Scott I. Reed: Like a fight last or anything.
Scott I. Reed: Or you can throw it up when you see it stop the rating.
Scott I. Reed: Oh God.
Scott I. Reed: Go on the line.
Scott I. Reed: Oh, it just fell.
Scott I. Reed: Come down to each line, because that's when we were.
Scott I. Reed: Each line to get full, so the bottom.
Scott I. Reed: Three, enough that and then you'll let it level
Scott I. Reed: we here. And then you have a stopper like it off.
Scott I. Reed: OK.
Scott I. Reed: Thank you.
Scott I. Reed: So the way it should play.
Scott I. Reed: It's not acting Bulldogs popping radiators and you've got to have it
Scott I. Reed: little folder.
Scott I. Reed: Hold on.
Scott I. Reed: Yeah, I guess that makes sense, 'cause.
Scott I. Reed: But actually, if you don't have a real high point.
Scott I. Reed: Well, and I remember that.
Scott I. Reed: Dollars. Your energy guys. Allen, I remember he was saying you got to be
Scott I. Reed: able to turn those pumps on, be able to lead it.
Scott I. Reed: And once it's been said, if we have a lead level in the pump,
Scott I. Reed: if you don't want to tap the pump.
Scott I. Reed: Then.
Scott I. Reed: We'll turn up on the Bleacher each vow.
Scott I. Reed: To get it once you upload each one of these deals.
Scott I. Reed: Just like before.
Scott I. Reed: I don't think these data, they don't care.
Scott I. Reed: Right. Yeah. You want to build space for that, right?
Scott I. Reed: Parser. One more thing, don't really actually have people that
Scott I. Reed: run.
Scott I. Reed: OK.
Scott I. Reed: Yeah, I would like to thank all.
Scott I. Reed: Hello.
Scott I. Reed: What?
Scott I. Reed: AT3PMI.
Scott I. Reed: Not being anything on theater.
Scott I. Reed: Or forget.
Scott I. Reed: Ting my tear down there.
Scott I. Reed: Got a prime it.
Scott I. Reed: Yeah, because again, you're coming off the top, so.
Scott I. Reed: It's off up here in natural dirt bombs so.
Scott I. Reed: There's still something said here from Alaska.
Scott I. Reed: Is that what you told him?
Scott I. Reed: I didn't even hear that.
Scott I. Reed: We got this right there.
Scott I. Reed: Yeah. I didn't even think about this.
Scott I. Reed: And the buck crab area.
Scott I. Reed: Get a disc.
Scott I. Reed: Ount.
Scott I. Reed: Got them everywhere.
Scott I. Reed: Wait.
Scott I. Reed: If we plug it in.
Scott I. Reed: We have a little bucket or something or that all you need is crack, no.
Scott I. Reed: Detecting sometimes.
Scott I. Reed: Oh.
Scott I. Reed: Oh my gosh.
Scott I. Reed: Oh.
Scott I. Reed: That's right.
Scott I. Reed: Oh my God.
Scott I. Reed: Maybe not, but what that stuff out?
Scott I. Reed: Let me.
Scott I. Reed: Now like it, it's a little bit about a *******
Scott I. Reed: horrible job of something, anything up there.
Scott I. Reed: I mean, they talk about.
Scott I. Reed: They talk about, yeah, there you go.
Scott I. Reed: You plug it in now.
Scott I. Reed: You want some reflection?
Scott I. Reed: You're out here.
Scott I. Reed: I'll be pretty gracious. That would be good.
Scott I. Reed: All right.
Scott I. Reed: You know.
Scott I. Reed: Got flow for three-point something.
Scott I. Reed: Not very flat.
Scott I. Reed: I have a little.
Scott I. Reed: Good food.
Scott I. Reed: That means you look at pool there so.
Scott I. Reed: That's a nifty little file you got.
Scott I. Reed: There you don't.
Scott I. Reed: So if it's sealed to that pipe.
Scott I. Reed: Basically, replace the pad and then it has to be
Scott I. Reed: replaced into it and then you can let it pick the pool and you fix it and stopped
Scott I. Reed: it.
Scott I. Reed: Then you pull your cap off.
Scott I. Reed: That's right.
Scott I. Reed: Yeah, they're vapor bars, but.
Scott I. Reed: That's the thing I need to get the white card, yeah.
Scott I. Reed: Like all sorts of the bathroom.
Scott I. Reed: Somebody was smarter. Yeah. Somebody got tired of it spilling stuff
Scott I. Reed: all over the place.
Scott I. Reed: I like how it's declared. You can see how much it's really in it.
Scott I. Reed: Claude.
Scott I. Reed: Aye.
Scott I. Reed: Back to New York.
Scott I. Reed: We haven't had any come out yet.
Scott I. Reed: Huh.
Scott I. Reed: Slowly increasing.
Scott I. Reed: Its flow or being able to buy an ounce of COC.
Scott I. Reed: Aine somewhere.
Scott I. Reed: OK.
Scott I. Reed: Yeah.
Scott I. Reed: OK, be the one you fell OK.
Scott I. Reed: 7/7.
Scott I. Reed: It went all over the place and you got to, like, close it out.
Scott I. Reed: All right, Jay, just thought, well, now it's back down to six.
Scott I. Reed: I just like my little guy.
Scott I. Reed: OK.
Scott I. Reed: Thank you.
Scott I. Reed: Probably the pump again.
Scott I. Reed: Got a hair lot you want to pop on or off? There it all.
Scott I. Reed: People, often ****** *******, turn that off with me.
Scott I. Reed: You know.
Scott I. Reed: Hey.
Scott I. Reed: Hey bro. Thoughts on lunch. If you had one hour.
Scott I. Reed: Yeah, put it that way for that. Life's blind, right? What, blonde?
Scott I. Reed: Very good.
Scott I. Reed: I don't know if that's done earlier.
Scott I. Reed: I just made that same thing last night.
Scott I. Reed: I highly have any idea of glad it was good to be.
Scott I. Reed: Basically starting a backseat.
Scott I. Reed: They're talking a good chicken.
Scott I. Reed: It's probably like ****.
Scott I. Reed: Yeah, I don't like the noodles in drop boxes.
Scott I. Reed: That's that did not work very well.
Scott I. Reed: Why you don't put them in there for six hours? 'cause, I don't know.
Scott I. Reed: They just thought.
Scott I. Reed: Oh.
Scott I. Reed: It was a good idea.
Scott I. Reed: I was there. Or not.
Scott I. Reed: It was a good idea.
Scott I. Reed: Poorly executed I was.
Scott I. Reed: I think we could make it work.
Scott I. Reed: Last time I do anything for you guys, where did stop?
Scott I. Reed: I don't know.
Scott I. Reed: We should be like a wrap of ribbons on top.
Scott I. Reed: No, no. I'll bring the smoker down.
Scott I. Reed: We'll go to it at 6:00 AM and by 1:00.
Scott I. Reed: Hey, I will plug it in.
Scott I. Reed: He's fine talking to the roof bit.
Scott I. Reed: I mean, ain't nobody even want?
Scott I. Reed: Aye, that one's got. Aye, aye.
Scott I. Reed: Well, I mean, while about lunch today, you get done.
Scott I. Reed: Not a day today.
Scott I. Reed: Oh well, alright what we did.
Scott I. Reed: Very good.
Scott I. Reed: I'm happy picking picking on you.
Scott I. Reed: OK, you ain't.
Scott I. Reed: Talking, man, this ******* hamburger out, that's true.
Scott I. Reed: I have little friends that.
Scott I. Reed: Have a lot.
Scott I. Reed: Then what? What the **** handle pack.
Scott I. Reed: Oh, that's not really.
Scott I. Reed: Bigger job.
Scott I. Reed: Well, to be fair.
Scott I. Reed: Like this news about I got the bulbs here.
Scott I. Reed: Hey all I do with you pal.
Scott I. Reed: And I put the info on the muscle.
Scott I. Reed: OK.
Scott I. Reed: Tell me, Bobby. Oh, yeah. Bobby. Bobby.
Scott I. Reed: Bob.
Scott I. Reed: I did all right.
Scott I. Reed: I guess we're gonna get on now.
Scott I. Reed: Oh, feel like you feel like you're falling.
Scott I. Reed: You go oh.
Scott I. Reed: I'm pretty sure.
Scott I. Reed: I mean, we're taking something for the grill.
Scott I. Reed: How is it?
Scott I. Reed: Almost 11.
Scott I. Reed: 101040.
Scott I. Reed: You got burgers.
Scott I. Reed: I don't know if we got roll.
Scott I. Reed: That's not what I asked.
Scott I. Reed: OK.
Scott I. Reed: It breaks loud.
Scott I. Reed: Yeah.
Scott I. Reed: OK, OK.
Scott I. Reed: This is a non sugar free.
Scott I. Reed: Non sugar free gotcha alright.
Scott I. Reed: Sure.
Scott I. Reed: Yeah.
Scott I. Reed: Start word.
Scott I. Reed: So tell me, did you get to play your new me?
Scott I. Reed: Segment draw.
Scott I. Reed: No, I mean, how's it OK.
Scott I. Reed: You want to be all over it, right?
Scott I. Reed: Say what you want me all open.
Scott I. Reed: ****. That's my understanding, yeah.
Scott I. Reed: Say what?
Scott I. Reed: What's the point like?
Scott I. Reed: So you're at 17 meters per minute.
Scott I. Reed: A lot better. Sure, I don't really know what you said.
Scott I. Reed: The test pilot is a theoretically don't have anything to stop it, right?
Scott I. Reed: Let me see what it used to be.
Scott I. Reed: I can't any difference.
Scott I. Reed: We don't have to say we can stand here.
Scott I. Reed: But I thought we were like at 30 before, maybe that's six point memory.
Scott I. Reed: Yeah.
Scott I. Reed: OK.
Scott I. Reed: Just to pull up, Anthony.
Scott I. Reed: 17.
Scott I. Reed: You're like, oh, God is.
Scott I. Reed: Excellent, good job.
Scott I. Reed: I'm going to the brake lights today, but you know, if you get bored and bored.
Scott I. Reed: I I got those.
Scott I. Reed: I drive the gammy no which is very that which is frayed again.
Scott I. Reed: First time I'm like three years.
Scott I. Reed: Yeah, I'm blowing it up.
Scott I. Reed: Don't count me out.
Scott I. Reed: Bluetooth setting.
Scott I. Reed: S OK.
Scott I. Reed: That would be all three.
Scott I. Reed: It really fluctuated.
Scott I. Reed: Sometimes they were down around this temperature,
Scott I. Reed: sometimes it was higher because once you get once this gets hotter,
Scott I. Reed: you're also going to have a convective heat force,
Scott I. Reed: just just like there's convection in here.
Scott I. Reed: Through the down comers, there's going to be some natural
Scott I. Reed: convection here, so it's actually going to bump your blow
Scott I. Reed: up once this gets hot.
Scott I. Reed: What you're also compounding pressure is pushing too.
Scott I. Reed: Yeah, you're as.
Scott I. Reed: Jason said.
Scott I. Reed: Your pool at temperature goes up.
Scott I. Reed: That's going to drive your pressure up. That's also going.
Scott I. Reed: But yeah, you can see it.
Scott I. Reed: And all the other ones drop em.
Scott I. Reed: That's basically alongside.
Scott I. Reed: So they're just charging now.
Scott I. Reed: There you go.
Scott I. Reed: I did a quick.
Scott I. Reed: OK. Then I'll go ahead and then we'll start
Scott I. Reed: the product pretty soon.
Scott I. Reed: I think so, yeah.
Scott I. Reed: OK.
Scott I. Reed: I'll go.
Scott I. Reed: I'll get my computer, then I'll be on.
Scott I. Reed: OK, let's go for like 1/2 hour. It's still getting like little
Scott I. Reed: microbolved probably not. We're going to get out way out.
Scott I. Reed: Take it slow for like 30 minutes and then I'll check it again. Oh, OK.
Scott I. Reed: It is blowing and I don't see any major air fracking.
Scott I. Reed: I mean more than two bubbles isn't gonna make a difference.
Scott I. Reed: But you know, we don't wanna talk.
Scott I. Reed: I mean, do you wanna? Do you wanna look at that?
Scott I. Reed: It seems to be you seem a little bubble city.
Scott I. Reed: Yeah. Did you see him down there? Yeah.
Scott I. Reed: I mean like mobile deep or big bubble at some point, right?
Scott I. Reed: Yeah, it looks like the world's worst campaign.
Scott I. Reed: Yeah.
Scott I. Reed: You taste it more than just. You say it didn't like. I'd rather not.
Scott I. Reed: Yeah. I mean, it's not gonna.
Scott I. Reed: It's not gonna hurt.
Scott I. Reed: That's the same stuff that.
Scott I. Reed: That's like the laxative they give you when you're about to get a colonoscopy.
Scott I. Reed: Oh, let me go, Ben.
Scott I. Reed: You might have to see it later, but it'll be fine.
Scott I. Reed: Right out. What is that stuff called?
Scott I. Reed: Right away, I'm not.
Scott I. Reed: What? What is that stuff called?
Scott I. Reed: It has a brand name. It's like.
Scott I. Reed: Yeah, that's what it is.
Scott I. Reed: So yeah, so why you hear that?
Scott I. Reed: My wife, I don't know.
Scott I. Reed: Oh, OK, yeah.
Scott I. Reed: OK.
Scott I. Reed: Yeah, it's. Oh, it hurts.
Scott I. Reed: Yep, I'll do that.
Scott I. Reed: I've never used beer, Lex.
Scott I. Reed: I have to take the antibiotic till.
Scott I. Reed: They make me all clean.
Scott I. Reed: I'm taking them to Utah.
Scott I. Reed: I didn't like that bad.
Scott I. Reed: I guess that's the problem.
Scott I. Reed: That's kind of weird.
Scott I. Reed: And it's all the other problems that you get it without any antisep.
Scott I. Reed: Tic.
Scott I. Reed: I gotta go to 12th doctor's bike.
Scott I. Reed: I went to it right.
Scott I. Reed: Right there.
Scott I. Reed: But he's like, no, it'll be fine, but it's like through the whole thing.
Scott I. Reed: And it's really jumping up.
Scott I. Reed: Oh shoot.
Scott I. Reed: Yeah.
Scott I. Reed: I I had one I was like.
Scott I. Reed: Put me.
Scott I. Reed: I don't know why you have to wait.
Scott I. Reed: Yeah, no, I'm they told me to count backwards.
Scott I. Reed: 100 and I made it to like 96.
Scott I. Reed: And.
Scott I. Reed: And next thing I know, they were telling me it was like 2 1/2
Scott I. Reed: hours later.
Scott I. Reed: Wow. Yeah, that's what I say.
Scott I. Reed: Did you wake up from bathroom correct? Yeah.
Scott I. Reed: So when this is done, how are you gonna take that off without
Scott I. Reed: fixing?
Scott I. Reed: It oh OK.
Scott I. Reed: Well, Ok's gonna have you hold, OK?
Scott I. Reed: I'll, I'll hold it and and then you'll have his
Scott I. Reed: mouth right underneath.
Scott I. Reed: It already after one. OK, OK.
Scott I. Reed: So then I'll we'll just let this go for a little bit, OK.
Scott I. Reed: The blood that I can gained.
Scott I. Reed: Yeah. Let me give you a little bit better.
Scott I. Reed: Is it still making bubbles?
Scott I. Reed: A little bit, but pretty spacious.
Scott I. Reed: There's a bubble.
Scott I. Reed: OK.
Scott I. Reed: They give me a portal and so I got pressure still. Like, OK, say what?
Scott I. Reed: Five times when we let it out, but the pressure still fluctuated a
Scott I. Reed: little bit.
Scott I. Reed: And now it's like stepping good sound.
Scott I. Reed: Douglas, **** ***.
Scott I. Reed: OK.
Carlo Parisi: Hey, Scott, I I I just logged in is something is
Scott I. Reed: I'll come back out in 20 minutes or so.
Carlo Parisi: changing.
Scott I. Reed: Actually, what time do you think?
Scott I. Reed: 81015023 hold on.
Scott I. Reed: Let me break that up over time.
Scott I. Reed: Hey, hold on.
Scott I. Reed: So you just give me a long minute.
Scott I. Reed: I was like, do you wanna go grab lunch now?
Scott I. Reed: So that since it's almost 7.
Scott I. Reed: So when this.
Scott I. Reed: I think it's just a thought, no?
Scott I. Reed: Yeah, because once we start, we're gonna want to go 'cause.
Scott I. Reed: It sounds like we're gonna be turning valves.
Scott I. Reed: And yeah, we're probably gonna bring them in.
Carlo Parisi: Scott.
Scott I. Reed: Yeah, we should just gonna have lunch.
Carlo Parisi: Hey, can you hear me?
Scott I. Reed: Yeah.
Carlo Parisi: Yeah, I just logged in.
Carlo Parisi: I want to understand what what's going on.
Carlo Parisi: I see some mass flow that is racing.
Scott I. Reed: Yeah, that, that's that's too high up on that chart.
Scott I. Reed: Hold on. I can't.
Scott I. Reed: I can't hardly hear you.
Carlo Parisi: Yeah. I I I just logged in and I want.
Carlo Parisi: I want to understand what's going on.
Carlo Parisi: I see a mass flow that is racing here the blue line.
Scott I. Reed: Into the brown one. True. Yeah. So they just.
Scott I. Reed: They just been pulling the the bubbles out.
Scott I. Reed: So what you're seeing is the the glycol starting to take some of that heat.
Carlo Parisi: Ah, OK, OK.
Carlo Parisi: So there is no pump on right now.
Scott I. Reed: No, the pump is on right now, but the hrus stop.
Carlo Parisi: Oh, it's on OK, yeah.
Scott I. Reed: But the hrus not.
Scott I. Reed: I mean they they just been trying to get the bubbles out.
Carlo Parisi: OK.
Scott I. Reed: There, they've got probably 90% of the bubbles
Scott I. Reed: out.
Carlo Parisi: OK.
Scott I. Reed: But they're still getting old blips here and there.
Carlo Parisi: OK.
Scott I. Reed: What? Josh was just suggesting is maybe we
Scott I. Reed: should just run the lunch and eat an early lunch.
Scott I. Reed: Let the bubbles come out and then come back.
Scott I. Reed: Because once, once we start into the testing,
Scott I. Reed: it's probably gonna be pretty hard to leave it.
Carlo Parisi: Yeah, yeah, yeah, I agree.
Scott I. Reed: So yeah, I I think that's probably a fair
Scott I. Reed: assessment.
Scott I. Reed: So probably take an early lunch hour early.
Scott I. Reed: And then when we come back, the bubbles will probably say enough
Carlo Parisi: Oh, I see.
Carlo Parisi: Yeah, it's 11 there, yeah.
Scott I. Reed: bubbles are out.
Carlo Parisi: Yeah. OK.
Carlo Parisi: OK, I'm gonna be online so.
Scott I. Reed: Yes, I don't.
Scott I. Reed: I don't think you'll see anything happening for an hour.
Carlo Parisi: Yeah, for yeah, OK, sounds good.
Scott I. Reed: So.
Scott I. Reed: OK.
Carlo Parisi: Enjoy your lunch, then.
Scott I. Reed: Thanks Kyle.
Scott I. Reed: Well.
Scott I. Reed: So I don't know if you guys can hear us or not,
Scott I. Reed: but we're getting ready to start this again.
Carlo Parisi: Yeah, we can hear you, Scott, OK.
Scott I. Reed: OK.
Benjamin A. Baker: Hey, Scott.
Benjamin A. Baker: Yeah, yeah. I was just wondering. So on this diagram here.
Scott I. Reed: Are you looking at my screen?
Benjamin A. Baker: The flow meters.
Benjamin A. Baker: Yeah, your screen.
Scott I. Reed: Uh huh.
Benjamin A. Baker: So flow meters are the ecfl 12/20 fi.
Scott I. Reed: Fi Zero 42.
Benjamin A. Baker: See Zero 42.
Scott I. Reed: He's got his mouse moving around on the far right.
Scott I. Reed: 'Cause, we're on #4.
Scott I. Reed: He'd exchange your 4.
Benjamin A. Baker: He said.
Benjamin A. Baker: Far right.
Scott I. Reed: Yeah, you may need to scroll to the right if
Scott I. Reed: you have a non widescreen screen.
Benjamin A. Baker: Yeah.
Benjamin A. Baker: OK.
Benjamin A. Baker: I see.
Benjamin A. Baker: So that's the flow meter that you're on then?
Scott I. Reed: Yeah. So we're at 15 liters per minute.
Benjamin A. Baker: OK.
Scott I. Reed: We we we don't have coolant, just just so you're aware.
Scott I. Reed: Ben 'cause you weren't on the call earlier today.
Scott I. Reed: We don't have coolant in the other three loops.
Benjamin A. Baker: What do you mean you don't have coolant like?
Scott I. Reed: There's only coolant in loop 4.
Carlo Parisi: Yeah.
Benjamin A. Baker: Oh yeah, you're just starting on the first one.
Carlo Parisi: So. So, Scott, I see the temperature are 26 Celsius.
Scott I. Reed: Yes.
Carlo Parisi: OK.
Carlo Parisi: And so the can you can you please show me also the temperature in the in the for
Carlo Parisi: the lad the loop for.
Scott I. Reed: Yeah.
Carlo Parisi: Hmm.
Carlo Parisi: I use.
Carlo Parisi: OK.
Carlo Parisi: See, now it's dropped.
Carlo Parisi: Yeah, it's 25 up there, OK.
Carlo Parisi: So there is a big Delta T now between the the lad. Can you show me also the other?
Carlo Parisi: One other ihx the one without coolant please.
Carlo Parisi: 75.
Benjamin A. Baker: Yeah, they're all pretty close to each.
Carlo Parisi: OK.
Carlo Parisi: These are all 93. OK, OK.
Carlo Parisi: So those calls, they're basically creating a large delta
Carlo Parisi: T in the in the IH X OK.
Benjamin A. Baker: Yeah, that was 20 to 60, was it or 50?
Carlo Parisi: Yeah, you can put back to the, yeah.
Carlo Parisi: Seems 50. Yeah, because it was 2070. Yeah.
Benjamin A. Baker: 50.
Benjamin A. Baker: So that's quite drop a 40° C drop from the 93.
Carlo Parisi: Yeah.
Benjamin A. Baker: So it overall reduces the whole thing and a delta T within it.
Carlo Parisi: Yep.
Scott I. Reed: Why is that so low?
Scott I. Reed: Why is that 25?
Carlo Parisi: There may be.
Benjamin A. Baker: You mean because it's a little lower than what the other one's reading?
Scott I. Reed: But Fatima is still alive.
Scott I. Reed: Even then, I don't know why it's so low.
Scott I. Reed: Well, there is a negative perch through there,
Scott I. Reed: but yeah, but I mean that would.
Scott I. Reed: I mean, I'd expect it looks like SCT 0.
Scott I. Reed: 45 is like close to ambient.
Carlo Parisi: Hmm.
Scott I. Reed: Which doesn't make any sense.
Carlo Parisi: Hmm.
Benjamin A. Baker: I it's cold.
Benjamin A. Baker: It's like, I mean 25 is.
Carlo Parisi: Yeah, it's.
Scott I. Reed: Yeah, but that's one of the ones that's in the
Scott I. Reed: lead.
Benjamin A. Baker: Yeah, but the water loop is right by it.
Scott I. Reed: Be shorted?
Carlo Parisi: Yeah, could get. Yeah, could get that.
Benjamin A. Baker: Potentially.
Carlo Parisi: That temperature is the water loop is 25, yeah.
Benjamin A. Baker: Yeah, it's basically the same as that water
Benjamin A. Baker: loop.
Carlo Parisi: Let me see that.
Carlo Parisi: Where is that not OK, close this.
Scott I. Reed: These are the same as this.
Scott I. Reed: And it's fairly close to that one.
Carlo Parisi: We can't.
Scott I. Reed: So you think maybe it's touching?
Scott I. Reed: It's actually physically touching the coil.
Carlo Parisi: Yeah.
Benjamin A. Baker: Could be, yeah.
Carlo Parisi: Yep.
Scott I. Reed: I would have still thought there would that lead touching it.
Scott I. Reed: It would be pulling all that heat into that metal around it and it would be
Scott I. Reed: somewhere higher than that, but maybe that's the case.
Scott I. Reed: We'll just have to watch it.
Benjamin A. Baker: Either touching or really close and yeah.
Scott I. Reed: But it's it's interesting.
Scott I. Reed: Is there a screen you guys want this on?
Carlo Parisi: I'm checking something here OK?
Carlo Parisi: Let me show the main screen.
Carlo Parisi: Yeah, the main screen I want to see the the
Carlo Parisi: mass flow is going.
Carlo Parisi: K.
Carlo Parisi: Now everything is arising.
Carlo Parisi: OK.
Benjamin A. Baker: Loops are starting to change.
Carlo Parisi: Yep.
Benjamin A. Baker: Because of the one that's really driving it all.
Carlo Parisi: The one that is driving is the blue one, so #4.
Benjamin A. Baker: Thank you.
Carlo Parisi: And we are at one about one thirtyish temperature Celsius.
Carlo Parisi: OK.
Benjamin A. Baker: From the core region, yeah.
Scott I. Reed: 132 right.
Carlo Parisi: Yeah, and yeah, and we have a 1717 kilowatt,
Scott I. Reed: Are you at at the heater's?
Carlo Parisi: right single power.
Carlo Parisi: So.
Benjamin A. Baker: Where are you seeing the kilowatts?
Carlo Parisi: Down there at the center of the screen here totaled the heater power. Yep.
Benjamin A. Baker: The total electrical K so 18 almost.
Scott I. Reed: We want to make sure we're below.
Scott I. Reed: Well, the list that we don't think we're gonna
Scott I. Reed: say. Yeah, I don't think we're going to get any of
Scott I. Reed: these thresholds.
Scott I. Reed: In the heat up to 180, it's the heat up to 450 that's
Scott I. Reed: potentially going to be problematic.
Scott I. Reed: Yes, I have. No.
Benjamin A. Baker: Oh, what's problematic?
Scott I. Reed: When we do the heat, currently we're heating the 180.
Scott I. Reed: When we do the heat up to 450 based on the test that we ran in September with
Benjamin A. Baker: Uh huh.
Scott I. Reed: one foil, it's pretty unlikely that we're going to
Scott I. Reed: be able to get to that point without having the cool.
Scott I. Reed: Boil with only one coolant loop running.
Benjamin A. Baker: The others?
Carlo Parisi: Yeah, what's?
Benjamin A. Baker: Let's see. Kanji pull out enough heat out of it is
Scott I. Reed: This is.
Benjamin A. Baker: what you're saying.
Carlo Parisi: Yeah, yeah, right now.
Scott I. Reed: Hello.
Benjamin A. Baker: Out of a single.
Carlo Parisi: Right now there is basically almost probably very poor heat exchange with the
Scott I. Reed: That that four is dropped and the other is going up.
Carlo Parisi: with the coil because it's everything is solid.
Scott I. Reed: Is it because that was already told a lot of them down the road and they were
Scott I. Reed: stabbing?
Scott I. Reed: Like, yeah, I guess.
Benjamin A. Baker: It's true, yeah.
Carlo Parisi: Scott, can you please put back the screen on the
Carlo Parisi: I checks #4.
Benjamin A. Baker: And I just crossed over.
Benjamin A. Baker: #4 is dropping verse or the other ones going getting hotter.
Carlo Parisi: OK.
Carlo Parisi: It's still still solid.
Carlo Parisi: It's 2075.
Benjamin A. Baker: Oh yeah, because the L BS just gonna solidify.
Carlo Parisi: Yeah. Yeah, it's solidified because water is so cold.
Carlo Parisi: So it's gonna stay probably solid also above 180, that's my guess.
Benjamin A. Baker: Uh huh.
Benjamin A. Baker: 'Cause. I mean it's like 123 is the melting point
Carlo Parisi: Hmm yeah.
Benjamin A. Baker: for LB, right?
Carlo Parisi: Well, yeah, certain point. I mean, I mean this probably the heat transfer
Carlo Parisi: now.
Carlo Parisi: It's very bad there, so it will start probably to melt.
Benjamin A. Baker: Mm hmm.
Benjamin A. Baker: LB. Solid then in all of them right now.
Scott I. Reed: Yes. Yep.
Carlo Parisi: They are all, yeah.
Scott I. Reed: Yeah, it's weird that these are all very
Scott I. Reed: similar on the other down comments, these are all right around 100 but or I
Scott I. Reed: guess we're just pulling out so much meat.
Scott I. Reed: I.
Scott I. Reed: I don't believe this. That doesn't.
Benjamin A. Baker: The 26.
Scott I. Reed: Right.
Scott I. Reed: But I have to say that those were all.
Scott I. Reed: Making sense? Last time we saw them.
Scott I. Reed: This is the first time that one has not made sense,
Scott I. Reed: but but we haven't moved in since.
Scott I. Reed: I don't why it would have gotten damaged anytime recently.
Scott I. Reed: Well, it may be not that damaged, but it might be.
Benjamin A. Baker: I don't believe it's damaged.
Scott I. Reed: It might have been that it was just in the lead and now it's just out of the lid
Scott I. Reed: or something like that maybe.
Scott I. Reed: Maybe.
Benjamin A. Baker: Yeah, it's functional. It's just why?
Benjamin A. Baker: Where is it located?
Benjamin A. Baker: Sort of stuff.
Scott I. Reed: Hi.
Benjamin A. Baker: Let's go.
Carlo Parisi: That's the number 2, right?
Carlo Parisi: The thermocouple that is providing weird.
Carlo Parisi: With the reading, Scott.
Scott I. Reed: Let's see number.
Benjamin A. Baker: 45.
Carlo Parisi: Then, oh, number 45.
Scott I. Reed: Yeah.
Carlo Parisi: So that's the number four it should be.
Carlo Parisi: Yeah, it should be in the on the periphery of
Carlo Parisi: the dog dish there.
Scott I. Reed: That's the one that's on the wall. I don't.
Scott I. Reed: I don't have that thing up in front of me, but.
Carlo Parisi: Yeah, yeah, yeah, yeah.
Carlo Parisi: I just opened on my laptop and yeah, it's on the the one that is on the
Carlo Parisi: periphery of the of the of the dog dish.
Carlo Parisi: So it should be close to the coil, right?
Carlo Parisi: Because coil they are all on the periphery.
Carlo Parisi: I mean most of them, but.
Scott I. Reed: Maybe it's touching the coil.
Scott I. Reed: Yeah, probably is.
Carlo Parisi: Yeah.
Scott I. Reed: And if and if it's touching the coil, that lead is solid, we're saying.
Carlo Parisi: Yeah.
Benjamin A. Baker: It's All in all of EM right now.
Carlo Parisi: Yeah, the yeah, everything is solid.
Scott I. Reed: But you're right.
Carlo Parisi: It's 7070.
Benjamin A. Baker: It's just you got a bigger gradient because of the cold lines and you got
Benjamin A. Baker: heat coming from the ihx coming in through the solid then transferring.
Carlo Parisi: Yep. Yeah. We just have one.
Carlo Parisi: Yeah, one 13113 Celsius. In Upper Plenum there and 67 so.
Benjamin A. Baker: So.
Benjamin A. Baker: What's that?
Benjamin A. Baker: Where's that 113 located?
Benjamin A. Baker: Or 114 the 41.
Carlo Parisi: That one should be there should behave well, yeah.
Benjamin A. Baker: Tc.
Scott I. Reed: That's the inlet to the down Comer.
Carlo Parisi: There should be a Thermo well, right? Yeah.
Benjamin A. Baker: So like in the middle is that in the middle of the wait. Wait. Sorry,
Carlo Parisi: Yeah.
Benjamin A. Baker: that's in the primary right there.
Carlo Parisi: In the primary, correct it's. It's in the in the knock, that is, it's a.
Benjamin A. Baker: OK.
Scott I. Reed: It's the horizontal.
Carlo Parisi: Yeah, there is a Thermo wall that is in the
Carlo Parisi: horizontal part of the yeah.
Benjamin A. Baker: OK.
Benjamin A. Baker: So we got 67 going in 115 coming out on the Mac side.
Carlo Parisi: Mm hmm.
Benjamin A. Baker: What does it look like on three?
Carlo Parisi: Yeah, it's probably worse, huh?
Benjamin A. Baker: Considering there's more flow going there.
Carlo Parisi: That's 115.
Carlo Parisi: But yeah, you have 89 on the down camera, yeah.
Benjamin A. Baker: 89 yeah, and the down Comer is hotter versus the
Carlo Parisi: Yeah. And so you should technically and and now
Benjamin A. Baker: other one.
Carlo Parisi: you should see differences in the mass flow.
Benjamin A. Baker: Yes, well, you got, but you actually have more mass flow on
Carlo Parisi: Should have a less mass flow.
Benjamin A. Baker: all the rest of them.
Carlo Parisi: Yeah. Can you can you go on the mass flow
Carlo Parisi: screen, the main one, yeah.
Benjamin A. Baker: I mean I.
Scott I. Reed: Yeah, four's the lowest.
Benjamin A. Baker: 'Cause I saw it, it changed and number four was dropping.
Scott I. Reed: Yeah, we we saw this when we ran it in the fall.
Carlo Parisi: These are weird.
Benjamin A. Baker: Yeah.
Benjamin A. Baker: So.
Benjamin A. Baker: Yeah, why is it causing more flow rate through
Benjamin A. Baker: the ones that are hotter?
Carlo Parisi: Right. It should be the opposite. Instead of the the number four,
Carlo Parisi: it's the blue one, right?
Scott I. Reed: Right.
Carlo Parisi: Yeah, and yes, the the lowest must flow, that's interesting.
Benjamin A. Baker: And it's obviously the one because the other three are trending in the exact
Scott I. Reed: Good.
Carlo Parisi: Yeah, the other.
Benjamin A. Baker: same way.
Carlo Parisi: Yeah, exactly.
Carlo Parisi: The other one should should have smaller volume.
Carlo Parisi: Maybe it's just a calibration at low mass flow here.
Carlo Parisi: Not sure.
Scott I. Reed: We saw this.
Scott I. Reed: We saw this in the ball as well.
Carlo Parisi: Hmm.
Scott I. Reed: And I, the consensus at the time. Where is it here?
Scott I. Reed: Was.
Scott I. Reed: That it had to do with the lbe heat.
Scott I. Reed: The thermal inertia, once we got past the point where all of
Scott I. Reed: the lbe was molten, then it went back to having the loop with
Benjamin A. Baker: And it changed.
Scott I. Reed: the coolant being the highest flow rate.
Scott I. Reed: I'm I'm fairly certain.
Benjamin A. Baker: In this specific heat or thermal conductivity change from the solid to
Benjamin A. Baker: liquid.
Scott I. Reed: No, it's that.
Scott I. Reed: It's that the heat is trying to melt.
Benjamin A. Baker: And.
Scott I. Reed: The LBE, but it's happening somewhat unevenly
Scott I. Reed: because the coolant is keeping that lbe.
Scott I. Reed: Farther away from the melting point.
Scott I. Reed: So more heat is being absorbed by the lbe.
Scott I. Reed: That's closer to the heating point.
Benjamin A. Baker: Yeah.
Carlo Parisi: Right, but the the but the the, yeah, the question still there because the mass
Scott I. Reed: The melting point.
Benjamin A. Baker: But the questions?
Carlo Parisi: flow on the primary side is proportional to the delta T when you have a natural
Benjamin A. Baker: Yeah. Why is delta T not driving it to be more?
Carlo Parisi: circulation system.
Carlo Parisi: Yeah. So you you would expect, I mean I cannot still explain this
Carlo Parisi: because of the delta T in that loop in those three loops the the 1-2 and three,
Carlo Parisi: it's smaller than the number 4.
Benjamin A. Baker: And it I mean the slope is obviously different there.
Carlo Parisi: Yes. Yeah, yeah, yeah.
Benjamin A. Baker: So even if it was a calibration difference there it it's just purely
Benjamin A. Baker: saying it's absorbing less heat than the ones that are just stationary.
Scott I. Reed: It looks good.
Carlo Parisi: Right.
Scott I. Reed: Control. But if you can something to other things.
Benjamin A. Baker: So that is an interesting phenomena that.
Carlo Parisi: Yeah, I don't.
Carlo Parisi: I.
Carlo Parisi: I don't believe.
Carlo Parisi: I I think it's something probably connected with.
Benjamin A. Baker: Are you sure?
Carlo Parisi: Yeah. Because I mean, I mean, if you want to explain the the natural
Carlo Parisi: circulation on primary side, that's proportional to delta T,
Scott I. Reed: Yeah.
Carlo Parisi: that's the what the physics tell me the mass flow is proportional to the delta T.
Carlo Parisi: And and so we have a larger delta T in loop #4 so.
Scott I. Reed: OK.
Benjamin A. Baker: Right.
Scott I. Reed: And I'll let you know.
Carlo Parisi: Unless, unless there are some changes in the
Carlo Parisi: friction factor as function of temperature.
Carlo Parisi: Loop #4 is operating at a lower temperature and so so that could.
Scott I. Reed: OK, OK.
Benjamin A. Baker: Repeating it on one of the other loops. If it's purely repeatable in other loops,
Carlo Parisi: Come.
Carlo Parisi: Yeah, exactly.
Benjamin A. Baker: then you know it's a physics phenomena.
Carlo Parisi: Yeah, yeah, yeah.
Carlo Parisi: Yeah.
Benjamin A. Baker: Well, I mean, it's physics obviously, but the but is it more?
Carlo Parisi: It's. Yeah, it's.
Benjamin A. Baker: Is it really something that's not being captured besides the Delta T?
Carlo Parisi: Yeah.
Scott I. Reed: It's it's kind of interesting to look at the Delta T across all four of these heat
Scott I. Reed: exchangers because the two, which are what one and two don't have
Scott I. Reed: near the delta T that three and four have.
Benjamin A. Baker: Which delta T are you looking at?
Scott I. Reed: I'm looking at these ones right here.
Scott I. Reed: Between 42 and 47, these two RT DS.
Carlo Parisi: 42.
Benjamin A. Baker: I'm not sure where you're OK. So 42 on #4.
Scott I. Reed: Recruitment flow on the far right.
Scott I. Reed: 42 and 47 here's your delta T.
Scott I. Reed: So the delta T impossible.
Scott I. Reed: Across the coils.
Carlo Parisi: 32O42 and 40.
Benjamin A. Baker: Oh, OK.
Benjamin A. Baker: Oh, so that's a delta already 2°.
Scott I. Reed: And then if you look at #3, it's fairly close.
Benjamin A. Baker: Across.
Scott I. Reed: Well, if you look at 1:00 and 2:00, they don't have.
Scott I. Reed: I just don't know why three has similar Delta T.
Carlo Parisi: Well, number number.
Benjamin A. Baker: But is that all in the noise?
Benjamin A. Baker: Because there's nothing in there, right?
Carlo Parisi: Yeah, there is nothing there.
Carlo Parisi: So that's that's. Yeah, yeah, yeah.
Scott I. Reed: Is that what it is?
Benjamin A. Baker: That's like background.
Benjamin A. Baker: I mean, it's kind of meaningless.
Scott I. Reed: But but this one has.
Scott I. Reed: This one is flowing though.
Carlo Parisi: Yeah, that one is flowing.
Benjamin A. Baker: Yeah, it is flowing.
Carlo Parisi: Yeah, but it's also.
Benjamin A. Baker: It has a half a degree extra beyond noise basically.
Carlo Parisi: Yeah, and. And he's also removing probably a little
Carlo Parisi: a little because.
Carlo Parisi: Everything is solid, you know it's removing heat through
Carlo Parisi: conduction, so it's not very efficient.
Carlo Parisi: But the other one, the other one, it's just noise.
Carlo Parisi: I agree with Ben because if they are empty,
Carlo Parisi: so they're basically measuring the the whole temperature there. So yeah.
Scott I. Reed: OK.
Scott I. Reed: I see alright.
Carlo Parisi: Yeah, that's why I'm. I mean, I think the other screen,
Carlo Parisi: the one with the checks, the lab, they are more interesting because we can.
Carlo Parisi: I mean, we can see what's going on also on the
Carlo Parisi: primary on the secondary and and also on the mass flow, yeah.
Benjamin A. Baker: 19.
Carlo Parisi: This one.
Benjamin A. Baker: I know now we got some areas that are getting up to 110 in this one,
Scott I. Reed: OK.
Benjamin A. Baker: while the other ones are getting close to like the 120 something.
Carlo Parisi: Hmm.
Carlo Parisi: Yeah.
Benjamin A. Baker: So they're getting close to the phase change.
Scott I. Reed: We're in 150, no, at 100 charity.
Carlo Parisi: Yep.
Scott I. Reed: On it.
Carlo Parisi: So now we should.
Scott I. Reed: All I'm done.
Carlo Parisi: Yeah. Now we should see also rise in
Scott I. Reed: Go watch your bees now.
Carlo Parisi: temperature in the water because. Yeah, because.
Scott I. Reed: Sorry, I was looking at the wrong side.
Scott I. Reed: No, let's play.
Scott I. Reed: Like I said, there's only 400 feet 30 of Thermo
Carlo Parisi: I see. Good.
Scott I. Reed: companies in this thing.
Scott I. Reed: I don't know why you're getting so.
Scott I. Reed: But yeah, we're we're at 180.
Benjamin A. Baker: To OK, the flows have stabilized and they're
Benjamin A. Baker: dropping even.
Scott I. Reed: Basically, I mean maybe a little.
Scott I. Reed: I don't think they're dropping a lot.
Carlo Parisi: Yeah, I doubt you have to wait for long.
Carlo Parisi: I mean, for sometimes I would say at least half
Benjamin A. Baker: Even #4 change so.
Carlo Parisi: an hour.
Carlo Parisi: Yeah.
Scott I. Reed: Also no.
Scott I. Reed: This is not a huge range.
Scott I. Reed: I mean, we're talking .047 to . 068 kilograms per second, so.
Benjamin A. Baker: Correct.
Carlo Parisi: Yeah.
Carlo Parisi: Yeah, yeah, I see.
Benjamin A. Baker: Right, I I'm assuming that I I look more at.
Benjamin A. Baker: The slopes and the. So like the slope on the last one was
Scott I. Reed: Trend.
Benjamin A. Baker: clearly different.
Benjamin A. Baker: You know, I didn't care about if I shifted it up
Benjamin A. Baker: and down.
Benjamin A. Baker: Umm.
Benjamin A. Baker: But as kind of a reasonability test.
Benjamin A. Baker: So.
Benjamin A. Baker: In the.
Scott I. Reed: Where we got the 180.
Carlo Parisi: Yeah, let's let's stay here for some time
Carlo Parisi: because I think they're still heating up.
Benjamin A. Baker: How close are the other ones to the melting points?
Carlo Parisi: Yeah, number.
Scott I. Reed: That's we're right around the melt, the melting.
Carlo Parisi: Yeah.
Benjamin A. Baker: Right around the melting point right now.
Carlo Parisi: Yeah. So you will need some time, yeah.
Benjamin A. Baker: I don't how much.
Benjamin A. Baker: The whatever it's called heat of fusion or whatever.
Carlo Parisi: Yeah.
Benjamin A. Baker: You kind of energy that that takes.
Scott I. Reed: For it to transition from a solid to a liquid.
Carlo Parisi: Yeah, this is quite yeah.
Benjamin A. Baker: Hmm, well, they're not.
Benjamin A. Baker: They're obviously not all that different though,
Benjamin A. Baker: meaning whether you have a liquid flowing in there and cooling it down or.
Benjamin A. Baker: Just letting it stay stagnant.
Benjamin A. Baker: I guess it's solid regardless of all of that.
Benjamin A. Baker: In this whole region.
Carlo Parisi: Number two, yeah, #2 is starting to liquefy. Yeah.
Scott I. Reed: And they they're saying that it.
Carlo Parisi: Power is 25 kilowatts, so OK.
Carlo Parisi: Nowhere.
Carlo Parisi: Decent amount of power.
Benjamin A. Baker: So again, Carlos Scott Gibson.
Scott I. Reed: What?
Scott I. Reed: Oh yeah.
Benjamin A. Baker: Sorry I didn't say the name.
Scott I. Reed: Stable point.
Benjamin A. Baker: But is there a flow meeting the flow meters right now?
Carlo Parisi: Yeah.
Benjamin A. Baker: So we have one loop.
Benjamin A. Baker: Water lines.
Benjamin A. Baker: The other two are just having solid LD.
Benjamin A. Baker: Solid unfortunately too, but.
Benjamin A. Baker: We just have one.
Benjamin A. Baker: Cool it down.
Benjamin A. Baker: Watch em. The differences right now.
Benjamin A. Baker: So to tell you right now, this is it's always about.
Benjamin A. Baker: So if you could link back.
Benjamin A. Baker: The same.
Benjamin A. Baker: Login that's sending all the signals to the pins and.
Benjamin A. Baker: Yeah, adjusted.
Benjamin A. Baker: So right now, face changes occurred to get the LP.
Benjamin A. Baker: So.
Benjamin A. Baker: I'm curious to see how these three vary from this one that has the water on it as
Benjamin A. Baker: they liquefy, and this one remains solid.
Scott I. Reed: Well, we we have those results from September.
Benjamin A. Baker: Oh, you do.
Benjamin A. Baker: It's a little different when you're, like watching it, you know,
Benjamin A. Baker: versus looking at raw data.
Benjamin A. Baker: Raw data you see the whole thing, but while it's happening.
Benjamin A. Baker: You're thinking about it.
Benjamin A. Baker: I have Tony here.
Benjamin A. Baker: I'm at Tony's lab.
Scott I. Reed: OK.
Benjamin A. Baker: OK.
Scott I. Reed: Yeah, but so far this is looking exactly like
Scott I. Reed: it did in September.
Benjamin A. Baker: OK.
Scott I. Reed: And once they all melt.
Scott I. Reed: Four went back up to a higher blow rate.
Benjamin A. Baker: OK.
Benjamin A. Baker: Right now we're sitting around .05.
Benjamin A. Baker: I forgot the units on that.
Benjamin A. Baker: Kilograms per second, OK.
Scott I. Reed: And honestly that I mean .05.
Scott I. Reed: That's the that's the absolute low end of the point at which the flow meters were
Scott I. Reed: calibrated at so.
Benjamin A. Baker: Right. I'm sure they're good to lower.
Benjamin A. Baker: That was just the data point though, right?
Scott I. Reed: Yes, yes.
Carlo Parisi: Scott, can you please go to the screen of the
Carlo Parisi: Dih X? The lab thing is a down camera.
Carlo Parisi: Yeah, this one. OK, this number one.
Carlo Parisi: #4.
Carlo Parisi: It's creating a large delta T of those coils and see 55.
Carlo Parisi: #4 the number 4.
Carlo Parisi: Yeah. Again, it's the one on the dog dish.
Carlo Parisi: And.
Carlo Parisi: #5. He's the one at the center of the dog
Carlo Parisi: dish, so 26.
Carlo Parisi: Yeah. OK.
Scott I. Reed: That that's got to be touching a coil or something like that.
Carlo Parisi: Yeah, yeah, yeah.
Benjamin A. Baker: Yeah.
Carlo Parisi: Because it's the one that is at the center.
Carlo Parisi: It just op on top of the down camera of the ihx.
Scott I. Reed: Yeah.
Carlo Parisi: Let me see the other one that are on the bottom or number one. So number one,
Carlo Parisi: that is it's 115, OK.
Carlo Parisi: Yeah, that makes sense because that is is down
Carlo Parisi: in the lower part of the ihx.
Scott I. Reed: Yeah, that's that's the bottle.
Carlo Parisi: Mm hmm.
Carlo Parisi: Yeah. And we have.
Carlo Parisi: We have 7070°.
Scott I. Reed: But.
Carlo Parisi: I mean one almost.
Carlo Parisi: No, no, no.
Carlo Parisi: 90° of Delta T across the yeah on the neck.
Benjamin A. Baker: Face on the neck.
Carlo Parisi: So again, this is like a mystery.
Carlo Parisi: Why the I don't see a a bigger mass flow?
Carlo Parisi: This loop.
Benjamin A. Baker: 90 versus the other ones have one.
Carlo Parisi: Yeah, the other one.
Carlo Parisi: Yeah. If you go to down camera number one for
Carlo Parisi: example.
Carlo Parisi: #2 is it's OK.
Benjamin A. Baker: To begin with, then 50.
Carlo Parisi: Yeah, here I have. Just fifty. Yeah.
Benjamin A. Baker: 90 versus 50.
Carlo Parisi: Yeah.
Carlo Parisi: Rest.
Carlo Parisi: Yeah, it could be the calibration or whatever,
Carlo Parisi: yeah.
Carlo Parisi: 125 S This other guys, they start to melt right now.
Carlo Parisi: Yeah, 126.
Carlo Parisi: Yeah, actually there is also 150.
Carlo Parisi: So they're partially melted, yeah.
Benjamin A. Baker: Melted.
Scott I. Reed: Yeah, they've, they've, they definitely started to melt.
Benjamin A. Baker: Down.
Carlo Parisi: #4 is dropping now interest.
Carlo Parisi: OK.
Carlo Parisi: That's really.
Benjamin A. Baker: I'll repeat on one of the other ones to tell you.
Carlo Parisi: Yeah, exactly.
Carlo Parisi: That would be really interesting to rerun on.
Carlo Parisi: I don't know #1 and see how it goes.
Benjamin A. Baker: Yeah.
Carlo Parisi: The problem then is, yeah, we probably need to drain the loop #4.
Carlo Parisi: Yeah. Hmm.
Carlo Parisi: Yeah, we should have started another loop
Carlo Parisi: instead of #4 since we did this in last four.
Carlo Parisi: As I'm thinking about.
Benjamin A. Baker: 3rd.
Scott I. Reed: 5555.
Carlo Parisi: So we're at 20 kilowatt K.
Scott I. Reed: Just a heads up to everybody on the line.
Scott I. Reed: They're about to run some other tests in here.
Scott I. Reed: We don't anticipate any issues, but it's the first time we're they're
Carlo Parisi: Mm hmm.
Scott I. Reed: going to be running that system.
Scott I. Reed: So if you start hearing alarms and or yelling and then people running.
Benjamin A. Baker: Yeah.
Carlo Parisi: OK.
Scott I. Reed: We may not be on the line immediately afterwards, so.
Carlo Parisi: OK.
Scott I. Reed: I don't anticipate anything like that will happen, but.
Benjamin A. Baker: OK.
Scott I. Reed: It's R&D work so.
Carlo Parisi: OK.
Carlo Parisi: If we if we hear a bang, we know what's going on.
Benjamin A. Baker: Let you get out, and then we'll call you.
Scott I. Reed: Hey. Hey, right.
Benjamin A. Baker: OK.
Carlo Parisi: This system is not noisy as the the engine.
Carlo Parisi: That's.
Scott I. Reed: Yeah, that's that's definitely Moulton.
Carlo Parisi: Yeah, OK. Yeah.
Carlo Parisi: 150, OK.
Scott I. Reed: It should start.
Scott I. Reed: They should all start shooting up now.
Carlo Parisi: Yeah.
Scott I. Reed: But that's that's almost definitely Moulton. This is based on these temps.
Carlo Parisi: No.
Scott I. Reed: This is the one the the lbe and four is probably starting to melt.
Carlo Parisi: Yeah, it's interesting the hmm.
Carlo Parisi: The dog dishes seems solid.
Carlo Parisi: And the rest of the ihx is liquid.
Scott I. Reed: They brought that over those guys in case something happens.
Carlo Parisi: Yeah, too. Too bad we cannot have.
Carlo Parisi: Have a look there.
Scott I. Reed: And now 1-2 and three are all starting to drop.
Scott I. Reed: Because the LDS already molten.
Scott I. Reed: Again, that's the same thing we saw in September.
Scott I. Reed: So they're starting to stabilize.
Scott I. Reed: No longer changing the rate at which oil.
Scott I. Reed: OK.
Scott I. Reed: I mean, that was our supposition in in the fall,
Carlo Parisi: Hmm.
Scott I. Reed: so.
Scott I. Reed: Again, four will start to go past it again.
Scott I. Reed: Once once 4 is Moulton.
Scott I. Reed: But these temps are all rock solid.
Scott I. Reed: This wattage is slowly tapering off now that this has all been molten.
Scott I. Reed: In one, three and four, sliding behind can't stop the coolant,
Scott I. Reed: but it's slightly ripe.
Carlo Parisi: Mm hmm.
Scott I. Reed: Yeah, that lbe has a lot of thermal mass.
Scott I. Reed: I mean, it has a lot of regular mass too, but.
Scott I. Reed: Is that just a test?
Scott I. Reed: Oh, OK.
Scott I. Reed: You have six, you have 6.
Scott I. Reed: I'd suppose.
Scott I. Reed: That's actually it's an off gas, but.
Scott I. Reed: Something really, I think it's real.
Scott I. Reed: Yeah, but they're so the goal is to recover the
Scott I. Reed: delinia.
Scott I. Reed: Which then you could recycle.
Scott I. Reed: Right now, I think they just put some cylinders in
Scott I. Reed: the desert.
Scott I. Reed: Yes, it's in the.
Carlo Parisi: Scott, can you please go to down camera #4?
Carlo Parisi: Josh, there is no way that we can have a look
Carlo Parisi: to what's going on in those on those.
Carlo Parisi: Checks #4 right. It's sealed.
Scott I. Reed: He can't do anything. Gets he can't see in there.
Carlo Parisi: Hmm.
Scott I. Reed: Even if you did, all you'd see was lead.
Carlo Parisi: Yeah. No, I want just.
Carlo Parisi: I was just wondering if some of the ladder there is is melted around those
Scott I. Reed: Yeah.
Carlo Parisi: coil cause from what I see from the from the thermocouple that doesn't seems the
Carlo Parisi: case because I see Twentyfour 2756.
Carlo Parisi: I'm not sure I'll, I'll.
Carlo Parisi: I'll can trust those number because the rest of the system, yeah.
Scott I. Reed: Yeah, there's 40.
Scott I. Reed: There's 46 is the one that's clear down in the tube cause furthest down in the
Scott I. Reed: down Comer right.
Carlo Parisi: 46.
Scott I. Reed: You've had me sure.
Carlo Parisi: Yeah, it's the one at the middle of the down
Carlo Parisi: camera.
Carlo Parisi: Actually, sorry in the middle of the racing pipes.
Scott I. Reed: Yeah. Sorry, right.
Carlo Parisi: Yeah.
Scott I. Reed: I you know, in hindsight, I wish I'd thrown that picture on top of
Scott I. Reed: that thing on off the side of the street.
Carlo Parisi: Yeah, we're just probably the best thing to do
Carlo Parisi: is to print and to keep on the desk.
Carlo Parisi: Yeah, but the.
Carlo Parisi: Yeah, numbers number six is the one at the mid
Carlo Parisi: in the middle of the.
Carlo Parisi: Erasing racing straight pipe.
Scott I. Reed: Yeah.
Carlo Parisi: And number one is the one on the bottom.
Scott I. Reed: Yeah. They don't really follow any kind of
Scott I. Reed: logical pattern.
Carlo Parisi: Number one is on the bottom, so it's 126.
Scott I. Reed: One is at the bottom, 6 is halfway down.
Carlo Parisi: Yeah.
Carlo Parisi: And #3.
Carlo Parisi: Is at the end.
Scott I. Reed: Two and two and three are at the base of the bowl, and four or five at the top.
Carlo Parisi: Yeah, yeah.
Carlo Parisi: 4-5 at the top, yeah.
Carlo Parisi: Yeah.
Scott I. Reed: Yeah, these are still.
Scott I. Reed: Staying pretty, pretty solid, the Delta T's 2 1/2. Still not that much.
Scott I. Reed: Yep, see.
Scott I. Reed: I love you. Drive.
Scott I. Reed: Cool.
Scott I. Reed: Put it in a Bloomberg.
Scott I. Reed: I sent it to this white boy, please.
Scott I. Reed: Show up.
Scott I. Reed: Peter wattage down below 14 kilowatts.
Scott I. Reed: That is.
Scott I. Reed: No #6 or #3 wishing.
Scott I. Reed: Four should be the hottest 04 or five.
Scott I. Reed: Well, it's a lot of fun.
Scott I. Reed: Number six.
Scott I. Reed: Is that because once you get out?
Scott I. Reed: That's where it comes in and then goes down.
Scott I. Reed: Well, yeah. I mean, it's coming in 'cause you're you're
Scott I. Reed: picking up tea as you go by. You got heat rising right on the outside
Scott I. Reed: of this. Well inside of it.
Scott I. Reed: The cool stuff's going back down.
Scott I. Reed: So your heat gets hotter, but then right here you have your heat
Scott I. Reed: exchanger coil that's pulling heat out as well, right?
Scott I. Reed: So somewhere in here, a hot spot, it's got to be that.
Scott I. Reed: 4-5 has to be touching the floor.
Scott I. Reed: Unless it's shorted somewhere, it has to be hunting before it.
Carlo Parisi: So you think that the the lat is liquid there Josh?
Scott I. Reed: What was the question you think is the is the left liquid do you think?
Carlo Parisi: In the dog dish.
Scott I. Reed: It may not be 100%, but I I definitely think it's pretty
Scott I. Reed: close.
Scott I. Reed: 'Cause it melts at 120 ish 125.
Scott I. Reed: South, yeah, there might be a couple.
Scott I. Reed: There might be a little bit of residual, but it it's almost certainly.
Scott I. Reed: Mostly molten, because the one that's in the down the
Scott I. Reed: return center.
Scott I. Reed: And #2 it's at 102, so it's not acting like it's liquid yet,
Scott I. Reed: right?
Carlo Parisi: Yeah, correct.
Scott I. Reed: Yeah.
Scott I. Reed: And then #4.
Scott I. Reed: This is what side of the bed she acts like this. Not with but.
Scott I. Reed: Text me.
Scott I. Reed: That's 58.
Carlo Parisi: Yeah.
Scott I. Reed: But it appears to be measuring temperature.
Scott I. Reed: It's not broken. If it was broken at the open.
Scott I. Reed: Yeah.
Scott I. Reed: I don't know.
Scott I. Reed: 44 is a weird 145. Is it just? It has to be touching it for it.
Scott I. Reed: Does that mean that 44 is also near it?
Scott I. Reed: Well, it is near equals.
Scott I. Reed: And the coil.
Scott I. Reed: So maybe it's just coils not too close enough that it's not.
Scott I. Reed: Let me put the pool in the other loops in basically the same kind of thing happens.
Scott I. Reed: That will.
Scott I. Reed: The hard part is, though, some of Paramoles aren't going to be
Scott I. Reed: exactly what they say.
Scott I. Reed: You were patient, so you could have that one actually
Scott I. Reed: touching the coil and the next one that's. I'm not saying it'll necessarily always
Scott I. Reed: be by.
Scott I. Reed: That's touching.
Scott I. Reed: But if you have the ones that are in the upper ones right where you think.
Scott I. Reed: So overall.
Scott I. Reed: We're down to 11 kilowatts.
Scott I. Reed: Oh, that's weird.
Scott I. Reed: 51 coming up now.
Scott I. Reed: You know, the hard part is you almost have to have
Scott I. Reed: to have a graph that has everything on it so you can see what everything's doing
Scott I. Reed: 'cause. It's hard to flip back and forth to these
Scott I. Reed: screens.
Scott I. Reed: Yeah, it's just.
Scott I. Reed: I don't know why this man.
Scott I. Reed: I mean, it apparently must be pulling more heat,
Scott I. Reed: right?
Scott I. Reed: Yeah, but why does it appear to be pulling more
Scott I. Reed: heat? If you look at, I mean, that's what this says.
Scott I. Reed: Yeah, but if you look at the other springs,
Scott I. Reed: does that bear out?
Scott I. Reed: That's returning at 1:32.
Scott I. Reed: Stingy pen.
Scott I. Reed: That was a little lower.
Scott I. Reed: I mean, we won't know that the lbe is entirely
Scott I. Reed: molten until our return temperature is above the LP.
Scott I. Reed: It's pretty to be absolutely 100% molten.
Scott I. Reed: Now it's dipping down again.
Scott I. Reed: It's just, I don't know why that.
Scott I. Reed: Unless you get Chloe.
Scott I. Reed: Yeah, that's a BLOB of molten LBD.
Scott I. Reed: On molten LV just sounds like an ice cube.
Scott I. Reed: Yeah, the last ice cube in the glass floating
Scott I. Reed: around.
Scott I. Reed: Maybe.
Scott I. Reed: Hello, Carl.
Carl E. Baily: How's it going out there?
Scott I. Reed: Carl.
Scott I. Reed: It's going you tell us.
Carl E. Baily: Yeah.
Scott I. Reed: We are wondering when you wanted to fly out.
Carl E. Baily: I don't.
Carl E. Baily: I'm flying the other way for a couple of weeks.
Scott I. Reed: Arya, where are you going?
Carl E. Baily: Honolulu.
Carlo Parisi: Much better place.
Scott I. Reed: Now, wait a minute. That's that's not quite fair.
Carlo Parisi: Yeah, it's oddly.
Carl E. Baily: I I know I didn't want to mention it, but you asked.
Scott I. Reed: We need to see if Justin will put the P cat in Honolulu next time. I'm for it.
Carlo Parisi: Yes.
Carlo Parisi: Definitely.
Scott I. Reed: We'll get C idle Op, Open an office over there.
Carl E. Baily: Now if later on.
Scott I. Reed: I'm more than willing to have that conversation.
Carl E. Baily: I'll need to go into your supervisor or whatever.
Carl E. Baily: So is everything working?
Carlo Parisi: So far, yeah.
Scott I. Reed: Everything might be a bit of a stretch.
Scott I. Reed: We've got a couple thermocouples that.
Scott I. Reed: We think are either touching or really close to a coolant loop.
Carl E. Baily: Oh, OK. I was wondering about that.
Scott I. Reed: Yeah, yeah, I think everything is working.
Scott I. Reed: It just may not be what we expected.
Scott I. Reed: Yeah, that's that's the biggest.
Carl E. Baily: OK.
Scott I. Reed: That's the biggest I guess issue at this point.
Carlo Parisi: Unless those call, they are creating a kind of blog of.
Carlo Parisi: Of a solid solid lad because they are so cold.
Carlo Parisi: And so we have those Thermo couple in the solid lat.
Carl E. Baily: Yeah, it's not that.
Carl E. Baily: It's just that I think when I wrote.
Carlo Parisi: And all around the data is a liquid, and so the heat is flowing from the
Carl E. Baily: This.
Carlo Parisi: liquid to the solid, and then to the coil.
Carl E. Baily: I just want.
Carlo Parisi: You know what I mean?
Carlo Parisi: It's like when you you put some, you freed some, some water.
Carl E. Baily: That launched this all of a sudden.
Carlo Parisi: Yeah, I mean you have to coil that are super
Carlo Parisi: cold and you freeze the water around the coil.
Scott I. Reed: Yeah.
Carl E. Baily: That's all I have, so I have the master spreadsheet.
Carl E. Baily: I don't understand.
Scott I. Reed: I was probably scared, probably wireless.
Carl E. Baily: Updated the formulas if that's if that's true.
Carl E. Baily: You should clear that up once you get to a higher.
Carl E. Baily: Input power.
Carlo Parisi: Yep.
Carlo Parisi: Yeah, now it's dropping at 8 kilowatt, sure.
Scott I. Reed: What's the weather like?
Scott I. Reed: Yeah. Again, these blow rates are all quite low.
Scott I. Reed: Communicate with them.
Carl E. Baily: We followed it.
Carl E. Baily: Oh yeah.
Carl E. Baily: That was perfect.
Carl E. Baily: God protection.
Carl E. Baily: Shut up.
Scott I. Reed: Hi can you help?
Scott I. Reed: Me.
Carl E. Baily: Thanks for that.
Scott I. Reed: Barely heating it up at all.
Scott I. Reed: This one's a little hotter. 'cause that's that's the 3/8 inch tube.
Scott I. Reed: These are half inch tube. So you got little less mass.
Scott I. Reed: To surface area ratio.
Scott I. Reed: That's why that's heating up a little more.
Scott I. Reed: The other one is no, it's actually the inner one.
Scott I. Reed: Was this one?
Scott I. Reed: Maybe I have it backwards.
Scott I. Reed: I mean, if she looked the way we did this.
Scott I. Reed: That's your inner 10, right?
Scott I. Reed: I'm sorry.
Scott I. Reed: So yeah, I had that balance.
Scott I. Reed: So this one doesn't have another cooler cooling coil on the other side.
Scott I. Reed: Right. So that's why to help it along.
Scott I. Reed: Now, now I'll return Tim.
Scott I. Reed: Is getting to our LBP melt temp.
Scott I. Reed: This is still lagging a little bit, but you can get about 120.
Scott I. Reed: Basically just at this point, we're waiting for it to reach equilibrium,
Scott I. Reed: right?
Scott I. Reed: It doesn't.
Scott I. Reed: It doesn't specifically say to do so, but that's what I that's what I assume
Scott I. Reed: you wanted to happen here, right, Carlo?
Scott I. Reed: Hello.
Carlo Parisi: Oh yeah. Sorry I was muted.
Carlo Parisi: Yeah, I said yes.
Carlo Parisi: To keep in my mind, Michael.
Scott I. Reed: So we'll we'll let this go to equilibrium and then?
Scott I. Reed: And we'll try bumping up the tents.
Carlo Parisi: Yeah, still 7 kilowatts now.
Carlo Parisi: How is?
Carlo Parisi: How is the water temperature in the loop 4D T?
Carlo Parisi: Yeah, the coil if yeah, the glycol temperature, yeah.
Scott I. Reed: Did you see the glycol?
Scott I. Reed: Oh.
Carlo Parisi: Let me scroll.
Scott I. Reed: The opportunity across the call.
Carlo Parisi: So you have 27 and 24, so you have 3 three Celsius.
Carlo Parisi: Of Delta T basically OK.
Scott I. Reed: And that's saying.
Carlo Parisi: And Joshua, just for my understanding is so the water
Scott I. Reed: Thank you.
Carlo Parisi: right now is flowing uniformly.
Carlo Parisi: I mean, it's flowing across all the four corners,
Carlo Parisi: right?
Scott I. Reed: Yes, all, yes.
Carlo Parisi: OK.
Carlo Parisi: They're all open, OK.
Carlo Parisi: And then eventually we can go and do some partitioning.
Carlo Parisi: Or OK.
Carlo Parisi: Can you regulate each coil or you have just evolve for throttling the flow on
Carlo Parisi: the Vol 4?
Scott I. Reed: 'Cause on each individual coil.
Carlo Parisi: Oh, OK.
Carlo Parisi: So you can do it right.
Carlo Parisi: Fine.
Scott I. Reed: Yeah, we we weren't sure how granular you might
Scott I. Reed: want to have it. As far as the controls and pricing back.
Carlo Parisi: Yeah.
Scott I. Reed: So we kind of went as far as we could get pointing as hard as you can write a
Scott I. Reed: document, what you've done seven turns here and
Carlo Parisi: Yeah.
Scott I. Reed: three turns there and.
Carlo Parisi: Yeah, I don't know.
Carlo Parisi: I agree, but yeah, it's good that we have.
Scott I. Reed: So not necessarily letting you go.
Carlo Parisi: I'm. I'm seeing that there is one call that is
Carlo Parisi: at 30 and the other one that are all 24242630.
Carlo Parisi: So it seems there is a call that. Yeah, yeah, so prior.
Scott I. Reed: That's your outside coil.
Scott I. Reed: So yeah.
Scott I. Reed: So you're going from inside to outside.
Carlo Parisi: OK.
Carlo Parisi: Makes sense?
Carlo Parisi: The flow of lead should be from outside to inside OK.
Carlo Parisi: Yeah, it's too bad that we cannot have a look
Carlo Parisi: what's going on there, I mean.
Scott I. Reed: That we can't have a what we.
Carlo Parisi: That we can not have a look to. What? What's going on?
Carlo Parisi: I mean, how?
Scott I. Reed: Oh, oh, look. OK.
Carlo Parisi: How do the yeah, yeah, look. Yeah.
Scott I. Reed: Yeah, we didn't.
Scott I. Reed: We didn't build it with internal cameras.
Scott I. Reed: Well, we should have made it have, like, a clear material like quartz.
Carlo Parisi: Yeah, yeah.
Scott I. Reed: That'd be cheap, yes.
Carlo Parisi: Yeah.
Scott I. Reed: We've done that with some other operation.
Scott I. Reed: I see those windows and things, but that's they're usually like.
Scott I. Reed: Yeah, cyber or $0.50 or something.
Carlo Parisi: OK.
Scott I. Reed: I'll build a fist.
Scott I. Reed: It's so different from this.
Carlo Parisi: Yeah, 148, so yeah, definitely.
Carlo Parisi: Yeah. Melted.
Scott I. Reed: And we shouldn't be losing any here.
Scott I. Reed: Maybe if you're actually author, yeah, it's going.
Scott I. Reed: Is it that way? All of them?
Carlo Parisi: You want then OK.
Carlo Parisi: Yeah, open the other one.
Carlo Parisi: OK, they are all 190 OK, the other one.
Scott I. Reed: See this one.
Scott I. Reed: Supposedly is in 20°.
Carlo Parisi: OK.
Scott I. Reed: Now why it's losing that much? I don't know. There's nothing.
Scott I. Reed: I mean, well, it makes me wonder, is are we sure the right one's plugged
Scott I. Reed: into the right spot? 'cause. It's from the Jack panel back.
Scott I. Reed: Somebody ever unplugged and put them back in the wrong spot?
Scott I. Reed: We haven't done that replication for a long time now. I mean,
Scott I. Reed: last time we checked, that stuff was forever physical.
Scott I. Reed: Check those all the way back and I was like, early on in the two.
Scott I. Reed: I mean, I guess it's possible.
Carlo Parisi: Yeah, what?
Carlo Parisi: What is that temperature there? On the 42, it's.
Scott I. Reed: 110.
Carlo Parisi: Yeah, no.
Carlo Parisi: Yeah, exactly.
Carlo Parisi: Yeah, 110.
Carlo Parisi: Yeah, because you have 130 there, yeah.
Scott I. Reed: Yeah, that's the temperature underneath the
Carlo Parisi: Does make sense?
Scott I. Reed: insulation.
Scott I. Reed: I mean, I could go in a while.
Carlo Parisi: Yeah, that's no temperature, right?
Scott I. Reed: And to verify that I can walk over and unplug the one that's that one and watch
Scott I. Reed: it go sky High.
Scott I. Reed: Or I can go hand over hand to it's truly plugged back in that 4243 aren't swapped
Scott I. Reed: on that end.
Carlo Parisi: Yeah, because it doesn't make sense that that.
Scott I. Reed: It is.
Scott I. Reed: It is odd that on all the other ones it's 20° difference the other way.
Carlo Parisi: Yeah.
Scott I. Reed: You can go what?
Scott I. Reed: Hello.
Scott I. Reed: Zero, 32 and that's down colour #4.
Scott I. Reed: 2:43.
Scott I. Reed: That's at the top.
Scott I. Reed: Of the waterfalls.
Scott I. Reed: Big difference.
Scott I. Reed: Down below 6 kilowatts.
Scott I. Reed: Yeah.
Scott I. Reed: Thank you.
Scott I. Reed: What's wrong?
Scott I. Reed: O 42 is definitely the one up top and O 43 is definitely the one on the bottom.
Scott I. Reed: OK.
Scott I. Reed: Now what?
Scott I. Reed: I don't know is.
Scott I. Reed: 'Cause those see oh, 43.
Scott I. Reed: That's the one that we remember. We had the issue with the amount of space
Scott I. Reed: there was between the magnet and we had to change those out for the MBS ones.
Scott I. Reed: You guys can solve later.
Scott I. Reed: Remember that.
Scott I. Reed: Very little room in that spot.
Scott I. Reed: But was that different for number 4 then versus the other? No, I'm just saying.
Scott I. Reed: Those have been I I wasn't here when we installed those.
Scott I. Reed: The only thing I can think is that maybe it's not in the thermal well.
Scott I. Reed: Like the others on one of those two, it was #4.
Scott I. Reed: We had a question on that.
Scott I. Reed: Thing is, what I don't know is, is it possible that 42 isn't in this blue?
Scott I. Reed: We could.
Scott I. Reed: We could loosen it.
Scott I. Reed: Try that.
Scott I. Reed: Sanetta is a is that a spring bayonet?
Scott I. Reed: No.
Scott I. Reed: There went up a little bit.
Scott I. Reed: Going up.
Scott I. Reed: Josh, I need it in that bar.
Scott I. Reed: That thing is there's nothing hold. I don't think the.
Scott I. Reed: Switch speed are in there or it's up to 130 already. Like I said,
Scott I. Reed: it was clear it was clear.
Scott I. Reed: I don't.
Scott I. Reed: Oh, it makes me worried though.
Scott I. Reed: I don't know if that was that loose or the other ones.
Scott I. Reed: That's great to know though, like I can see it all the.
Scott I. Reed: Oh.
Scott I. Reed: Well.
Scott I. Reed: Alright, restart.
Scott I. Reed: Restart it.
Scott I. Reed: Yeah.
Scott I. Reed: Oh.
Scott I. Reed: I mean, it's up to 140 now.
Scott I. Reed: This one.
Scott I. Reed: So that thermocouple wasn't the whole way in the end of thermal well.
Scott I. Reed: But still, that's a really small delta T.
Scott I. Reed: But uh.
Scott I. Reed: Down to 4500 kilowatts, or 4 1/2 kilowatts.
Scott I. Reed: Hey, Ben, can you hear for a minute?
Scott I. Reed: Yeah, it's me.
Scott I. Reed: That's my last name, yes.
Scott I. Reed: OK.
Scott I. Reed: Looking like baseball there.
Scott I. Reed: Better.
Scott I. Reed: Hold it in there and wrap some tape tape around it.
Scott I. Reed: Well, wait.
Scott I. Reed: Wait until. Oh, there's Scott.
Scott I. Reed: I don't know.
Scott I. Reed: I mean, really.
Scott I. Reed: It.
Scott I. Reed: There's.
Scott I. Reed: This is government, so.
Scott I. Reed: I want to look at it again.
Scott I. Reed: Over their millimeter.
Scott I. Reed: Correct.
Scott I. Reed: OK.
Scott I. Reed: Let's prepare to talk to him about.
Scott I. Reed: Correct.
Scott I. Reed: Did you eat well? It sounds awesome.
Scott I. Reed: Sounds terrible.
Scott I. Reed: Hey.
Scott I. Reed: I will be there.
Scott I. Reed: Tomorrow.
Scott I. Reed: It's needed to bulk.
Scott I. Reed: We're fiddling with the thermocouple now. That's why the temperature keeps changing.
Scott I. Reed: 15401.
Scott I. Reed: Bottom down and ******* bottom, you can go away.
Scott I. Reed: Another one is blue America.
Scott I. Reed: This one.
Scott I. Reed: Is.
Scott I. Reed: It's been way too long, remember.
Scott I. Reed: If anything was going to hit him.
Scott I. Reed: But I would have to pay.
Scott I. Reed: Like higher wage jobs?
Scott I. Reed: Correct me a here.
Scott I. Reed: Yeah, but I like red.
Scott I. Reed: Actually I don't know if he installed ever.
Scott I. Reed: Did they install? I'm not sure.
Scott I. Reed: I'm not sure.
Scott I. Reed: I.
Scott I. Reed: I don't.
Scott I. Reed: I don't recall.
Scott I. Reed: Tell me about your voice.
Scott I. Reed: You want to spend more, you know.
Scott I. Reed: Yeah.
Scott I. Reed: Time this one was not seen.
Scott I. Reed: I wrote it down.
Scott I. Reed: Yeah, 'cause, it was 42.
Scott I. Reed: So we identified why Pcto 42.
Scott I. Reed: Was reading low.
Carlo Parisi: Mm hmm.
Scott I. Reed: It it wasn't pushed into the thermal well fully.
Carlo Parisi: OK.
Scott I. Reed: So we found that the the ferrule on the OR I guess the thermocouple or or the
Scott I. Reed: thermal. Well one of those two is not sized
Scott I. Reed: appropriately.
Carlo Parisi: OK, that would explain why we were unable to
Carlo Parisi: understand the mass flow because those delta T that were not,
Scott I. Reed: Now it's.
Carlo Parisi: they were not realistic.
Scott I. Reed: Yeah. Does that make sense now, 'cause, now you're looking at 42.
Carlo Parisi: Yes.
Scott I. Reed: It's at 139 and the one below it's 137.
Carlo Parisi: Yes, yes.
Scott I. Reed: Yeah, it is still odd that there's a A1 to two
Carlo Parisi: Yeah.
Scott I. Reed: degree delta T here.
Scott I. Reed: Now the one thing about it, we may still have a problem between with
Scott I. Reed: some of these other ones too like 23.
Scott I. Reed: Maybe we should go make sure that all of those are pushed in because those are
Scott I. Reed: fighting gravity.
Scott I. Reed: Ones from underneath.
Scott I. Reed: So look at those.
Carlo Parisi: OK.
Scott I. Reed: But big picture, this continues to slowly separate and
Scott I. Reed: we're less than 4 kilowatts.
Scott I. Reed: Actually I'm not so sure that's true, yes.
Scott I. Reed: But we are at least rock steady at 180.
Carlo Parisi: Can I see?
Carlo Parisi: Yeah, yeah.
Carlo Parisi: Can I see the number four, the lat bismuth and the?
Carlo Parisi: OK.
Carlo Parisi: So here.
Scott I. Reed: Yeah, this is a delta T.
Scott I. Reed: Like what I would expect.
Scott I. Reed: Because there shouldn't be much temperature loss here.
Carlo Parisi: Yes, exactly. Yeah.
Scott I. Reed: Because this this has crazy insulation on it.
Carlo Parisi: Yeah.
Carlo Parisi: Yeah, once the installation reach temperature
Carlo Parisi: should be all all the same. Almost yeah.
Carlo Parisi: OK, up there.
Carlo Parisi: OK, seems the.
Carlo Parisi: Temperature are also stable.
Carlo Parisi: In the.
Carlo Parisi: In the I checks.
Scott I. Reed: So they're gonna try and.
Scott I. Reed: Just do a double check on the other Thermo couples.
Carlo Parisi: OK, sounds good.
Scott I. Reed: The other.
Scott I. Reed: 3323 and 13.
Scott I. Reed: To see why those three all have such a such a higher delta T.
Carlo Parisi: Right.
Scott I. Reed: But the good news is our plenum temperatures.
Scott I. Reed: Are all very similar.
Scott I. Reed: So that seems to me that we should be getting the equilibrium.
Carlo Parisi: Yeah, same.
Carlo Parisi: Yeah. Let let's let's do this check. And then after you finish your check,
Carlo Parisi: we can we can ramp the the temperature.
Scott I. Reed: Yep.
Scott I. Reed: Yeah, Scott's doing that with a couple of fab
Scott I. Reed: guys right now.
Carlo Parisi: OK.
Scott I. Reed: It's not super easy to get under there so.
Carlo Parisi: Hmm.
Scott I. Reed: We don't know.
Scott I. Reed: OK. But they're a larger thermocouple and
Scott I. Reed: it's likely that, OK, so I'm assuming at all cities on the pcap
Scott I. Reed: were folder edge. Judging by those, OK.
Scott I. Reed: So we've probably been put the man's weights on me and then so those are suede,
Scott I. Reed: they're quarter inch.
Scott I. Reed: So it's quarter inch fitting there then?
Scott I. Reed: Yes, OK.
Scott I. Reed: Better sound suspense, OK?
Scott I. Reed: Yes, a lot better chance.
Scott I. Reed: OK.
Scott I. Reed: It's just odd that there's such a such a higher delta T on those.
Scott I. Reed: Like so, the ones that we were working with four,
Scott I. Reed: there's, you know, 1-2 degree difference between the upper
Scott I. Reed: one and the lower one.
Scott I. Reed: But on the other ones there's like 20° difference.
Scott I. Reed: Between the four, no.
Scott I. Reed: Between the the upper one and the lower.
Scott I. Reed: High. No different pipes.
Scott I. Reed: No different than cover for these. Like are you saying this like, oh, yeah,
Scott I. Reed: that's 43.
Scott I. Reed: Is that this is all the same pipe.
Scott I. Reed: It's just whether it's the ones that are at eye level or the ones that are at shin
Scott I. Reed: level.
Scott I. Reed: But if you look at this, it's on the that's it on the pipe as well.
Scott I. Reed: You're you're definitely dropping.
Scott I. Reed: One Pixel 243, that's what I said to Scott.
Scott I. Reed: Well, maybe she's been so long.
Scott I. Reed: We should have pictures.
Scott I. Reed: Yeah. Before it was insulated.
Scott I. Reed: But our flow is a lot lower.
Scott I. Reed: Well, it would be a lot though. Our flow is a lot lower.
Scott I. Reed: So and two in, yeah, in 1-2 and three or is it 4, Are you sure?
Scott I. Reed: Yes, you should be able to look.
Scott I. Reed: Yeah. If you go back to the main.
Scott I. Reed: Yeah. So we're.
Scott I. Reed: Five times more.
Scott I. Reed: Flow.
Scott I. Reed: So yeah.
Scott I. Reed: So that's probably.
Scott I. Reed: But the only way I would know to to say how we did it anymore is to look back at
Scott I. Reed: pictures.
Scott I. Reed: And we should definitely have pictures of all that agreed.
Scott I. Reed: Yeah, it's like being.
Scott I. Reed: Actually, we do see the gradient. Both of these agree that there's a
Scott I. Reed: gradient from there to here.
Scott I. Reed: Yeah, it.
Scott I. Reed: I mean that is definitely that would make sense.
Scott I. Reed: So if you look at one of the other ones, it doesn't have the same gradient, right?
Scott I. Reed: You're not losing.
Scott I. Reed: You don't have much flow in it.
Scott I. Reed: Practice in both sets.
Scott I. Reed: What this one?
Scott I. Reed: Right.
Scott I. Reed: Well, your question is how well is that
Scott I. Reed: attached to your pipe.
Scott I. Reed: Or is that the magnet?
Scott I. Reed: No, this is your magnet on here, your ambient.
Scott I. Reed: Can you tell that it's like?
Scott I. Reed: OK. That's on the pipe.
Scott I. Reed: Yeah, this is the one that's on the pipe that's
Scott I. Reed: under the air blow.
Scott I. Reed: Yep.
Scott I. Reed: No, that'll happen when translate.
Scott I. Reed: Well, both are wrong to say.
Scott I. Reed: You know how they're bad?
Scott I. Reed: Wrong. There's. Yeah. Again, if you pull the pictures up,
Scott I. Reed: you should be able to see all of them.
Scott I. Reed: Because I know before we insulate, we made sure we put all.
Scott I. Reed: Well, that that makes sense.
Scott I. Reed: I thought one of these might be the one.
Scott I. Reed: There's one of them. I actually looked at the thermocouple.
Scott I. Reed: It looked like it might have been damaged even a little bit because the back of it.
Scott I. Reed: Where the junction is.
Scott I. Reed: Just right over here. I remember looking and going.
Scott I. Reed: Thank you, Ben.
Scott I. Reed: It's not rain.
Scott I. Reed: But you have to flashlights. Look at it.
Scott I. Reed: Where the junction is where it winds out, right?
Scott I. Reed: And that's all potted.
Scott I. Reed: It looks like that piece of like a little bit of.
Scott I. Reed: Junction's been something.
Scott I. Reed: Doesn't look like the rest of them, but there's nothing like you can do with
Scott I. Reed: that at this point.
Scott I. Reed: Sort of taking these apart.
Scott I. Reed: So we're just looking to stabilize right now, right?
Scott I. Reed: What do we say? Stabilized was?
Justin Johnson: ±2.
Scott I. Reed: On the let me I gotta read through here. So let's see here.
Scott I. Reed: We said, well, these have definitely been ±2 for a while.
Scott I. Reed: Well, those ones ±2 most immediately. It was the ones that were.
Scott I. Reed: It was the ones that were in the.
Scott I. Reed: But the oh wait till ext 010019015018.
Scott I. Reed: No, the ones that are in the lab. Oh, that.
Scott I. Reed: Oh, right, Carlo.
Scott I. Reed: Please wait a minute.
Justin Johnson: Those ones right there.
Scott I. Reed: Yeah, I've got a floor.
Carlo Parisi: Yeah. Sorry, I was muted.
Carlo Parisi: Oh, can you repeat the question?
Scott I. Reed: You know what? Hold on.
Justin Johnson: Which temperature needs to be stabilized?
Scott I. Reed: Oh, we're just trying to make sure we got the
Scott I. Reed: right ones for making sure we're at equilibrium.
Scott I. Reed: 010 so maybe you're right.
Scott I. Reed: Well, but that we were planning on being one.
Scott I. Reed: Well, that's that's how we get written.
Scott I. Reed: These ones 404548 and 49, they haven't changed 2° since we started.
Justin Johnson: I think you just want ice.
Justin Johnson: It doesn't matter, right?
Justin Johnson: A set of thermal couples that stay the same should show you your steady state.
Justin Johnson: Is that the idea carne?
Scott I. Reed: Well, you you have to know which set you're
Scott I. Reed: using, because these Thermo couples here, they're on the heaters.
Scott I. Reed: They're they're steady. As soon as you hit 180.
Justin Johnson: Yeah.
Scott I. Reed: Whereas everything else is still changes, you got to decide which ones are your
Scott I. Reed: equilibrium.
Scott I. Reed: That's why I had said all. Well, the problem is all is a ton of Thermo
Justin Johnson: Look.
Scott I. Reed: couples to try to look at.
Justin Johnson: You want the coolant.
Justin Johnson: The coolant lines, Carlo or the pots of lead.
Scott I. Reed: I think it's the lead that's that's.
Carlo Parisi: The because yeah, that's what I was looking at #4 and try
Carlo Parisi: to see it seems quite stable right now, yeah.
Scott I. Reed: So we'll add that note.
Scott I. Reed: 'Cause, you're saying we want 4645?
Carlo Parisi: Yeah.
Scott I. Reed: Well 40414243.
Scott I. Reed: Oh yeah, there's six of them.
Carlo Parisi: Yeah.
Scott I. Reed: Sct.
Scott I. Reed: O 41.
Scott I. Reed: Through O 46.
Carlo Parisi: 41 yeah, 41 is one on the bottom.
Scott I. Reed: Say what?
Carlo Parisi: Yeah, it's the one on the bottom of the I it
Carlo Parisi: checks right.
Carlo Parisi: The 41.
Scott I. Reed: Well, there's SC41 and there's EC 41.
Carlo Parisi: 4.
Carlo Parisi: OK.
Scott I. Reed: You're talking about, are you?
Scott I. Reed: You're talking about these, right?
Carlo Parisi: Yeah.
Scott I. Reed: These are you, the ones you want to be steady.
Carlo Parisi: Yeah, I'm talking.
Carlo Parisi: The one in the ihx.
Carlo Parisi: Yeah. And the secondary coolant.
Scott I. Reed: Yeah, so it's the SDS, yes.
Carlo Parisi: Yeah, I see. Yeah.
Scott I. Reed: OK.
Scott I. Reed: So to check those we take a picture of them and then wait for 5 minutes.
Carlo Parisi: Yeah.
Scott I. Reed: Well, that should do that. Since you're doing this house.
Scott I. Reed: Star o'clock and watch.
Scott I. Reed: Yep, that's 138.
Scott I. Reed: We got somewhere. If you've messed around.
Carlo Parisi: Can I see also the water temperature in loop 4?
Carlo Parisi: Glycol temperature.
Carlo Parisi: Tell me a scroll.
Scott I. Reed: 24 to 30.
Carlo Parisi: 24 to no 30, but I'm looking the 27, the other one, the E CTE042 'cause.
Carlo Parisi: That's an average of all three.
Scott I. Reed: Oh.
Carlo Parisi: Yeah, and didn't change a lot.
Carlo Parisi: So that tells me that yeah, the delta T is constant so.
Carlo Parisi: Yeah, that's the other thing I would.
Carlo Parisi: I would check, but it's bit more difficult to see
Carlo Parisi: because yeah, there are all these.
Carlo Parisi: Other three loops that are averaging I mean 3 coils,
Carlo Parisi: 4 coils that are being averaged.
Carlo Parisi: But yeah, it was 30 also.
Carlo Parisi: Probably 20 minutes ago that loop so.
Carlo Parisi: Since we reached a kind of steady state, the element, see also the. Yeah,
Scott I. Reed: Yeah. These all look very.
Carlo Parisi: these are all steady. Yeah.
Scott I. Reed: About 3 1/2 kilowatts.
Carlo Parisi: All steady.
Carlo Parisi: Three and half kilowatt, OK, yeah.
Carlo Parisi: Yeah, I'm satisfied. If you guys want to raise the raise the
Carlo Parisi: temperature, yeah.
Carlo Parisi: We can.
Carlo Parisi: We can move to the next step.
Scott I. Reed: Said, didn't we say he wanted to wait 5 minutes?
Carlo Parisi: Oh, OK.
Carlo Parisi: Yeah, let yeah.
Carlo Parisi: Let. Yeah, let's wait.
Carlo Parisi: Let's wait this 5 minutes, right?
Carlo Parisi: I don't think it's gonna change, but yeah.
Carlo Parisi: Let's let's wait and just.
Scott I. Reed: I mean certainly not changing much, but.
Carlo Parisi: Yeah, yeah, yeah. No. Let's wait. Right.
Scott I. Reed: We'll give it a couple more minutes.
Carlo Parisi: Then and then after that.
Carlo Parisi: So after that, Josh, we are gonna increase temperature of step
Scott I. Reed: Fish Russell.
Carlo Parisi: of 2450 CI don't.
Carlo Parisi: I don't remember.
Scott I. Reed: Well, that's when we we said we were gonna try
Scott I. Reed: to go to 450.
Scott I. Reed: Yeah, that's what we said.
Carlo Parisi: Oh, one step.
Scott I. Reed: It's 450 mean.
Carlo Parisi: OK.
Scott I. Reed: That's what we had.
Scott I. Reed: That's what we identified this morning.
Carlo Parisi: No, no, no, right.
Scott I. Reed: I mean, we can.
Carlo Parisi: I I was.
Carlo Parisi: I mean, I don't why I'm with this mindset of that.
Scott I. Reed: We can try some interstitial temperature.
Carlo Parisi: Yeah.
Scott I. Reed: Say what, Carlo?
Carlo Parisi: No, sorry. I was I.
Carlo Parisi: I got confused.
Carlo Parisi: I was thinking that we were raising the temperature a step stepwise,
Carlo Parisi: but we are just turning. I mean setting 450 and just ramp up
Carlo Parisi: temperature and see what we get OK.
Scott I. Reed: How high we can get?
Scott I. Reed: Yeah. Before we, I hear rejection overcomes us.
Carlo Parisi: Yeah, yeah, yeah, yeah.
Carlo Parisi: It makes sense.
Carlo Parisi: Yeah, makes sense.
Carlo Parisi: We yeah.
Carlo Parisi: We can.
Carlo Parisi: We can see what we got from those coils.
Scott I. Reed: Another one.
Scott I. Reed: And then we're gonna stop.
Scott I. Reed: At that point, that was kind of where we were going to
Carlo Parisi: Hmm.
Scott I. Reed: regroup and see what we were doing.
Carlo Parisi: Yeah.
Scott I. Reed: So if same thing happens that happened in the fall, which should?
Carlo Parisi: Mm hmm.
Scott I. Reed: The the Max temperature we should be able to get to before.
Scott I. Reed: Things start to get on the precipice of boiling for coolant is.
Scott I. Reed: 3 twentyish.
Carlo Parisi: OK.
Scott I. Reed: So we could set that as a target or we could go straight to 4:50.
Carlo Parisi: Which which is set, yeah.
Carlo Parisi: Yeah. Which limit did you set for boiling on
Carlo Parisi: the tertiary side?
Carlo Parisi: Josh.
Scott I. Reed: I'm sorry, I didn't hear.
Scott I. Reed: What? What was that, Carlo?
Carlo Parisi: I was asking which temperature limit use you set on the tertiary side for.
Carlo Parisi: Tacting boiling, I mean.
Carlo Parisi: I remember this fall.
Carlo Parisi: It was very conservative.
Scott I. Reed: Well, you identified that 150 is the actual
Scott I. Reed: boiling point hundred 15115.
Carlo Parisi: One of 15 OK.
Scott I. Reed: Because he did that a couple days ago in a fume hood.
Carlo Parisi: Ah, OK.
Carlo Parisi: So can we reach 110 or so? What's the limit?
Scott I. Reed: Yeah, it should have done that.
Scott I. Reed: 110 was what?
Scott I. Reed: We were saying we're going to be worried about once you get 110,
Scott I. Reed: that's when we're starting to act.
Carlo Parisi: Hmm.
Carlo Parisi: OK.
Scott I. Reed: Protect the system, right?
Scott I. Reed: That's what we wrote down.
Carlo Parisi: OK.
Carlo Parisi: SO1OK. So we push to 110, OK.
Scott I. Reed: And we're going to get a pop up that was at 97.
Scott I. Reed: Well, we'll see that on the.
Carlo Parisi: Yeah, yeah, because this I think this fall you Josh
Scott I. Reed: Outlet of the.
Carlo Parisi: used 97, right?
Carlo Parisi: I remember it was a number under 100.
Scott I. Reed: When we were when, when you guys were out here in the fall?
Scott I. Reed: Yes.
Scott I. Reed: We were being we were trying to be extra conservative because we didn't have the
Carlo Parisi: Hmm.
Scott I. Reed: PSV at that point.
Carlo Parisi: OK.
Carlo Parisi: So so likely today we should get higher temperature because you stop the task at
Carlo Parisi: 97.
Carlo Parisi: So if today we can go to 110, yeah, we should get higher temperature, OK.
Scott I. Reed: Yeah, I I don't think it's going to be hundreds
Scott I. Reed: of degrees higher, but a little bit.
Carlo Parisi: Yeah. No, no, right.
Carlo Parisi: Yeah, a little bit, yeah.
Scott I. Reed: So it's been 5 minutes. So we checked all six of those Thermo
Scott I. Reed: couples.
Carlo Parisi: Mm hmm.
Carlo Parisi: Seems stable.
Scott I. Reed: Certainly agree on the first point.
Scott I. Reed: Those are all ±2.
Scott I. Reed: Yeah, I think you're there.
Carlo Parisi: OK.
Scott I. Reed: Let's document when you start the next tramp.
Carlo Parisi: So let's go.
Scott I. Reed: So what are we doing now?
Carlo Parisi: Yeah.
Scott I. Reed: We're going to 100 and what does it say?
Carlo Parisi: 4:50.
Scott I. Reed: Boy, 450 was the next goal, so we did get to 180.
Carlo Parisi: Yep.
Scott I. Reed: So I'm gonna record that from 14. 7 gonna say.
Scott I. Reed: 138.
Scott I. Reed: So are we going to 4:50?
Carlo Parisi: Mm hmm.
Scott I. Reed: Correct.
Carlo Parisi: Yeah.
Scott I. Reed: OK.
Justin Johnson: Going where we've never gone before.
Scott I. Reed: Here she goes.
Scott I. Reed: That's a split infinitive.
Scott I. Reed: We'll have to make sure the challenger doesn't blow up.
Justin Johnson: That's right.
Scott I. Reed: Maybe you could have picked a different.
Scott I. Reed: Maybe not the challenger, maybe.
Scott I. Reed: No, I mean, let's pick one of the space shuttles that
Carlo Parisi: Hmm.
Justin Johnson: I was thinking the enterprise.
Scott I. Reed: didn't blow up as Ari.
Carlo Parisi: Yeah, it's oddly.
Justin Johnson: What's the what's the Star Trek quote?
Scott I. Reed: Yeah, the challenger did.
Scott I. Reed: That was 80.
Scott I. Reed: That's what I said, right?
Scott I. Reed: Let's let's pick one that didn't blow up.
Justin Johnson: No, we don't want that one.
Justin Johnson: Pick Discovery or Atlantis.
Carlo Parisi: Yeah. Yeah, exactly.
Scott I. Reed: Oh, that's why, he said.
Scott I. Reed: Let's hope it doesn't blow up.
Justin Johnson: Yeah. No, I was thinking Star Trek like, boldly go where?
Justin Johnson: I can't remember the tagline.
Scott I. Reed: I was thinking Toy Story.
Justin Johnson: Yeah, I like it.
Scott I. Reed: Well, that's the.
Scott I. Reed: Star Trek is the enterprise.
Scott I. Reed: Not the Toy Story.
Justin Johnson: What's the tagline?
Scott I. Reed: What's the guy in Toy Story that has the spaceman?
Justin Johnson: Buzz lightyear.
Scott I. Reed: That's the lightyear.
Scott I. Reed: Yeah, to Infinity and beyond.
Justin Johnson: Yeah, that's right.
Scott I. Reed: He didn't write in the challenger. I know, but the challenger blew up, yes.
Justin Johnson: No, this is the line to boldly go where no
Scott I. Reed: That's what I'm saying. We, we.
Justin Johnson: one has gone before. Star Trek tagline used in 1966.
Scott I. Reed: Right and I right.
Scott I. Reed: And I said that's a split infinitive.
Justin Johnson: OK.
Scott I. Reed: To boldly go.
Scott I. Reed: It should be to go boldly.
Justin Johnson: Oh, you're talking to the wrong dude, man. I'm a grammar.
Scott I. Reed: Illiterate.
Justin Johnson: Vandal. Yeah, I actually got that on my one of my
Justin Johnson: performance review feedbacks go to get work on grammar.
Justin Johnson: It's very poor 'cause it hikes.
Scott I. Reed: Nice. You must be an engineer.
Justin Johnson: That's right.
Justin Johnson: I wasn't like, that's why I told him. I said you didn't hire me to write
Justin Johnson: grammar.
Justin Johnson: That's why we have tech editors.
Scott I. Reed: That's right.
Scott I. Reed: Anyway, so we are slowly going up and we are
Scott I. Reed: watching for anything over 110.
Scott I. Reed: Or a pressure over 14 / 14 pitching it.
Scott I. Reed: We were at about 10.
Scott I. Reed: Psi.
Scott I. Reed: About where we were.
Scott I. Reed: Playing. He's got a lot of bigger.
Justin Johnson: Dude, it does respond pretty fast, doesn't it, Carlo?
Carlo Parisi: Mm hmm. Yeah, that's the beauty of these systems.
Justin Johnson: It's pretty cool.
Scott I. Reed: Yeah, those those lines were never wet, so.
Carlo Parisi: Yeah, all.
Carlo Parisi: All atmospheric pressure so.
Justin Johnson: Mm hmm.
Scott I. Reed: That's what you did.
Carlo Parisi: Earlier.
Scott I. Reed: Well, that's what they told me.
Carlo Parisi: OK, can can we can we see the loop #4 the
Scott I. Reed: But the good news is the ramp race for mm hmm.
Carlo Parisi: glycol loop so.
Carlo Parisi: I'm curious to see how the yeah, the.
Scott I. Reed: Like a loop #4.
Scott I. Reed: What was the last?
Carlo Parisi: Yeah, yeah. How they start to change.
Carlo Parisi: Yeah, the one with glycol, not, not not this one.
Scott I. Reed: Not really, no.
Scott I. Reed: This temperature is right about where it was previously.
Carlo Parisi: Yeah.
Carlo Parisi: OK.
Carlo Parisi: So we'll take some time probably.
Carlo Parisi: OK here.
Scott I. Reed: The exchangers temp is still all about the same.
Carlo Parisi: Yeah. Yeah, let's take some time.
Scott I. Reed: I mean, we've only gone up to 190.
Carlo Parisi: Hmm.
Scott I. Reed: So.
Carlo Parisi: Yeah, probably.
Carlo Parisi: I don't know. Maybe in other 3030 C.
Scott I. Reed: What? Oh, oh oh.
Scott I. Reed: Yeah, we probably don't really care about 200 X.
Carlo Parisi: 30C to change.
Carlo Parisi: 250.
Scott I. Reed: He said.
Scott I. Reed: We don't care about 45 either.
Scott I. Reed: No.
Carlo Parisi: Let's see.
Carlo Parisi: 16 kilowatt so.
Carlo Parisi: OK.
Scott I. Reed: Yeah, just a little bit.
Scott I. Reed: Oh yeah.
Scott I. Reed: At least for now, I usually set that at 33000.
Scott I. Reed: Hour. Yeah, but it's also.
Scott I. Reed: This is kind of like watching paint dry.
Scott I. Reed: Or is it more exciting?
Justin Johnson: Have never watched an $11 million paint job dry,
Justin Johnson: so I think it's a little more exciting.
Scott I. Reed: This is more exciting, OK?
Carlo Parisi: Yeah.
Justin Johnson: Yeah.
Scott I. Reed: 11,000,000 thought it was more than that.
Carlo Parisi: Yeah, there is no, no, no card that costs so much probably.
Justin Johnson: No, this is.
Justin Johnson: I think we're.
Justin Johnson: I mean we're.
Justin Johnson: I think we're between 11 and 12 million right now total on pcat.
Scott I. Reed: Just just for the pcat.
Justin Johnson: Yeah, just pcat.
Scott I. Reed: Oh, OK.
Justin Johnson: No, this has been a fairly expensive test.
Scott I. Reed: Yeah, so far we've shown that heaters work and
Justin Johnson: Yes.
Scott I. Reed: that hot things go in a circle.
Scott I. Reed: Roughly 12 million Don.
Justin Johnson: Yeah, I think so.
Carlo Parisi: Well, I don't know what what was the cost of
Scott I. Reed: Don't let Elon know.
Carlo Parisi: destroying a nuclear reactor with the sterling?
Justin Johnson: Yeah. If we would have blown that, if we would have done what we did with
Justin Johnson: the sterlings once they were on Marvel, we would have talked in the order of like
Carlo Parisi: Yeah.
Justin Johnson: $200 million plus cleanup.
Carlo Parisi: Yeah.
Justin Johnson: So I think we're saving a lot of money.
Carlo Parisi: Yeah.
Scott I. Reed: We would have been another history lesson.
Justin Johnson: Yeah, we would have a documentary about the
Carlo Parisi: Mm hmm.
Carlo Parisi: Yeah.
Justin Johnson: love triangle that ruined Marvel.
Carlo Parisi: Yeah, yeah.
Justin Johnson: Stacy MW and Mark.
Justin Johnson: They're not really in a love triangle.
Scott I. Reed: Well, blame it all on Yasser.
Scott I. Reed: He left.
Justin Johnson: All I do every day.
Scott I. Reed: I'm sorry, sorry I didn't catch what you do every
Scott I. Reed: day.
Justin Johnson: Blame it on Yasser.
Justin Johnson: Although the one of the other P Miss Mark from MFC is leaving here in like a month
Justin Johnson: so.
Scott I. Reed: Mark nefter.
Justin Johnson: We'll get, yeah. Yeah. Hopefully that was public knowledge.
Carlo Parisi: Yeah.
Justin Johnson: He announced that the LD meeting on Friday.
Justin Johnson: So I figured it's public now.
Carlo Parisi: Oh, OK.
Scott I. Reed: So who's 'cause? I mean, they just announced him as the new guy.
Justin Johnson: Yep, yeah, I think he maybe should have said that
Justin Johnson: before they announced that.
Justin Johnson: I don't know.
Justin Johnson: Rescanon is gonna start stepping in for MFC.
Scott I. Reed: Who?
Justin Johnson: Ree scanning. He was working on sample prep web.
Scott I. Reed: Don't know who.
Justin Johnson: I think I've heard his name, but I've never worked with him.
Justin Johnson: So that makes him the.
Justin Johnson: Hold on a second.
Justin Johnson: He'll be the 7th project manager on Marvel.
Scott I. Reed: Well, that's how we make sure we we can blame
Scott I. Reed: nobody.
Scott I. Reed: We've had too many people.
Justin Johnson: Well, the bad thing is now I have the most.
Justin Johnson: I have the most seniority. I've been on the longest.
Scott I. Reed: I've been on it longer than you have, Justin.
Justin Johnson: I'm sure.
Justin Johnson: Yeah, that's true.
Justin Johnson: I mean, I'm not saying Carlos been on it since
Justin Johnson: the day one. I'm saying as a project manager.
Scott I. Reed: Oh, OK.
Justin Johnson: The actual the actual working people have stayed the same.
Justin Johnson: They're just getting poked by different pokers.
Scott I. Reed: Gotcha.
Carlo Parisi: Yeah, we we sync with the ship, Justin.
Justin Johnson: That's right.
Justin Johnson: Yeah, you guys are the the the rats that can't
Justin Johnson: get off the ship.
Justin Johnson: We're the we're the captains. That definitely jump off 1st.
Carlo Parisi: Hmm.
Scott I. Reed: I thought the captains were supposed to stay on till after say.
Carlo Parisi: Exactly, exactly should be the last one.
Justin Johnson: Yeah. Well, I maybe you're the Captain Carlo.
Justin Johnson: You and Scott are the captain.
Justin Johnson: Maybe I'm the bill. Drat.
Carlo Parisi: Yeah.
Scott I. Reed: I think I think CEI is the build threats.
Scott I. Reed: I think you're Mr. Smee, Justin.
Justin Johnson: Premier was the builder at CES.
Justin Johnson: You're you guys aren't the build rats.
Scott I. Reed: OK.
Justin Johnson: Just while.
Scott I. Reed: I tell you what, if I'm the captain, I had no idea I had so much authority.
Justin Johnson: Well, that's the secret about Marvel.
Scott I. Reed: Or wish I had known that a long time ago.
Justin Johnson: Nobody knows.
Justin Johnson: Nobody has actual authority.
Scott I. Reed: Patrick would have run a little better if he did that.
Justin Johnson: That's they asked me. What do I think the number one thing that
Justin Johnson: we could do to improve Marvel?
Justin Johnson: And I said I would just like to know who the decision maker is because no one
Justin Johnson: makes decisions.
Justin Johnson: So no one could answer me that question yet.
Carlo Parisi: Exactly, yeah.
Justin Johnson: But it's because they asked me during the the meeting Ron did.
Justin Johnson: He's like, so if you hadn't decide today, what would you do?
Justin Johnson: And I was like, pumped Knack.
Justin Johnson: No, he or no thermal energy storage and super
Justin Johnson: super.
Justin Johnson: Critical CO2 and he's like that's why you're not making decisions so.
Justin Johnson: I didn't like my answer and I just told him I'm not promise it'll be right,
Justin Johnson: but we'll try something.
Justin Johnson: We'll move ahead.
Scott I. Reed: About 10 psi.
Justin Johnson: Why are you reading that from?
Carlo Parisi: Yeah.
Scott I. Reed: That's the that's a local gauge.
Justin Johnson: Oh, OK.
Carlo Parisi: Oh, OK.
Carlo Parisi: So we don't have here, yeah.
Justin Johnson: What are these showing us?
Justin Johnson: Oh, are these are in Celsius, OK.
Scott I. Reed: It it's it's basically right about here.
Scott I. Reed: Just after the pump.
Justin Johnson: Oh, I see. OK.
Scott I. Reed: So. So yeah, they're there. Definitely is the pump contribution to
Scott I. Reed: that.
Scott I. Reed: So maybe 14 is a little bit.
Scott I. Reed: A little bit conservative, but.
Carlo Parisi: Oh, is that the EC?
Carlo Parisi: FI 042 Josh.
Scott I. Reed: I'm sorry, could you repeat that?
Carlo Parisi: It's the number that I see there, yeah.
Carlo Parisi: EE CFI 042.
Carlo Parisi: That's in psi, right?
Scott I. Reed: No, that's the that's liters per minute. That's the flow speed.
Carlo Parisi: Oh, OK.
Carlo Parisi: So we don't have a pressure reading here.
Scott I. Reed: No, you can't see it.
Scott I. Reed: It's just a gauge, a manual.
Carlo Parisi: Ah, oh, OK, OK.
Scott I. Reed: Yep.
Scott I. Reed: I'm gonna run to the rescue.
Carlo Parisi: So right now we are 27.
Carlo Parisi: It's still the same delta T against. It's interesting.
Justin Johnson: And we're about 12 minutes in, so we haven't seen,
Justin Johnson: we haven't seen any increase on the Delta T after 12 minutes.
Carlo Parisi: What's going on with mass flow of the four loops?
Scott I. Reed: Sh.
Carlo Parisi: No going up, hmm.
Justin Johnson: They're ramping.
Scott I. Reed: Yeah.
Carlo Parisi: OK.
Carlo Parisi: It takes forever.
Justin Johnson: So what do we have expected?
Justin Johnson: Hmm.
Justin Johnson: I guess let's be patient and give it some time.
Scott I. Reed: 'Cause, your lads gonna take time to respond,
Scott I. Reed: alright?
Scott I. Reed: You're increasing the heat, the leads in the lag.
Justin Johnson: The interesting thing is the blue one's not really like look at the ramps on the
Justin Johnson: four that aren't being cooled.
Scott I. Reed: Because they don't have anything cool in them.
Justin Johnson: Yep. So they're ramping the mass flow up
Justin Johnson: pretty quickly.
Justin Johnson: And then I think looks like Blue's gonna take a while,
Justin Johnson: like it'll probably get past here pretty quick potentially.
Scott I. Reed: Yeah, it's probably gonna do just like it did
Scott I. Reed: on the last run, where it gets flipped down to the bottom
Scott I. Reed: and then at the end it comes back.
Justin Johnson: Good morning.
Carlo Parisi: Can I see down camera #4?
Carlo Parisi: K.
Scott I. Reed: Were you listing Justin when we explained what happened with the Thermo couples
Scott I. Reed: that weren't making sense on the down comers?
Justin Johnson: Yeah, the potting came loose.
Justin Johnson: Was that what the you could see? Something was different, but not.
Scott I. Reed: Well.
Justin Johnson: I didn't hear. What, really.
Scott I. Reed: The.
Scott I. Reed: They were loose because.
Scott I. Reed: There's the swages.
Scott I. Reed: These are the thermocouples, the wrong size or the fittings are the
Scott I. Reed: wrong size.
Scott I. Reed: But you couldn't swage them in to make a mistake.
Justin Johnson: OK.
Scott I. Reed: But they were loose.
Scott I. Reed: So what all we've been able to do because we need to have to get bigger Thermo
Scott I. Reed: couples.
Scott I. Reed: Or take the pecat apart. Well, new.
Scott I. Reed: Thermo Wells and we just we just taped them, taped them in there so.
Justin Johnson: Maintaining zone? Yep.
Justin Johnson: OK.
Justin Johnson: Sounds good.
Scott I. Reed: Now I am curious with regards to the quality assurance side of this.
Scott I. Reed: I probably need to talk to.
Scott I. Reed: I don't know whether Mike Fish or just Jen or whoever, but.
Scott I. Reed: We're kind of in a sticky spot that way from saying that,
Scott I. Reed: we're falling a test plan.
Scott I. Reed: 'Cause we aren't we no longer having a the approved test plan that I would have
Scott I. Reed: written down. My CGI is not what we're following.
Justin Johnson: OK.
Scott I. Reed: So we'll have to have that discussion, I guess maybe part of the question here
Justin Johnson: Yep.
Scott I. Reed: is there were a couple of things that I had originally intended to make sure we
Scott I. Reed: did before we before I left what was to make sure that all the the pumps worked,
Scott I. Reed: which I.
Scott I. Reed: Pretty sure they're going to work.
Scott I. Reed: Before I signed off on the EQT as being complete.
Scott I. Reed: And then the CGI portion of it.
Justin Johnson: OK.
Scott I. Reed: Which was main mainly the witnessing of this one test.
Scott I. Reed: To say that, yeah, they can, they can follow a test procedure.
Justin Johnson: Yep.
Scott I. Reed: And the struggle we've had obviously with the test procedures either we haven't
Scott I. Reed: written it in a way that we can follow it well,
Scott I. Reed: which is I guess is really the answer, right.
Scott I. Reed: We we haven't provided something that we could follow and actually do it all the
Scott I. Reed: way through, so.
Justin Johnson: Execute.
Scott I. Reed: I don't know how we want to do that.
Justin Johnson: Good.
Scott I. Reed: We probably ought to have that discussion sooner than later 'cause if I need to
Scott I. Reed: extend, extend time out, I'd prefer to do it.
Scott I. Reed: Sooner than.
Scott I. Reed: At the last minute.
Justin Johnson: OK.
Justin Johnson: I mean The thing is if we can.
Justin Johnson: So I'll just reiterating, make sure I heard the parts that.
Justin Johnson: Are were sort of witnessing the test right now.
Justin Johnson: We saw the three from Saturday.
Justin Johnson: We're witnessing one now, but we're having to redline the test
Justin Johnson: procedure.
Justin Johnson: So we need to figure out kind of the process of that because.
Justin Johnson: My assumption is we are going to be redlining the test procedure for every
Justin Johnson: test.
Justin Johnson: At some extent.
Scott I. Reed: I suspect you're right.
Justin Johnson: So there we I think that that has to be able to be done and we'll have to make
Justin Johnson: sure we document that and allows that 'cause I what?
Justin Johnson: I don't wanna end up doing if we can help it is.
Justin Johnson: Sending a vendor data Seminole through every day.
Justin Johnson: You know what I mean?
Scott I. Reed: No, I understand.
Justin Johnson: I think we'll. So let's talk about that and then the
Scott I. Reed: Patty.
Justin Johnson: pump witness.
Justin Johnson: 'Cause that's part of the CGI that you probably won't be able to complete for at
Justin Johnson: least.
Justin Johnson: Three more days. Four more days.
Scott I. Reed: Four days.
Scott I. Reed: And really I mean.
Scott I. Reed: I'm I'm comfortable signing off on that based on seeing the data.
Justin Johnson: Right.
Scott I. Reed: And it says they're flowing.
Justin Johnson: Yep.
Scott I. Reed: And since the fact is we're not going to sign off on the EQT.
Scott I. Reed: Until that state, anyway.
Scott I. Reed: I mean, there are there are things in there that
Scott I. Reed: we are like, well, we can't really do this.
Scott I. Reed: Until we're done right, I guess that is the thing that we're
Justin Johnson: So. So let me talk to Raymond and I'll set us
Scott I. Reed: waiting on.
Justin Johnson: up a meeting. But to me this sounds like we.
Justin Johnson: I don't want to use the term NCR because I have such negative connotations,
Justin Johnson: but we almost just NCR it and say we've had a change the approach,
Justin Johnson: but let me find out who the people are that need to be in there.
Justin Johnson: I know to start with Jen and Raymond and I'll try to set up a quick call.
Scott I. Reed: Right.
Justin Johnson: Today.
Justin Johnson: Play.
Scott I. Reed: OK.
Justin Johnson: And see if we can just iron that out.
Scott I. Reed: Alright.
Justin Johnson: Well, here, let me just see if.
Scott I. Reed: Yeah. And I I think that the part that for me
Scott I. Reed: that is tricky is I know if we were, if we were doing this at the site.
Scott I. Reed: And a nuclear facility.
Scott I. Reed: That's approach you always have to red. You have to redline it.
Scott I. Reed: You have to go through DCR right?
Scott I. Reed: You can have no more than five red lines before you actually have to revise it,
Justin Johnson: Yeah.
Scott I. Reed: and I think that we had hit that like right away.
Justin Johnson: Yep.
Scott I. Reed: And so I'm not sure.
Scott I. Reed: How that works when we're doing commercial grade dedication,
Scott I. Reed: it's I worry that it might throw us into the same boat.
Justin Johnson: OK.
Scott I. Reed: But obviously that's a struggle because I I agree with you that the direction we're
Scott I. Reed: heading, we're probably gonna be redlining stuff
Scott I. Reed: on a regular basis.
Justin Johnson: Yep. All right. Let me find out with some background
Scott I. Reed: Yes, I think we should have that meeting.
Justin Johnson: finding out.
Scott I. Reed: OK.
Scott I. Reed: We're at about 10 1/2 psi on the loop.
Scott I. Reed: Temperatures have started to go up a little bit as you can see.
Scott I. Reed: Our Delta T is is up to 6 1/2.
Scott I. Reed: We.
Scott I. Reed: Are.
Scott I. Reed: Heaters are about 280.
Carlo Parisi: And yeah, we are dumping 44 kilowatt there.
Scott I. Reed: Our return temp is starting to go up, as is our feed temp,
Scott I. Reed: so temperatures are going up across the board.
Scott I. Reed: We I mean that's what we would expect, but keeping everybody making sure
Carlo Parisi: Yeah.
Scott I. Reed: everybody's in the loop.
Carlo Parisi: Yep.
Scott I. Reed: And run it.
Scott I. Reed: You're still.
Scott I. Reed: Josh yes.
Scott I. Reed: Little bit, what's up?
Scott I. Reed: Would you like to look at some numbers I just calculated for next?
Scott I. Reed: Yeah, sure. So
Scott I. Reed: on the lot.
Scott I. Reed: It's it's OK.
Justin Johnson: Yeah. Don't talk trash.
Scott I. Reed: That's Justin.
Scott I. Reed: I'm sorry. No, you're fine.
Scott I. Reed: If we want it like I'm going to summarize it for you, you know what I mean.
Scott I. Reed: People like to get a distance number on the.
Justin Johnson: Now we're finally seeing the temperature rise on one of them.
Justin Johnson: I muted you guys.
Justin Johnson: Josh, just in case you didn't notice.
Scott I. Reed: Oh, you needed us.
Justin Johnson: Yeah, sorry I didn't want you guys to have to
Justin Johnson: be careful when you wanted the talks.
Justin Johnson: Talk smack on me.
Scott I. Reed: No, we we were working on. Diana was just asking a question about
Scott I. Reed: Marvel, so.
Justin Johnson: Oh, I owe you back. A drawing still for the down Comer.
Justin Johnson: I am working on that.
Scott I. Reed: Yes, yes, she did say that.
Scott I. Reed: That would help.
Scott I. Reed: Oh, the marble, yeah.
Scott I. Reed: So our our attempts are starting to come up.
Scott I. Reed: For about 10 1/2 lbs just to watch it for 110 is our Max at the we still got a
Scott I. Reed: little ways to go certainly, but.
Scott I. Reed: We're at.
Scott I. Reed: 312 wow, we're getting up there. Maybe so.
Scott I. Reed: That lag in the leg.
Scott I. Reed: Yes, maybe.
Scott I. Reed: Maybe I was misremembering.
Scott I. Reed: Well, you may be looking at the legend, but you're not the legend.
Scott I. Reed: That's true.
Scott I. Reed: I don't remember which temperature I was looking at. What is arletta?
Scott I. Reed: They were so happy there were no, I'm pretty.
Scott I. Reed: I was looking at these temps 'cause I was.
Scott I. Reed: I was looking at the the local reader guys.
Scott I. Reed: I think there's both.
Scott I. Reed: Are those plugged in?
Scott I. Reed: We have signals going to vote.
Scott I. Reed: Oh, you have the clamp.
Scott I. Reed: You still have clamp Thermo couples up there.
Scott I. Reed: What it's possible?
Scott I. Reed: America.
Scott I. Reed: I checked your log, I didn't see.
Scott I. Reed: Yeah.
Scott I. Reed: Those who have a shot.
Scott I. Reed: OK.
Scott I. Reed: It's all right.
Scott I. Reed: Yeah.
Scott I. Reed: Of course I could stop Ariel.
Scott I. Reed: She wanted to save it as well, but that's what we're seeing right now.
Scott I. Reed: So you ought to be very close 'cause. I mean,
Scott I. Reed: there's clams and like one above the other.
Justin Johnson: OK, Josh, I put the down Comer drawing in the pcap
Justin Johnson: marble heat extraction folder.
Scott I. Reed: OK.
Scott I. Reed: Thank you.
Justin Johnson: I think it's just not peak at sorry. Marvel heat extraction, raft drawings.
Scott I. Reed: Oh, OK.
Scott I. Reed: I will.
Scott I. Reed: I will get them to Diana in just a couple minutes.
Justin Johnson: OK.
Scott I. Reed: 688.
Justin Johnson: Hey, Scott.
Scott I. Reed: Yeah.
Justin Johnson: You wanna just call Jen into this right now and have this discussion?
Scott I. Reed: Yeah, we can.
Scott I. Reed: I I mean it sounds like from what you're saying there, it sounds like.
Justin Johnson: Recovered right.
Scott I. Reed: What I don't know is I don't actually says anywhere that we can redline it.
Justin Johnson: OK.
Justin Johnson: Me. Look in the test.
Scott I. Reed: You would.
Scott I. Reed: You would know better than I would because I haven't.
Scott I. Reed: You know, up until we started, I hadn't really seen it.
Scott I. Reed: I just started reading it.
Justin Johnson: Yeah. Let me look really quick.
Scott I. Reed: I would think it'd be at the very beginning of it.
Justin Johnson: Yep, we've got to find the e-mail that Josh
Justin Johnson: sent this morning.
Scott I. Reed: Now I know there's a piece that says things can be done out of order.
Scott I. Reed: Somewhere.
Justin Johnson: Yep.
Justin Johnson: OK.
Justin Johnson: I thought we now, she says that I thought we had included
Justin Johnson: something like that.
Scott I. Reed: At 6. 9 says that while it is recommended the
Scott I. Reed: test be completed in the order presented in this document,
Scott I. Reed: not sequentially by test number, the PMA authorized a deviation from that
Scott I. Reed: order of circumstances arise.
Justin Johnson: Oh, it says the test included could be
Scott I. Reed: But I don't see.
Justin Johnson: altered. 7. 3 says they can be altered with receipt
Justin Johnson: of ACR or approval by the project manager.
Scott I. Reed: OK.
Justin Johnson: So I think that probably covers us.
Scott I. Reed: So we're we're following it. So as long as we do a good job
Scott I. Reed: documenting our stuff.
Scott I. Reed: Sounds like we're OK and that's what if I'm reading. That's what Jen is saying.
Justin Johnson: Yep.
Justin Johnson: So I think what we'll do is we'll just.
Justin Johnson: OK, perfect.
Justin Johnson: So I think we're set. So what?
Justin Johnson: What my recommendation is, and I hate to say this 'cause,
Justin Johnson: it means I gotta get out of bed really early every day.
Justin Johnson: 'cause maybe we have a quick plan of the day meeting at the beginning of the day.
Justin Johnson: It doesn't have to be at six, but we go.
Justin Johnson: Over the tests know if there's any red lines for the test for that day.
Justin Johnson: But anytime we get to a spot that's messed up.
Justin Johnson: Or we can't proceed. We'll hold a meeting.
Justin Johnson: Will document the time Josh and the you know the attendants and oh,
Scott I. Reed: Josh, Josh isn't here.
Justin Johnson: so Scott will tell Josh this, but we'll document the time and
Justin Johnson: attendance and provide concurrence as a team.
Scott I. Reed: Yeah, I think we should just continue to
Scott I. Reed: redline the document like we did this morning. Now that we're done,
Justin Johnson: Yep, I agree.
Scott I. Reed: we actually have a a real copy.
Justin Johnson: Yep, I agree.
Justin Johnson: So we'll just set up teams meeting and.
Justin Johnson: We'll just provide concurrence in the teams meeting.
Justin Johnson: We can even do it in the chat that we all accept the red lines for the day and then
Justin Johnson: if we need to change, we'll change later and just continue that
Justin Johnson: same methodology.