we'll do Couple more hours and up around 4.30. Okay.

154:31

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