O'Neill Cylinders
I'm writing a bit of background material and I have come to the point where I want to briefly mention the construction of some really big habitats in space. I don't want to interrupt the flow of the text (which is historical overview material), but I would like to give the readers an idea of what the structures are: hollow cylindrical worlds spinning on their long axes, about the size of Arthur C. Clarke's Rama. That is, fifty kilometres long, twenty kilometres wide, and with an interior surface larger than the land area of Rhode Island or Luxembourg.
Now, the term "O'Neill cylinder" is sometimes used for this design in SF, and I propose using "O'Neill" as the in-setting term for these large cylindrical habitats (as opposed to the smaller "Stanfords", which are wheel-shaped rather than fully enclosed). But O'Neill's design was actually for a much more elaborate and specific design, with two cylinders counter-rotating, a separate agriculture ring, windows for natural lighting, etc. Question: is "O'Neill cylinder" going to be misleading if used in the common sense without explanation? Supplementary: anyone know off hand the limits for stability for a hollow cylinder rotating about its axis? |
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I don't think most people have read High Frontier. Plus calling all the big cylindrical habs "O'Neils" is just the kind of popular corruption that would reasonably propagate.
I think you'd be okay. |
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A thin cylindrical shell - a hollow cylinder without endcaps - with mass M and radius R has a moment of inertia of MR^2 for rotation around its center axis. A uniform circular disk - one of the endcaps of the cylinder - with mass M' and radius R has a moment of inertia of M'R^2/2 for rotation around its center axis. The cylinder will have two of these endcaps. Thus, the moment of inertia for the entire hollow cylinder is MR^2 + 2 * M'R^2/2 = R^2 (M + M'). A hollow cylinder of length L, radius R and mass M without endcaps rotating around an axis perpendicular to its primary axis has a moment of inertia of M(L^2/12 + R^2/2). A disk M' of radius R oriented perpendicular to its axis of rotation at a distance of L/2 - the endcap - has a moment of inertia of M'(L/2)^2 + M'R^2/4. Again, there are two endcaps. Thus, for a hollow cylinder tumbling end over end, we have a total moment of inertia of ML^2/12 + MR^2/2 + 2 * (M'(L/2)^2 + M'R^2/4) = L^2 (M/12 + M'/2) + R^2 (M + M')/2 If the cylinder and endcap both have a uniform areal density D (probably equal to 1 ton/m^2, as this is sufficient to cut the dose from cosmic radiation down to levels without known long term health risks), then M = 2 * pi * R * L * D, M' = pi * R^2 *D. For rotation about the cylindrical axis, this gives I_z = pi * R^3 (2 * L + R) * D. For end-over-end tumbling, on the other hand I_x,y = pi * L^2 R (L / 6 + R / 2) * D + pi * R^3 (L + R/2) D And we need I_z > I_x,y for stability. This gives us the condition R^3 + 2 * L R^2 - L^2 R - L^3 / 3 > 0 Since it is late, I'm not going to solve this cubic inequality now (or check my work, for that matter - others may wish to look it over for accuracy), but will note that cubic equations do have closed form solutions, so you can find the allowed values of R in terms of L that give you a cylinder that rotates stably about its axis rather than tumbling end over end. http://en.wikipedia.org/wiki/Cubic_equation Luke |
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R = 20: L < 33 L = 50: R > 30 In other words, if lwcamp did his math right, your O'Neil cylinder isn't going to be stable if it's got a radius of 20 kilometers and a length of 50 kilometers. |
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Which means I'm stuck with active stabilisation, I think. |
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The "natural" stability of L4 and L5 gets overrated too. You need to maintain your physical plant, you're going to need to maintain your stability too. |
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1) Ditch the precession and use mirrors to keep the sunlight aimed in. 2) Increase the moment arm with some sizeable masses on spokes. These needn't be entirely deadweight, they can be high-gravity applications like wastewater separation or detention. Or if the yoke technology was realistic, you could mount the spokes on coaxial bands like barrel hoops and have them spinning at slower rates for the same apparent gravity, less gravity for invalids and sybarites, or adjustable if you like. |
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Okay, so the Imperial Capitol in FLAT BLACK is going to be 20 km in diameter and 60 km long including hemispherical end-caps. Lit by a string of lights down the middle. It has a usable interior surface of nearly 3,000 square kilometres, making it larger than Luxembourg or Delaware. Most offices, residences, and such facilities can be under "ground", or rather, the interior can consist largely of a huge roof garden. Places with view windows will do best on the slopes of the end-caps.
With a population of, say 500,000, the Imperial Senate buildings and residences for a thousand senators and staff, can we spare room for a military academy? One campus of the military academy? Or should all military academies be put where cadets can bang off guns safely? What's a good level of centripetal acceleration ("gravity") for such a place? 10 ms^-2 is a "standard gravity". 9.81 ms^-2 recalls the gravity of Old Earth. About 8.5 ms^-2 would be about average for people growing up in the colonies (weighted by population) and very convenient in GURPS rules. 10 ms^-2 would require that the place rotate at about 0.3 RPM. |
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By the way, does anyone know of a suitable ray-traced (not artist's impression) interior shot for something like this? I'd like one without Island Three-style longitudinal windows, and without the Rama-style spikes in the end-cap.
I already have these on Youtube: |
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An experiment involving several generations of chickens and a centrifuge showed that they are healthier when raised under higher gravity. So farming should be OK.
Having your cadets train under varying g levels would also be useful. |
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And using O'Neill as a general term for rotating cylindrical space habitats that aren't too large (several hundreds of kilometers) is fine. |
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http://panoptesv.com/Zoe/wheels/habitat.html Luke |
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What about high-speed flywheels at the caps of the tube to provide stability?
Also, when I was doing similar thought experiments and web investigations, I found that you need a very large radius to approach proper "radial" gravitation, otherwise you can still feel rotating frame effects. These include differing ballistic trajectories depending on the direction you're firing, vertical drops being slanted, and weight varying with your direction of travel. There was a nifty flash animation I found somewhere for simulating dropping or throwing a ball in a rotating frame. |
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I don't think it will affect anyone's Rugby skills. |
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If it instead runs north-south, play will tend to drift to the East side of the pitch, as it will be easier to pass east. |
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I think Rotating Frame G-Experience would be a valid enhancement if you want to go for realism. |
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Blown up or no, my point is that they don't necessarily have to go far afield to have those environments available for training, especially if there's a place purpose-built for high-budget, short-time-span tourism/dversion. Like the luxurious capital space habitat described. |
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For slow RPM rotations, like in an O'Neill size habitat, the coriolis(sp?) effect should be neglible, but for much smaller habitats it will be an issue. |
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:) |
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http://panoptesv.com/Zoe/wheels/ringscenelg.html what you would perceive when standing on the ringworld would be the ring going straight up, but in ray tracing you get a tilted looking projection unless the ring is right in the center of your field of view. Luke |
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And a 15% easier in antispin vs 15% harder spin throw definitely means sufficient difference to alter play... and a lot more missed throws due to differences in ball performance. |
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I built a little calculator for the thickness of the structural hull, mass of the hull and contained atmosphere for a rotating cylindrical habitat, as functions of the length and radius, the "gravity" and air pressure, the mass-per-unit-area of the shielding, armour, landscaping, and fittings, and the strength and density of the structural material. It's an Excel workbook with no macros.
Just at the moment the list of possible building materials is a bit incomplete and some of the values for strength questionable. I put it on Dropbox for review and personal use: https://www.dropbox.com/s/7iilf35hdx...ator.xlsx?dl=0 |
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