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10:34 am February 8, 2010
| brmj
| | Rochester, New York, United States | |
| Member | posts 349 |
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Good work! This looks like it is really comming along. I agree that the second image could be great for some of our promotional material.
I've been trying to find some similar images from the internet to sanity check your results, but so far I haven't found much. However, your results do look a lot like what Wikipedia tells me the behavior of a nozzle with ambient exit pressure (the optimum) ought to look like.
Making sense of your earlier results, wikipedia tells me that grosely overexpanded nozzles have increased thrust but highly unstable exhaust jets.
Source.
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Main work groups: Propulsion (booster), Spacecraft Engineering, Computer Systems, Navigation and Guidance (software)
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10:59 am February 8, 2010
| Rocket-To-The-Moon
| | Grand Forks, North Dakota, USA | |
| Member | posts 572 |
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What are the physical dimensions of this rocket? I see that you have scales on the images, but it is hard to tell accurately. 143 kN is a lot of thrust (as much as an F-16 fighter jet)!
Have you spoken with anyone regarding fabrication of parts and pieces? If you can get a local machinist interested you could probably expect him to help mill out the parts.
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Main Workgroups: Propulsion & Spacecraft Engineering
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11:13 am February 8, 2010
| brmj
| | Rochester, New York, United States | |
| Member | posts 349 |
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Rocket-To-The-Moon said:
What are the physical dimensions of this rocket? I see that you have scales on the images, but it is hard to tell accurately. 143 kN is a lot of thrust (as much as an F-16 fighter jet)!
Using the provided scale, it appears to be .5 meters in diameter and about 5.5 meters long. I'm not sure if the length numbers are arbitrary or not, though.
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Main work groups: Propulsion (booster), Spacecraft Engineering, Computer Systems, Navigation and Guidance (software)
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11:22 am February 8, 2010
| Luke Maurits
| | Adelaide, Australia | |
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The best way to approach the scale issue is to figure out what sort of delta-v we want (USOFS wll help with this), then use the rocket equation to figure out the propellant masses we would need for various propelland choices (I have a table of Isp values for common hybrid propellant choices in my hybrid rocketry text book) and then use density/pressure figures to figure out the required volume.
This will give us a volume, and to come up with radius and length values we will need to decide on a ratio between these two. Obviously smaller radii lead to less drag (drag is proportional to cross sectional area, which is proportional to radius squared). Of course, if we let the radius get extremely small and the length extremely long, there would be problems associated with that too. Looking to other suborbital sounding rockets for guidance on radius to length ratios might be a good idea.
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Starting a new TA job next week, might be busy for a while! Main CLLARE workgroups: Mission Planning, Navigation and Guidance. I do maths, physics, C, Python and Java.
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12:23 am February 9, 2010
| rpulkrabek
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brmj said:
I've been trying to find some similar images from the internet to sanity check your results, but so far I haven't found much. However, your results do look a lot like what Wikipedia tells me the behavior of a nozzle with ambient exit pressure (the optimum) ought to look like.
Making sense of your earlier results, wikipedia tells me that grosely overexpanded nozzles have increased thrust but highly unstable exhaust jets.
Source.
Thanks, this is good to know. I was always pessimistic about my results because the nozzle shape wasn't looking like other nozzles I have seen, such as the one at SpaceX. After reading a bit from the Wikipedia link you provided, I assume that SpaceX is then optimizing for a thrust at near vacuum. Since OHKLA is to be optimized near atmospheric pressure, the shape will be different. I now feel more confident with this, but of course, let's still be pessimistic as to not over look some error.
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12:42 am February 9, 2010
| rpulkrabek
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Post edited 12:43 am – February 9, 2010 by rpulkrabek
Rocket-To-The-Moon said:
What are the physical dimensions of this rocket? I see that you have scales on the images, but it is hard to tell accurately.
Have you spoken with anyone regarding fabrication of parts and pieces? If you can get a local machinist interested you could probably expect him to help mill out the parts.
The scale from the pictures isn't really meant to accurately measure the rocket as much as it is to give an idea of what the size is. I could create nice 2D CAD documents with the measurements shown, but at the moment, I only have my work's default template with their logo and such. I'll see if I can come up with a modified one. Maybe at some point, we can have an official CSTART CAD template. This will have to wait until a later time when things are more complete.
For now, I can provide screenshots with quick measurements. The measurements of the rocket as a whole should not be taken seriously. They are just guesses based on what others have done. We should take the approach Luke had mentioned and use the equations to determine the radii and lengths needed to provide the delta-v we desire. All measurements are in mm.
 
The nozzle geometry is what I spent my time working on and has more accurate dimensions. Keep in mind, however, the dimensions will change based on what the dimensions will be for the rocket itself and the combustion pressure that occurs.
 
To answer your second question, no, I haven't asked anyone about machining these parts. This would have to wait until we are ready to start testing, I believe. Perhaps brmj could even do some of this from his university. A static test would be a great start once we know the fuel grain geometry and fuel composition we are using. That sounds quite exciting; I wonder how far away we are from that.
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12:51 am February 9, 2010
| Luke Maurits
| | Adelaide, Australia | |
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Post edited 12:55 am – February 9, 2010 by Luke Maurits
rpulkrabek said:
once we know the fuel grain geometry and fuel composition we are using. That sounds quite exciting; I wonder how far away we are from that.
I will try to make some more posts later tonight with the express aim of clearing this up and getting us better on track for a static test. :)
EDIT: Note to self: don't forget to discuss precombustion chamber.
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Starting a new TA job next week, might be busy for a while! Main CLLARE workgroups: Mission Planning, Navigation and Guidance. I do maths, physics, C, Python and Java.
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1:35 am February 9, 2010
| brmj
| | Rochester, New York, United States | |
| Member | posts 349 |
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Post edited 1:42 am – February 9, 2010 by brmj
I can pretty much guarantee that the thrust numbers are bogus in the context of what OHKLA will actually be getting. This image shows a thrust graph from a HATV test. They get nothing near 143 kN. Something is obviously going wrong, but the fact that the flow patterns we are getting line up with what is expected suggests something is also going right. Just on a hunch, would you mind rerunning it with lower chamber pressures? Typical chamber pressure seem to scale with rocket size as far as I can tell, and the upper stage engine in a Falcon 1 runs at .93 MPa. I'm not quite sure what we can reasonably expect, but 3 MPa may well be too high.
I've been wikipediaing rocket engines pretty heavilly, and these numbers just aren't lining up. I'm not sure exactly what the underlying issue is, but there seems to be one.
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Main work groups: Propulsion (booster), Spacecraft Engineering, Computer Systems, Navigation and Guidance (software)
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1:55 am February 9, 2010
| Luke Maurits
| | Adelaide, Australia | |
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We will certainly not be getting anything close to 143 kN, nor, I think, would we want it.
Chamber pressure may well be what is at fault here – was the current number chosen according to any kind of logic or is it just a random figure?
Another thought: the streamlines in these situations seem to show a nice, laminar flow through the length of the fuel grain, which could not possibly be further from the true situation of a hybrid rocket. Things like temperature, density, velocity and turbulence are all going to vary along the length of grain due to the combustion process. It might make more sense to simply prescribe sensible values for these at the end of of the combustion chamber, for the purpose of investigating nozzle shapes.
Surely there are some nice analytic models for de Laval nozzles we can use for some basic sanity checking?
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Starting a new TA job next week, might be busy for a while! Main CLLARE workgroups: Mission Planning, Navigation and Guidance. I do maths, physics, C, Python and Java.
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2:05 am February 9, 2010
| brmj
| | Rochester, New York, United States | |
| Member | posts 349 |
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If I remember correctly, the pressure number was arbitrary.
I'm not sure if the issue of the flow through the grain would matter, or if the postcombustion chamber would even it all out. In this particular model, however, the grain doesn't seem to do anything interesting to the flow, so I'm not sure how that could make a difference. I might have missed something, however.
I don't realy know what I'm doing here, unfortunately, but I suspect that there is some model we could use for sanity checking. I suppose I could go ask the Project Meteor people what they do for this sort of thing. Another option might be to ask the Copenhagen Suborbitals for a bunch of HATV data and, if we get it, compare our results to their actual static tests and, if they are grossly off, try an figure out why.
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Main work groups: Propulsion (booster), Spacecraft Engineering, Computer Systems, Navigation and Guidance (software)
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2:18 am February 9, 2010
| rpulkrabek
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3 MPa was only a guess to what chamber pressure to use. I am not quite sure what our fuel of choice will produce. I can surely run a new set of simulations for a lower combustion pressure. What pressure should I use, 1 MPa? 0.5 MPa?
As for the fluid flow through the fuel grain, I can reassign the "inlet" as well. At the moment it as at the very top of the fuel grain housing. Is it better to have the inlet at the end of the fuel grain, or would it be even better to have the inlet assigned to every surface of the fuel grain?
I am unable to perform the simulations today, it will have to wait until maybe tomorrow. After I get the conditions/boundaries setup, will take about a day to simulate. So, before I run these, let me know your thoughts on what should be set as inputs.
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2:30 am February 9, 2010
| brmj
| | Rochester, New York, United States | |
| Member | posts 349 |
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3 MPa was only a guess to what chamber pressure to use. I am not quite sure what our fuel of choice will produce. I can surely run a new set of simulations for a lower combustion pressure. What pressure should I use, 1 MPa? 0.5 MPa?
As for the fluid flow through the fuel grain, I can reassign the "inlet" as well. At the moment it as at the very top of the fuel grain housing. Is it better to have the inlet at the end of the fuel grain, or would it be even better to have the inlet assigned to every surface of the fuel grain?
I don't know, something in that range I guess. Let's arbitrarily say perhaps 0.5 MPa, unless someone else has a reason to favor some particular value. Unfortunately, we don't have good numbers to estimate this off of yet as far as I can tell.
As for the fluid flow through the fuel grain, I can reassign the "inlet" as well. At the moment it as at the very top of the fuel grain housing. Is it better to have the inlet at the end of the fuel grain, or would it be even better to have the inlet assigned to every surface of the fuel grain?
The absolute most accurate way to do this would be to have some come off of the grain, and some off of the top of the housing, since there will be an excess of oxidizer in the gas mix. That said, I am of the opinion that this shouldn't be a big factor in what it does beyond the grain.
I am unable to perform the simulations today, it will have to wait until maybe tomorrow
Okay, no hurry. You've been doing a lot of great work. Thanks.
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Main work groups: Propulsion (booster), Spacecraft Engineering, Computer Systems, Navigation and Guidance (software)
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2:54 am February 9, 2010
| Luke Maurits
| | Adelaide, Australia | |
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Okay, time for some numbers!
At this Wiki page (which will hopefully slowly grow with time to be a good repository of hybrid rocket info) I have began transcribing a table of propellant info from the hybrid rocket textbook I currently have on loan. Please note that this is a small portion of the entire table – I have focused on the propellants that seem most likely for us because I don't have too much spare time at the moment. I will endeavour to complete the table in time.
The values in the table are supposedly for P_c = 500 psia and P_e = 14.7 psia. Frustratingly, the book doesn't seem to explain these variables, but it seems a likely bet that P_c is combustion chamber pressure and P_e is the external or ambient pressure (because 14.7 psia is in fact mean sea level pressure). So this straight away suggests that 500 psia is a decent ballpark for combustion chamber pressure. Converting this into sensible units gives 3447.378647 kPa, or about 3.4 MPa, so rpulkrabek's pressure figure is actually pretty close to the mark. Good to know.
Now, re: propellants. Our most likely oxidisers seem to be LOX or N2O. I was originally quite a fan of N2O because it is self pressurising and not as cold as N2O, making it simple and safe. However, I am starting to rethink this. Not only does it give lesser performance than LOX, but in a sense it minimises OHKLA's usefullness. When it comes to CLLARE and other, larger projects, we are going to have to use LOX for things to be practical. This means that we will eventually need experience with (1) safe LOX handling and (2) use of helium pressurants. We might as well get that experience from OHKLA, otherwise OHKLA is kind of useless as a learning experience (and remember it was originally conceived as a learning experience for a large hybrid cluster booster). So LOX seems like a really sensible choice. Do people agree with this line of reasoning?
As for fuel, we were initially quite keen on paraffin, because it is very cheap, very safe, and very familiar, so easy to cast our own grains with. Gary Schnyder commented that he was not a fan of paraffin (or hybrids in general, really), giving two main reasons. One was that it is tricky to cast because it expands while drying. I think that, for our purposes, this is a moot point since Copenhagen Suborbitals have clearly figured out a way to do it and they should be more than happy to show us how. Gary's other reason was that paraffin, especially when hot, has very little structural strength. Accelerate it too hard and it is likely to slump, potentially closing off combustion ports and causing other problems. This seems like a valid concern – I note that CS appear to have only done static tests of their paraffin motors, so they wouldn't necessarily know how to deal with this. Considering OHKLA is going to involve very high acceleration, paraffin slumping could be a very real concern. Still, we may not want to rule it out entirely.
The most popular fuel seems to be HTPB. I don't know if we could make this ourselves but apparently it is farily easy to find commercially.
At any rate, it looks like we can expect to be working with an Isp between 250 s and 280 s. This number, combied with the O:F ratios in the table, should help us roughly estimate the mass of propellants required, and hence the rocket size, once we have chosen propellants and know the delta-v.
I will play around with USOFS a bit later tonight and try to get a suitable delta-v figure.
To get the propellant mass figures I will need an estimate of the empty rocket mass. Anybody want to throw out some figures?
A final thought on propellant choice: the more fuel we need (not oxidiser), the larger the combustion chamber has to be. Large combustion chambers are heavy, which is bad. Hence it seems like it might make sense to target a propellant combo with a high O:F ratio (i.e. mostly oxidiser), since oxidiser tanks can be made much lighter since they have to endure much less pressure.
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Starting a new TA job next week, might be busy for a while! Main CLLARE workgroups: Mission Planning, Navigation and Guidance. I do maths, physics, C, Python and Java.
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2:58 am February 9, 2010
| Luke Maurits
| | Adelaide, Australia | |
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Post edited 3:00 am – February 9, 2010 by Luke Maurits
Oh, another thought on explaining the absurdly high thrust estimates: to get a thrust estimate from the gas exit velocity and the nozzle area, we naturally also need a gas density. This will certainly depend on the choice of propellants. What have we been using for this so far? Due to the high temperatures involved, I expect the density will be quite low. If the simulations so far have been using standard density of air or something, that could explain things.
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Starting a new TA job next week, might be busy for a while! Main CLLARE workgroups: Mission Planning, Navigation and Guidance. I do maths, physics, C, Python and Java.
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3:30 am February 9, 2010
| Luke Maurits
| | Adelaide, Australia | |
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| posts 1083 |
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See some important and relevant thoughts on OHKLA in this thread.
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Starting a new TA job next week, might be busy for a while! Main CLLARE workgroups: Mission Planning, Navigation and Guidance. I do maths, physics, C, Python and Java.
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4:43 am February 9, 2010
| rpulkrabek
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| Member | posts 150 |
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Luke Maurits said:
Okay, time for some numbers!
At this Wiki page (which will hopefully slowly grow with time to be a good repository of hybrid rocket info) I have began transcribing a table of propellant info from the hybrid rocket textbook I currently have on loan. Please note that this is a small portion of the entire table – I have focused on the propellants that seem most likely for us because I don't have too much spare time at the moment. I will endeavour to complete the table in time.
Great, this will help out quite a bit! My only suggestion is that we keep the units metric. Also, to avoid confusion, it might be a good idea that we start writing pressure like kPaa or kPag for absolute and gauge pressures. Thanks for starting this, I would like to think that over time, these types of tables will be quite complete.
Luke Maurits said:
To get the propellant mass figures I will need an estimate of the empty rocket mass. Anybody want to throw out some figures?
Do you need the mass of the rocket minus the oxidizer and fuel grain? If so, with every component currently assigned as steel, the Pro/E model I have gives the following information with a coordinate system at the center of the nozzle diameter (the very bottom of the rocket):
VOLUME = 4.8727940e+08 MM^3
SURFACE AREA = 2.6528419e+07 MM^2
AVERAGE DENSITY = 7.8270800e-06 KILOGRAM / MM^3
MASS = 3.8139749e+03 KILOGRAM
CENTER OF GRAVITY with respect to DEFAULT coordinate frame:
X Y Z 0.0000000e+00 2.6753948e+03 0.0000000e+00 MM
INERTIA with respect to DEFAULT coordinate frame: (KILOGRAM * MM^2)
INERTIA TENSOR:
Ixx Ixy Ixz 4.2233764e+10 0.0000000e+00 0.0000000e+00 Iyx Iyy Iyz 0.0000000e+00 3.4322134e+08 0.0000000e+00
Izx Izy Izz 0.0000000e+00 0.0000000e+00 4.2233764e+10
INERTIA at CENTER OF GRAVITY with respect to DEFAULT coordinate frame: (KILOGRAM * MM^2)
INERTIA TENSOR:
Ixx Ixy Ixz 1.4934334e+10 0.0000000e+00 0.0000000e+00
Iyx Iyy Iyz 0.0000000e+00 3.4322134e+08 0.0000000e+00
Izx Izy Izz 0.0000000e+00 0.0000000e+00 1.4934334e+10
PRINCIPAL MOMENTS OF INERTIA: (KILOGRAM * MM^2)
I1 I2 I3 3.4322134e+08 1.4934334e+10 1.4934334e+10
ROTATION MATRIX from DEFAULT orientation to PRINCIPAL AXES:
0.00000 0.00000 1.00000
1.00000 0.00000 0.00000
0.00000 1.00000 0.00000
ROTATION ANGLES from DEFAULT orientation to PRINCIPAL AXES (degrees):
angles about x y z 0.000 90.000 90.000
RADII OF GYRATION with respect to PRINCIPAL AXES:
R1 R2 R3 2.9998409e+02 1.9788096e+03 1.9788096e+03 MM
Luke Maurits said:
Oh, another thought on explaining the absurdly high thrust estimates: to get a thrust estimate from the gas exit velocity and the nozzle area, we naturally also need a gas density. This will certainly depend on the choice of propellants. What have we been using for this so far? Due to the high temperatures involved, I expect the density will be quite low. If the simulations so far have been using standard density of air or something, that could explain things.
I have been using N20 as a combusted gas. I am not sure what the density of it was though. If I remember, I can find out more specifics when I have access to a work station tomorrow.
I should also point out that the entire enclosure the model was simulated in was N20. For a future simulation, it would be nice to have the enclosure as air and the combusted fluid as N20. It might also be beneficial to have another inlet of air at the front of the rocket.
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5:21 am February 9, 2010
| Luke Maurits
| | Adelaide, Australia | |
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rpulkrabek said:
MASS = 3.8139749e+03 KILOGRAM
First of all, it's really awesome that your software can simply give us mass etc. figures like this.
Second of all, 3 tonnes?!?!?! Even using steel, that sounds like way too much to me. Have I missed something?
As for using N2O as the gas, this may be the problem. While some uncombusted N2O may make it out of the nozzle, much more of the exhaust gas will be composed of the byproducts of the combustion reaction. N2O's role in the reaction is as an oxidiser, so I would suspect that straight nitrogen gas, N2, is part of what comes out the other end (and obviously N2 is less dense than N2O). The fuel quite likely contributes something to the exhaust gas, too. CO2 and H2O seem like likely candidates to me, but I'm not a chemist. Even if we are able to figure out the exact mix of gases that comprise the exhaust, we won't be able to reckon an accurate density without knowing the combustion temperatures either. Fortunately, finding combustion temperatures for common propellants shouldn't be too hard. There may even be tables of this in the book if I look around.
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Starting a new TA job next week, might be busy for a while! Main CLLARE workgroups: Mission Planning, Navigation and Guidance. I do maths, physics, C, Python and Java.
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6:49 am February 9, 2010
| rpulkrabek
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Post edited 6:57 am – February 9, 2010 by rpulkrabek
Luke Maurits said:
First of all, it's really awesome that your software can simply give us mass etc. figures like this.
Second of all, 3 tonnes?!?!?! Even using steel, that sounds like way too much to me. Have I missed something?
After reading how you said that, I was a bit shocked too. Then after thinking about it logically, yes, I guess it is about 3 tonnes of steel. As an example, I'll go through the steps of the mass for the oxidizer tank, which is roughly 3 meters tall and has an outside diameter of 255mm and an inside diameter of 215mm.
l=3000mm
r_o=255mm
r_i=215mm
d_steel=7.85g/cm^3 => d_steel=7.85*10^-6kg/mm^3
V=l*pi*r_o^2-l*pi*r_i^2=1.7719*10^8mm^3
m=V*d_steel=1390.9kg
So, the oxidizer tank alone has a mass of about 1.4 tonnes. According to Pro/E, I am given the mass to be 1.4096042*10^3kg.
The values from Pro/E are correct, it's the design of the rocket that needs rethinking. Do we go with steel as the material or do we choose something better? I am sure the wall thicknesses don't need to be as thick either.
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7:00 am February 9, 2010
| Luke Maurits
| | Adelaide, Australia | |
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Hmm, okay, so the figures are correct. It seems like either the rocket is far too tall/wide and/or the walls are far too thick. The rocket shouldn't weigh anywhere close to 3800 kg, even if we do use steel. The Atea 1 rocket has a fuelled mass of just 60 kg and gets to an atltitude of 150 km. We should expect the OHKLA rocket to have a fuelled mass of, I think, no more than 100 kg, certainly less than 150 kg or 200 kg at absolute most. A figure of 3.8 tonnes is just insane.
While steel is a bad choice for its mass, it's also quite appealing in that it is cheap, easy to find and easy to work with. I think we should use it wherever we can get away with doing so. For the most massive parts (like the combustion chamber) we could fall back on aluminium if we need to shed some mass. Things like the nose cone and fins can probably be done using fibreglass or, if we can afford it, carbon fibre.
Is it easy enough in your Pro/E model to specify different material densities for different parts of the rocket? E.g. could we set the combustion chamber to aluminium, the nose and fins to fibreglass and the rest to steel, or something like that? Or do you have to set the density of the entire thing as a whole?
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Starting a new TA job next week, might be busy for a while! Main CLLARE workgroups: Mission Planning, Navigation and Guidance. I do maths, physics, C, Python and Java.
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7:04 am February 9, 2010
| rpulkrabek
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Luke Maurits said:
As for using N2O as the gas, this may be the problem. While some uncombusted N2O may make it out of the nozzle, much more of the exhaust gas will be composed of the byproducts of the combustion reaction. N2O's role in the reaction is as an oxidiser, so I would suspect that straight nitrogen gas, N2, is part of what comes out the other end (and obviously N2 is less dense than N2O). The fuel quite likely contributes something to the exhaust gas, too. CO2 and H2O seem like likely candidates to me, but I'm not a chemist. Even if we are able to figure out the exact mix of gases that comprise the exhaust, we won't be able to reckon an accurate density without knowing the combustion temperatures either. Fortunately, finding combustion temperatures for common propellants shouldn't be too hard. There may even be tables of this in the book if I look around.
Good point. I'll try to investigate further into what types of material properties can be used. I do remember seeing some sort of combustion branch in the setup tree, so it could be possible that we can specify the material involved in the combustion and the software will solve the rest, but this is also probably wishful thinking.
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