dot lines are flow of EM radiation aka light an IR
the curve in bottom is moon surface
each dot on the surface which is between object and horison for the object will illuminate the object with reflected light and IR of its temperature
stick is radiator
reversed hat on the stick is your mirror
black triangles are a percentage of radiation which is emitted from dot on the surface
it does not look like a lot so probably needs take integral to know the real value
but I'm ok just assuming it will be some
dot lines from the hut is the shadow created by the hut mirror
dots in the shadow do not emit or emit less fo the scattered EM
so basically you need trace light in the scene
it is not that big of a problem those scattered light - you can just ignore it, to some extent, because there are simple solutions to solve it. aluminum foil and let it reflect in a slightly different direction.
it seems i followed what your diagram meant, but don't get the message. the reflector under the final rad prevents most of the light from the ground from touching that rad. A fringe on the edges of the reflector would remove all of that light.
do you recall that this radiator turns over the course of the day? it is always edge-on to the sun, the sun's rays fall parallel to it and don't touch it, all day.
since that final rad is there to get the heat carrier down to 300 K, that seems important
the radiator is the whole thing, but the heat carrier is sent up from one rad to the next, each of which cools the fluid more. The final one is the one that is lowering the fluid to below the surface temperature of the moon, so in its case i thought the protection from that heat might be significant
the heat field may be an interesting solution. if it can ever be mapped out for me in a way that allows me to see how it all works
you looking at the angle of a tangent line to parabola scaled 10 (arct/10), normals to the parabola in respective points, parabola itself with the focal point of (0,10)
I was interested in reflection of light from radiator where it goes after reflection from parabola
wonderful thing is that parabola so beautiful - seem it cooperated with what should be done
I have no problem to imagine the model, I'm not sure about reflection angles in the model and which shapes those reflections are forming according to radiator emitting surface
math is real. there is no question about that, it's everywhere. so the quote is good in that regard. no one hides that but it is related to properties of knowledge - it can't be stolen and it can't be given, it can be only taken and no one can take more than he deserves.
yeah, but the quote was referring to there being a dimension or connected universe or something where math literally exists. that is, that the formulas that describe reality are themselves actually real somewhere.
it was the opening of a book by a mathematician that was about the nature of reality. but i can't remember his name, or the book's name.
ok, all the pipes are in place, and i'm ready to try to approximate size of the radiators
@MolbOrg so, now i've looked over the WB answer you referenced before, with the section on radiators, and i've looked at your additions to the spreadsheet, and i'm trying to figure out how i adapt that to what i'm doing here.
this system has 4 radiators, each one using a different fluid in the heat pipes running to the radiator surfaces, and the coolant goes from one heat exchanger to the next so that each radiator can cool it more, and then circulates back to the cold end of the Stirling engines
so, on the spreadsheet you consider pretty small changes in the temperature of the coolant, and i don't know what you were doing there. My understanding is that this system has to take the heat of the hot end, which is 1450 K, and cool it to the cold end temperature, which is 300 K
since the heat is never going to be cleanly one temperature on the inlet, is it that the thing to do is take the average?
but then, do we have to think in terms of the watts that need to be shed, or something?
even though this is 0th degree, it would be nice if the radiators weren't clearly off in a way a good engineer would spot.
so, i don't know how much i need to work through this and understand it better right now, but maybe i need to know a bit more in order to take your input and size the damn thing
i need to figure out j - that seems to be my task right now for each level of the rad
"My understanding is that this system has to take the heat of the hot end, which is 1450 K, and cool it to the cold end temperature, which is 300 K" - if you need such big difference in cooling of waste heat you doing something wrong
steam gets in inlet of the turbine under pressure and 550C temperature and gets out of the turbine with a temperature below 100C (about 60C) but with pressure below 1 bar
and for what they cool down the thing - to condense the vapor - hidden heat capacity(?) - the energy they have to get rid of. it might be at the same temperature all along
yes, phase change and its heat - then they pump the water back in the system
the main cooling from hot end to cold end happens in the engine itself - by making the work
that is the whole point of particular cycles (not all of them)
when there is not phase change - you cool the output while compressing it
so the output can have the same temperature during the whole process of compressing the thing back. then they heat the compressed thing and let it do the work - which cools it down
and you get those paralelargamm like plots on P-V graph
you can heat the working carrier all time during its work in the engine - and can get the output at the same temperature as the hot end temperature. But usually, it is in engines which do not reuse heat carrier(roughly speaking)
The Stirling cycle is a thermodynamic cycle that describes the general class of Stirling devices. This includes the original Stirling engine that was invented, developed and patented in 1816 by Robert Stirling with help from his brother, an engineer.
The ideal Otto and Diesel cycles are not totally reversible because they involve heat transfer through a finite temperature difference during the irreversible isothermal heat-addition and heat-rejection processes. The irreversibility renders the thermal efficiency of these cycles less than that of a Carnot engine operating within the same limits of...
in this simplistic diagram your coolant will change temperature slightly, if not then the gas in cylinder will not reach 300K and will make less work and will be less efficient
the connection between the two piston chambers of a stirling engine does mean that some of the heat of the hot chamber is always being pushed to the cold chamber
and the 300K coolant is what you should cool in radiators - and less the difference of temperatures of the coolant then better, but not realistick because it needs infinite supply of it or very rapid movement in cooling system
@kimholder yes, not in all cases, as example jet engines - but they have infinite supply of fresh cold air so they do not care
so, the volume of the piston chambers has one working fluid, that is passing heat to the coolant passed around the chamber, which is probably a different fluid
you have an electric power you need (10MW) you have an efficiency of the engine ((Thot-Tcold)/Thot
if efficiency is 50% as an example - you supply 20MW heat power from your heat reservoir, you get 10MW electric power, 10MW heat power which you need to get rid of
well, this is a modular unit now. i need to figure out how much power it can be expected to produce, and then set up a bunch of them, so they add to 10 MW
i worry now too much about things melting or being insanely hard to pump fast enough, since you have started talking to me about this
so i made the heat store much smaller so the problem is manageable
alright - the thing is i was thinking in terms of the heat coming in much hotter. it didn't seem right, but the definition of efficiency is hot end vs. cold end, so i thought that had to be part of the calculation somehow
power, efficiency, cold end temp - those are freeing you from defining working fluids, those variables are independent of that. However, in fact, cold end temperature is dependent on working fluids and design of the system.
it will be defined by the limitation of the system and which materials it uses, which gases/liquids it uses etc
but you can select the temperature arbitrary in hope that there will be a design which satisfies the requirement
the design system here is different. it starts with the best numbers that can be reasonably expected, and then figures out what the system needs to be.
@MolbOrg exactly
that is what i've spent quite a lot of time doing, figuring out the best reasonable numbers.
i really don't think they are excessive, i tried my best to put them where they can be done. and sized the system with that consideration too.
and show that some system can work and if one will offer a better system I will be much happier, but I aware about my limitations and do not try to bite more than I can chew )
it uses one because a range of temperatures is not high, and because it relays on a way to extract the heat media from ISRU and because it requires a lot of it. - those are reasons for that. Another reason it is just simpler to estimate things when such systems are can be considered independantly
yes, but i can't model it. that's why i set it aside. and that brings me back to the need to estimate heat the radiators need to shed, which requires me to estimate how much power this thing is producing
i put a guess of 380 KW on the spreadsheet, but i don't know if that was good or not
"estimate how much power this thing is producing" - if you mean radiator then it does not produce and how much it is from - PowerElectrical/efficiency - Power electrical = how much radiator has to dissipate
Electrical power is assumed value - based on requirements of the base
it isn't arbitrarily a certain power, it has been set up so that the aluminum heat carrier can be pumped reliably fast enough to keep the pipes in the mirrors at a good temperature
alright, forget the damn modularity, look at the sizes in the spreadsheet
(she says, to the person who convinced her it was necessary to make it modular in the first place.)
true, so you do not calculate the sizes for a total 10MW base consumption - but you just calculate systems for a 10MW of electricity production. If they need more 100MW they will just build another 9 systems like that and that all - not problem there in assuming some number.
look. i have designed a unit. we don't need to talk about how many we are going to need. we need to talk about how much power that one unit - which, i feel a need to comment, i have spent like 6 weeks building - is going to produce.
if you don't see how the spreadsheet is working, the thing is the heat store receives about 3 MW of heat all through the day
there is probably something connected wrong, that is why it doesn't make sense to you...
let me check it
E5 and H5 are showing the heat coming in per square meter, and the heat shed
look at G9
that is that 3 MW times the efficiency, divided by 2 as a really simple consideration of the night
solar light is about to be parallel so the shadow will be about the size of pipe, so we loose light and od not squeeze max o the installation, however, there might be some manufacturing reason for that
@MolbOrg that's true, but the base being worked on right now is at the equator, and it will be producing gasses that need liquifying. oxygen, at least.
the assets are all stored right now on GitHub
except for a few things that are outdated, and even some of that is there