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how hard would it be to build a Dyson Sphere about 2 au in diameter with no star at its center? Lets say the Dyson Sphere had the mass of Jupiter, it consists of two shells with hydrogen gas sandwiched in between. Jets on the inside of the shell accelerate the hydrogen toward the center of the sphere to impact it with such force that the hydrogen fuses to form helium in a sun like nuclear reaction but without a sun if it fuses as much hydrogen per second as the Sun does at its core, it would release as much energy as does the Sun, collectors on the inside of the Dyson shell would then collect the energy and turn some of that energy back towards accelerating more hydrogen towards the center of the sphere releasing more energy through fusion. The thing to remember is while the fusion reactor would produce as much energy as the sun, it wouldn't have the mass of the Sun, so this removes the requirement of the Dyson Sphere to hold itself out against the gravity of a star, since there is no star there, only a fusion reaction. So lets say we took apart Jupiter to make this Dyson Sphere and placed it outside the Solar System far enough away so the Sun's gravitational effects are manageable with ordinary materials. Much of Jupiter is made of hydrogen, the solid part, its core would be used to make the outside and inside walls of this shell to contain the hydrogen within. Perhaps there is room between the shells to put 50 meters of breathable air in weightlessness lluminated by artificial light powered by the fusion reaction at the center of the sphere.
Last edited by Tom Kalbfus (2014-06-18 16:07:06)
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You can't escape the virial theorem.
In order the shell to excert enough P/T in the core to fuse the combined weight towards within must balanse exactly the pressure towards outside.
I.e. your shell/reactor system MUST mimic in mass/pressure a real star.
I proposed similar concept regarding terraformation of stars / fusors - regardless whether brand new ( accumulating mass from clouds and/or interstellar/intergalactic medium or existing.
Outer layers to be growing habitat ( like a mollisk or coral ), the core to be growing reactor, which provodes not only the energy to keep the habitat on 1 gee radius, but also to transmutate hydrogen and helium into "metals" for consruction material. Something like controlled manner "main sequence excursion".
One can start with little planet or no planet at all, and to step by step lift more and more floors all the time keeping them on the ~1 gee zone.
The habitat could be the pressure excerting outer stellar layers, which anyway do not take part in the fusion.
Using 3K radiator the Sun only could have trillions of Earth area-wise of habitat area. Adding more mass = more habitat ...
Till we reach the Supra-self level.
9. BLUE SKIES
That's more or less it for custom planets. Except for those planets of gold I mentioned.
Unfortunately, there's not enough gold in the asteroids, the cores of gas giants, or even the atmospheres of stars. To satisfy our lust we must seek out, the neutron stars, where mass transmutation of the elements goes on. Neutron stars are the philosophers' stone of the universe.
To mine a neutron star (Fig 9.1) we use the powerful magnetic fields of the star itself and an energy beam spearing down to the magnetic pole. Now we can guide the near-relativistic jet of neutron star material through a clever mass spectrometer arrangement to yield streams of pure elements. By tuning the beam, we can obtain any element we want. it becomes as easy to build a planet of gold as a planet of muck. And if you want a miniaturised personalised, private star — just assemble a moon of uranium and stand back!
Star-mining lets us build even bigger supramundane planets. Around ordinary stars we build multi-layered suprastellar planets (Fig 9.2). With some 10,000 layers the total area is around three billion Earths — that's for a G3 star like the Sun. Even larger are suprahole planets, powered by material falling into a black hole of a few solar masses up to galactic masses. There may be a 3 x 10 8 solar mass black hole at the centre of our own galaxy, which we could use as the underbody for planets 1014 times the size of the Earth. Even greater masses may be found in the core of cluster-dominant elliptical galaxies.
Eventually, in this sequence of ever larger supramundane planets, we come to Supraself (Fig 9.3), which has no underbody, for its gravity is generated by its own mass; each shell is dynamically supported within the gravity of the shells beneath. Supraself has a mass of about 2 x 10 12 solar-masses, as massive as the largest galaxies. The outer shell is about 1.2 light years in radius, and 14 square light years in area, which is quite a lot of land to find in one chunk. And of course that's only the first layer; there's another 30 million shells below that. The total habitat area is thus about 2 x 10 23 Earths. I guess even Americans, would take a fortnight or more to "do" Supraself!
At this size we have to be careful to avoid gravitational collapse, as some of the layers lie very close to their event horizons. Considerable space-time distortions occur around Supraself — it takes General Relativity to describe the geometry and analyse the physics. Thus time in the heart of Supraself is running 2500 times slower than in the universe at large, and even on the outer shell the stars in the sky are strongly blue-shifted.
Well, that's about the biggest planet in the current catalogue, and all I have for you today. Perhaps the next stage should be the Custom Universe, or, Move over Gods!
* * *
P.Birch of course!
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CUSTOM PLANETS OR MOVE OVER SLARTIBARTFAST!
PAUL BIRCH
48, Cliff Road, Cowes, IOW, P031 8BN.
Planets come naturally in a variety of unappealing forms and must be customised to clients' needs. This may involve modest landscape gardening (carving fjords, for instance) or simple climate change (using such obvious techniques as illumination from space by mirrors, shifting the planet's orbit or creating a nearby supernova). Sometimes a change of air may be required. Sometimes the starting material is so unpromising (such as gas-giants) that its easier to start over with a new surface a few thousand klicks up. Prompt delivery is essential.
The most popular models are ordinary terraformed planets or earthlike habitats, suitable for hunting lodges and retirement homes. But we can also cater for more exotic desires, like low-gravity worlds rented out as theme parks. Then there are ocean worlds, always popular with deep-sea fishermen. Desert worlds, for the sort of people who like desert worlds. And black hole planets for people who really want to get away from it all.
However, such bijou curiosities as diamond worlds (7.5 x 1028 carats) and planets of gold (1.5 x 1025 troy ounces) are only expected to become available (to the very rich and rather stupid) after the neutron star mines have reached full production.
1. INTRODUCTION
In this lecture we'll travel much further — and use more radical technologies — than in previous lectures. Even so, I see it as an extremely conservative approach to the future, drastically under estimating what we'll actually be able to do.
First we'll look at terraforming, asking what it is, why we should do it, how we can do it, and what other things we could do instead. You'll have heard most of this before, but from a different perspective; you'll find that I'm in marked disagreement with almost everybody else — especially over time scales and economics. We'll look at the rapid terraforming of planets like Mars and Venus, but since there aren't all that many suitable planets in the Solar System we'll also look at space habitats and artificial planets. Some of these will be far larger than any natural planet.
Other solar systems may contain terraformable planets too; we'll look at a selection of generic terraforming techniques, useably throughout the galaxy. Then we'll consider a possible scenario for the next few hundred years. Notice that I'm already talking about time scales very much smaller than most terraforming pundits would accept.
2. WHY TERRAFORM?
2.1 What is Terraforming?
Terraforming is the art of making new Earths or transforming hostile planets into life-bearing ones. There are several types. First, the unpronounceable ecopoesis. This means that only plants can live there, and a pretty dismal sort of terraforming it is too. Better is a habitable terraform which means that human beings can live there too. Best of all is a planetological terraform, which is stable over geological epochs. For the most part we'll be looking at habitable terraforms.
2.2 What are the Motives for Terraforming?
Motives for terraforming fall into a variety of categories, such as:
Ideological — By and large, advocates of ecopoesis are concerned with the preservation and dissemination of Life with a capital 'L', whereas those of us who spell it with a little 'l' are usually more interested in taming the universe for mankind.
Scientific — Scientists want to learn about planets and how planetary ecosystems can work. Experiments one would hardly risk doing on Earth can safely be carried out on other planets.
Economic — The economic approach considers terraforming in terms of industrial growth and capital accumulation – every new piece of real estate can be sold for profit; and every new habitat can develop its own economy and industry, adding further to the Gross Human Product.
Aesthetic — The aesthete looks at terraforming as a means of enhancing the human environment. It increases options. And terraformed worlds can be fun: fun to make, fun to live on, fun for films, fun for holidays.
Self-preservation — Terraformed worlds are safety nets: if another dinosaur-killer strikes the Earth, if war takes out the space colonies, or civilisation collapses, the human race will not become extinct.
2.3 What are the Terraforming Options?
Many terraforming scenarios take things very slowly, over thousands or millions of years. I don't believe humans have the patience for this. I haven't, anyhow. Furthermore, slow terraforming would be quite uneconomic. I am strongly of the opinion that any terraforming we do has to be done fast — preferably within a human lifetime.
Life-bombing is the "natural" way to terraform. This can mean something as simple as dropping a few bacteria, going away for a few billion years, and hoping that when you come back you'll find a pretty place — with a diverse earthlike ecosystem. Apart from being slow, it's not too likely to succeed, the more likely outcome is a planet of greenish, slime.
Bombing with a succession of tailored bacteria and plants, Followed by or interspersed with the introduction of carefully chosen animal species, may be more effective; however, it may be hard to maintain sufficient interest in the project over the centuries.
Alternatively, we can terraform "artificially" with high-tech methods, which are usually faster.
We won't take on the highest of high-tech in this lecture; that would involve nanotechnology, self-replicating systems or molecular copiers, and would let us do essentially anything we liked in about seven days! We won't be doing anything that fast today; instead we'll be taking from a few decades to a century.
2.4 What is the Competition?
In the future people will live in all kinds of habitat — both natural and artificial. Each will have to compete for inhabitants in terms of cost, availability, security, and quality of life. Terraformed planets will be only one option among many.
Naturally habitable planets have the disadvantage of being rare: so far we only know of one. It is doubtful whether there are more than a handful of planets in the galaxy on which a man could live without a space suit. Furthermore, extraterrestrial life forms, if they exist on these planets, may pose an unknown and potentially catastrophic threat.
When it comes to man-made habitats we find that, by planetary standards, rotating space colonies will mostly be rather small; they also come inside out. And although artificial planets can be very large, they may be considered less robust than a well-terraformed world.
To be economically viable a project may need to be completed (or at least begin generating adequate returns) within thirty years or less; otherwise the interest charges become astronomical. Hence any terraforming must be rapid.
3 ECONOMICS
My economic assumptions are as follows (Fig 3.1) . People will still be people; there will be no little green men no extraterrestrial, and no von Neumann machines or molecular copiers. If I'm wrong, all bets are off. I assume that existing trends, such as industrial growth and increasing personal wealth, will continue. For convenience, I use a population growth rate of 2.4% per annum, with an industrial growth rate of 4.8%.
The growth of industry and population is what makes terraforming and space colonisation possible. If you haven't the industry, you haven't the wherewithal to build extensive habitats; if you haven't enough people, you can't populate them. It works the other way round too — the construction of space habitats, and the terraforming of other worlds, will both encourage and enable further economic and population growth.
We can demonstrate long-term progress by means of empirical trend lines. Consider the human population in space since the start of the space age (Fig 3.2). Over the last thirty years it has increased at around 25% per annum. Even with the post-Apollo cutbacks it has continued to grow. At present rates, the population in space will exceed that of the Earth in less than a hundred years.
In the scenario used in this lecture the growth of space habitats soon outstrips growth on Earth (Fig 3.3); indeed, it is not long before the population of the Solar System is itself vastly exceeded by the population of the colonisation wave sweeping out through the galaxy.
In the earliest stages of space colonisation we have very small colonies, at very high population densities — perhaps as little as ten square metres of "land' per person. With time, however, habitats get bigger and population densities fall. By the time we get around to terraforming Venus, habitat areas are up around 100,000 m 2 per person (the same as the current figure for Earth). In the era of artificial planets and suprastellar habitats, even more room is available to the ever richer population.
It is hard to guess how long the demand for ever more extensive estates is likely to persist. I have assumed, quite arbitrarily, that demand levels off at 2500 km2 per person. This is only an average, of course; many estates will be very much larger yet.
4 LUNAR AND ASTEROIDAL SETTLEMENTS
The closest world beyond our own is the Moon. Unfortunately, it's not particularly good for colonisation. The sort of habitat we might build there is a sort of subsurface ellipsoidal cavern, artificially illuminated from within (Fig 4.1). Digging the hole is easy enough but finding enough nitrogen to fill it may be a problem; we may have to make do with imported nitrogen — as little as possible — eked out with oddments of helium, neon or argon.
On the Moon, the gravity is far too weak for earthlike habitats; whilst on the asteroids it is both too weak and inconveniently strong (it's easier to build rotating habitats in zero gee). The rotation periods are all wrong — nowhere near twenty-four hours — and surface temperatures are extreme. All in all, less than ideal for settlement.
However, both the Moon and the asteroids are excellent sources of raw materials. They can provide any amount of fused rock and soil for the construction of space habitats. They can be mined for metals like titanium and aluminium. There are carbonaceous asteroids rich in volatiles, and nickel-iron asteroids yielding not only an excellent steel but also gold and platinum by the billions of tonnes. Perhaps not enough to make the planet of gold, but it's early days yet!
5 RAPID TERRAFORMING
5.1 Mars
Even without terraforming, Mars is easy to colonise. In a way, that's a problem; the presence of colonists in their dome cities could prove a nuisance.
What do we have to do? First, warm the planet to ~290K, about the same as Earth. Second, increase the atmospheric density to 300 mbar or so, providing ~240 mbar of breathable oxygen Third find sufficient liquid water to fill the Martian seas.
We'd also like to increase the gravity to 1 g, but no one's worked out how to do that yet — not over the whole planet, anyhow!
Mars has abundant water and carbon dioxide, we think, but nitrogen seems to be under-supplied perhaps 100 mbars' worth in all, perhaps even less. We're not sure. One of the first things we need is a full geological survey of the planet. Till then, we're guessing.
If the planet turns out to be as short of nitrogen as some people think, we may be stuck with para-terraforming, which can get by with just enough to fill the space below the roof. Or we could import extra supplies from Venus or Titan — an expensive business on a planetary scale.
Otherwise, we have to make do with the nitrogen available and accept a lower atmospheric density than on Earth. It turns out that we don't actually need as much nitrogen as on Earth because low gravity is quite effective at damping down the spread of fire.
The strength of the convection currents feeding the fire is directly proportional to the gravity, so that 240 mbar of oxygen on Mars becomes equivalent to only 100 mbar on Earth. We're probably okay.
To terraform Mars we proceed as follows: —
First, we start warming the planet by means of a soletta, a rather complicated mirror positioned in space between Mars and the Sun (Fig 5.1). The sunlight comes in, bounces between tile slats and narrows down onto the planet. The soletta actually works like a condensing lens, but because it's only a thin aluminised film, like a solar sail, it's very light; even though the mirror is wider than the planet its mass is a modest 50 million tonnes. The soletta goes some 100,000 kilometres out from Mars — still within the planet's gravitational influence. The pressure of sunlight reflected from the annular mirror onto the back of the soletta is what stops it failing down.
Mars can thus be illuminated with sufficient sunlight to warm it to Earthlike conditions. Exactly how much sunlight it needs is not completely clear, but the value lies somewhere between 1.3 and 2 times the present insolation. We can play tricks with this by filtering out the stuff we don't need — the infrared and ultraviolet — and increasing the amount of visible light to compensate. This allows us to match (or even exceed) the intensity of visible light on Earth.
Unfortunately, simply warming the planet won't release enough volatiles. For one thing, it takes a million years or so for the heat to sink down through the deep crust. For another, a lot of the volatiles are locked up chemically in the regolith (we believe).
We're going to have to get drastic.
Let's nuke the place. Even better, lets burn holes in it (Fig 5.2). Sunlight, coming in from the magnifying soletta, converges onto another solar-sail lens. This aerial lens is very light and floats very high up in the Martian atmosphere — at a height of ~400 km.
It acts like a burning glass, concentrating all the sunlight that would otherwise fall over the whole planet down into a spot some 80 km across. The rock melts and vaporises. The rock-vapour flows away under the lens, condensing out to form glassy hills on either side of the melt. Volatiles — like oxygen, nitrogen, carbon dioxide and water vapour — are freed.
Now it is likely that when the ancient Martian seas disappeared they left behind evaporate deposits of nitrates and nitrites. Strongly heated, such deposits would release copious amounts of nitrogen and oxygen. If we can find pure nitrate deposits in sufficient quantity we should be able to make a breathable atmosphere in as little as ten years, which of course is jolly fast.
Naturally, we choose to melt out the regolith preferentially in those regions containing the best deposits.
Carbon dioxide is also released by regolith vaporisation (from carbonates) and photosynthesis can turn as much of this into extra oxygen as we need.
In the meantime, colonists and terraformers can live in dome cities: say, 1 km domes with a full Earth atmosphere pressure inside and the ambient Martian atmosphere outside (Fig 5-3). Because of the low gravity it is probably a good idea to have a few surface centrifuges (Fig 5.4); like space colonies rotating about a vertical axis, they provide a full Earth gravity towards the periphery of the habitat. That's the main problem with living on Mars: the low gravity may not be at all good for one's health. If nothing else, it won't make going to the toilet any easier (the Moon, of course, is even worse).
After terraforming we have a pretty-looking Mars with old-fashioned canals (Fig 5.5). Water drains from the uplands and the polar ice caps into the valleys, cascading through chains of broad lakes and sweeping falls into canals like narrow seas, and thence into the broad equatorial canal. Away from the canals lie the high deserts, the tablelands, the mountains.
In the handramits (the canal valleys, if you know your C. S. Lewis), the climate is pleasant — temperate or tropical according to latitude. Fertile lowlands, on either side of the deep water, give way to forest slopes and gaunt hills of glass. The harandra (the uplands, the old surface) is wild and lonely. Its climate is harsh and continental, arctic tundra to and desert; freezing by night, sweltering by day. Shallow seas in the old basins moderate these temperature extremes, producing a subtropical or Mediterranean climate.
Earthlike — and yet not like Earth — a world familiar enough to be pleasant and different enough to be interesting. The New Mars. Think of it as a planetary "Disney World".
5.2 Venus
For really living we want Venus.
Venus is practically a twin of the Earth. Or it could be, once we've cooled it down to 290K from its present molten-lead heat; removed the excess CO2 (it has around 100 atmospheres at present — and practically all of it must go); provided breathable oxygen, reduced the day to something like 24 hours (because the Venusian day lasts about 120 Earthly days — and that's a bit too long to stay out of bed, and provided upwards of 100 metres of water over the whole parched planet.
We could proceed as follows.
First we cool the planet with a sunshade (Fig 5.6), quite similar to the Mars soletta. It's a little more complicated than a simple shade — sunlight is deflected sideways just enough to miss the planet — but this way we eliminate most of the light pressure, making it easier to hold the shade in place with light from the annular support mirror.
At a later stage, when we want to occupy the planet, we can orbit another soletta in a 24-hour polar orbit; the sun will then appear in the sky 90 degrees away from its true position Venus is now in shadow and starts to cool down Unfortunately, because the atmosphere is so very think, it contains an enormous amount of heat and thus takes a long time to cool down — something like 200 years. Not so long to a planetologist, but to an engineer it's ridiculous. So we look for ways of speeding things up. There are several possibilities.
One way is to construct gigantic heat pipes connecting the hot dense lower atmosphere and the cool thin atmosphere around the 1 bar level (Fig 5.7). This keeps the upper atmosphere radiating as high a temperature as possible. Such heat pipes, although tens of kilometres high, are entirely feasible with fused rock construction. The way they work is this: at the bottom of the pipe the working fluid (water, to begin with) boils, flashing into steam through an expansion nozzle; at the top, the steam jet spreads out, cools and condenses; water drains back clown to the bottom and closes the loop. As the temperature falls, water is progressively replaced by ammonia. With heat pipes the cooling period can be cut to about 90 years.
Ninety years is still rather a long time, so recently I came up with a better scheme: heatballs (Fig -5.8).
Heatballs are hollow spheres containing a small amount of water. Down at the Venusian surface, they get hot: the water inside them evaporates. Now fling them up into space from the north pole. Out in space, they cool; the water recondenses. Wandering along magnetic field lines, they find their way back to the south pole and plunge towards the surface.
Guided now through evacuated conduits deep in the atmosphere back to the north pole, they heat up once more before swinging back out into space.
The heat balls are electrically charged, and follow magnetic field lines at orbital speeds without loss of kinetic energy. The required magnetic field can be generated by a pair of solenoids, one at either pole; the field strengths are quite small, so the amount of energy stored in the magnetic field is not enormous.
Because the heatballs can spread over a considerably wider expanse than that of the planet's surface alone, they can radiate from a much greater total area, and consequently radiate a correspondingly greater amount of heat. If the heatballs swing out to, say, three planetary radii cooling rates can thus be increased by a factor ~10, bringing cooling times down to as little as a decade,
The total mass of the heatballs is surprisingly low (equivalent to only ~16 mm of water over Venus) because the water (which has a high latent heat of vaporisation) is effectively reused every orbit, say every 10,000 seconds.
As Venus cools, carbon dioxide rains out of the atmosphere, forming oceans in the low-lying regions. I don't know whether dry ice is denser or lighter than the liquid CO2, so I'm not sure whether those oceans freeze over; however, any water ice will naturally float on top of the CO 2. Now because we don't really want oceans of liquid carbon dioxide we can cover them over with a floating platform of lightweight hollow blocks (Fig 5.9). The water ocean goes on top.
To get that water ocean we have to find some water. Where from? The icy moons of Saturn are the best bet — Enceladus, for example, could provide enough water to cover Venus to a depth of ~140m.
A steam-powered rocket drives the iceman out of its orbit, bouncing it off the gravity fields of other satellites, flinging it away from Saturn and into the inner Solar System. Eventually it approaches Venus, where we break it in half, one half swings round one side of Venus, the other half round the other (Fig 5.10). Now divide each half further into, say, 100 moonlets. These moonlets orbit the Sun with the same period as Venus; every half orbit then, that is, every 112 days, they return to the vicinity of Venus, where they collide, a pair at a time, just, short of the planet. Water vapour from the vaporised moonlets falls onto the planet and cools to become rain.
During icefall, it's a good idea to protect the surface from the heat and flash. We use a sky canopy, not unlike a para-terraforming roof, but a good deal thinner (we're not trying to hold in an atmosphere, just providing a sort of lightweight tent around the globe).
You can live on the surface during icefall; simply cover your colony with a transparent tent (Fig 5.1 1); the atmosphere inside is soon made breathable, but the pressure inside and outside is the same (this makes it much easier than para-terraforming on Mars). Enlarging the colony is easy; just make the tent bigger.
In the early stages of terraforming, the construction of aerial colonies (Fig 5.12), floating like enormous dirigible balloons high in Venus' atmosphere — at around the 1 bar level, where the temperature is not excessive — would enable us to move colonists in straight away providing useful economic returns early on.
After terraforming, we have a planet very like the Earth, with both land and seas, and a sun crossing the sky once every twenty-four hours. However because day and night is produced by an orbiting soletta, instead of by the planet's spin, the sun's path across the sky is peculiar Fig 5.13). This feature is likely to lead to climate patterns more even than on Earth; nowhere as persistently cold as the Arctic and Antarctic, nor as persistently hot as the equator.
5.3 Suitable Planets are Few
The snag is: there are only two readily terraformable planets in the Solar System — Mars, and Venus. We might be able to do something with oddments like Ganymede or Titan but even so, the potential of terraforming is limited to a total additional surface area less than twice that of the Earth. For more, we must turn to artificial planets, space colonies, or other solar systems.
6. SPACE COLONIES
Space colonies, indeed most forms of human habitat, will comprise (Fig 6.1):
The luminosphere provides the habitat with light and heat from the sun or some other source of energy. The atmosphere provides breathable air and is important in weather. The biosphere includes all life forms but not their non-living environment (in the literature, biosphere is sometimes given the wider meaning of an ecosystem). The geosphere is the landscaped surface of soil, rock and water, over a contoured base. The geosphere base is likely to be of a lightweight fractal honeycomb construction Below the base is the toposphere, supporting the whole habitat.
These are generic descriptions applicable to most forms of habitat, including natural planets like the Earth (where the geosphere is mostly solid rock, and the toposphere is the mantle and core).
6.1 Rotating Space Habitats
Suitable locations for space colonies include orbits around the Earth-Moon Lagrange points. Consider a large fat cylinder rotating on its axis (Fig 6.2); a landscape of seas, plains and mountains girdles it within, while sunlight, reflected from external mirrors, enters through the end caps.
The total mass of the habitat works out at around 40 tonnes per square metre of habitable land, more or less equally divided amongst atmosphere, crust, geosphere base and toposphere (Fig 6.3).
The geosphere base uses a low-density fractal architecture to keep the structural mass low, slotted together out of strong but readily available fractal blocks of fused rock (Fig 6.4). This is a constructional technique equally suitable for supramundane planets and rotating space habitats; it provides strength in tension as well as compression whereas normal masonry construction only has strength in compression.
The maximum size of conventional rotating space colonies is determined largely by the strength of available structural materials. The limit is about 250 km radius for quartz, 1000 km for sapphire, and 2500 km for diamond. That last case is actually pretty big, a colony equalling the land area of the Earth. Even so, most conventional space colonies will be considerably smaller than natural planets.
To some extent we can get around the size limit by making colonies longer, because the constraint is on the radius not the length. An extreme example is the macaroni habitat (Fig 6.5), an ultra-long habitat with a sunshine tube down the middle, if we loop it all the way round a star the total habitable area may be around 2000 times that of the Earth. And if we stretch a macaroni tube along tramlines between one star and another, the habitat area becomes something like 100 million Earths. There is sufficient material in the solar system to construct macaroni habitats thousands of light years long.
Even the largest diamond colony or the longest macaroni habitat is not a planet, though, because planets have horizons and you live on the outside, whereas space colonies have the outside on the inside!
6.2 Supramundane Habitats
Now we come to artificial planets.
A supramundane planet is a kind of ultimate space colony, an artificial planet with the outside properly on the outside, with natural horizons and natural weather, with night and day naturally chasing each other round the spinning globe.
A supramundane planet (Fig 6.6) is built around a massive heavenly body, such as a jovian planet. The habitable surface is supported dynamically above the underbody by orbital rings or dynamic compression members; the details of its landscaping, geosphere, geosphere base, biosphere and atmosphere are similar to those of other space habitats. It is illuminated from above with mirrors. Below is the toposphere (the support mechanism and orbital rings) in the otherwise empty space above the underbody.
Supporting the habitat with orbital rings avoids any requirement for ultra-strong materials: we no longer need to manufacture diamond in gigatonne lots.
The underbody could be a planet, a star, even a black hole; however, its gravity has to exceed 1 g because that's the gravity we want for the habitable surface. Then the area of the supramundane planet in Earth areas is simply equal to the underbody mass in Earth masses. The more mass you have the bigger your supramundane planet.
Rotating supramundane planets take up a shape like an oblate spheroid (Fig 6.7); a twenty-four hour period is easily provided for habitats above any size of underbody, up to the heaviest super-jovian on the verge of becoming a brown dwarf star.
A rotating supramundane planet is illuminated by means of a magnifying soletta (Fig 6.8), supported by the pressure of light from an annular support mirror, the rather complex shape is for stability. It turns out that wherever the planet is situated – even far- into interstellar space – it's possible to gather enough sunlight to enable earthlike conditions to be maintained.
Damage limitation is a bit of a problem (Fig 6.9). If someone sets off a nuclear explosion or drops an asteroid onto the habitat, we don't want the whole artificial planet collapsing on us. Observe how the support grid, even with a big chunk knocked out, of it, has to redistribute itself into a distorted grid that nevertheless continues to support the planet. This is probably the trickiest part of the whole affair: to make certain that the supramundane planet cannot possibly fall down under any limited number of failures.
There is enough energy in the system to vaporise the whole planet, so we must make absolutely sure it can't get loose.
We don't have to complete a supramundane planet in one go (Fig 6.10); we can start off with smaller units, such as a strip habitat in a ring around the planet, or a plate habitat at the junction of several strips. We then simply extend those strips sideways as we need. We don't have to find the money for the whole planet at once — only for the next habitat extension.
Where does the material for these artificial planets come from (Fig 6.11)? There's plenty in the underbody planets and their moons. We don't even have to spend any energy; with a bit of cunning we can carry mass simultaneously inwards from the moons and up from the planet, balancing both angular momentum and energy. Another possible source of material is the Sun (Fig 6.12), which could be mined using a ramscoop to collect gases from the stellar atmosphere and separate out the metals.
7. GENERIC TERRAFORMING TECHNIQUES
7.1 Extrasolar Planets
Well, that's more or less it for the Solar System. But are there planets in other solar systems? Probably there are. However, in all those billions of other solar systems there are probably very few genuinely habitable planets, planets where you could jump out of your ship without a space suit and start farming. Nevertheless, many extrasolar planets will be suitable for terraforming.
The most valuable planets will be like the Earth before life arose. Others will be like Mars or Venus. At the most, there may be a handful per solar system. Their combined areas will therefore be small compared to the potential habitable area of fabricated space colonies and supramundane planets. Nevertheless, such planets will have a not inconsiderable value as robust reservoirs of life; once created, a terraformed planet is much harder to knock out than a space habitat.
Our strategy should therefore be to terraform each planet quickly (so that settlers can move in), then proceed to a full planetological terraform over a longer period, so that the system becomes adequately stable without drastic maintenance over geological time.
7.2 Mirrors for Planetary Warming/Cooling
Among cheap and cheerful generic techniques, lightweight mirrors in space must take pride of place. With soletta mirrors it is easy to warm a planet, or cool it, or to adjust the temperature distribution across its surface almost any way we like.
On excessively hot worlds like Venus, temperatures can be moderated by means of a light-supported sunshade. This is practicable surprisingly close to the central star — even to within a few stellar radii. Thin atmospheres will cool quickly; thicker ones may call for heatpipes or heatballs to speed things up.
On icy worlds like Mars, temperatures can be raised by means of a magnifying soletta. This is practicable even to distances of about a third of a light year from the central star (depending upon stellar type). Indeed even in interstellar space, enough starlight could be collected to illuminate and warm an earthlike habitat or terraformed planet The thin atmospheres of such worlds will warm quickly.
A problem arises with low-gravity worlds, like Mars. the greater depth of their atmospheres enhances the greenhouse effect (water vapour, by the way, is by far the most important, greenhouse gas in the atmospheres of habitable planets), which tends to destabilise the climate. Icehouse and hothouse runaway may then only be avoided by active control of the insolation to maintain temperatures within the desired range. This degree of control of the soletta is not at all onerous; the requirement does however mean that the full planetological terraform may not be achieved.
7.3 Energy Intensive Engineering of Crust
Regoliths can take for ever to thaw, but with regolith vaporisation we can release volatiles and mould the surface topography quickly. Options for regolith vaporisation include the use of thermonuclear explosives, the impact of comets, the projection of pellet streams from space, or the focusing of sunlight by solettas and aerial lenses.
Since interstellar flight also demands powerful energy sources (such as relativistic pellet streams) the same energy sources are likely to be available to colonists for terraforming extrasolar planets on arrival.
7.4 Photosynthesis for Atmosphere Modification
Photosynthesis is clearly an integral feature of the ecosystems of habitable worlds, but in most terraforming scenarios is also used to generate a breathable atmosphere in the first place.
Initially, photosynthesis should be much faster than on Earth as higher levels of CO2 and an abundance of water, nitrates and other nutrients encourage rapid and efficient plant growth. An immature surface, without pervasive drainage channels, leads to extensive eutrophic lakes. The climate is controlled. There are few decay organisms or animals. Only the most productive strains of algae, grasses, reeds and other luxuriant species are employed.
All in all, photosynthesis can probably provide a breathable atmosphere in decades rather than millennia. Most people would probably disagree with me on that, and that is almost certainly because they are basing their ideas upon the natural ecology of the Earth. However, I would claim that terraforming is an engineering problem not a question of natural ecology. The quasi-equilibrium state of Earth has tittle in common with the purposeful, radical and rapid transformation of a planet during the process of terraforming.
7.5 Import/Export of Volatiles
The import and export of volatiles can be expensive in planetary quantities. Perhaps that can be turned to an advantage — volatiles can be traded. By exporting excess volatiles we don't need we can pay (both in money and energy) for the import of other volatiles — for example, swapping carbon dioxide or nitrogen for water.
Crashing comets — or moonlets of water or ammonia ice — onto planets to be terraformed is likely to be considerably cheaper. The supply is limited, but likely to prove adequate for the similarly limited number of terraformable planets.
If we consider the elemental abundances obtaining throughout the universe we see that adequate quantities of the elements needed for terraforming and habitat construction should be available in all parts of the galaxy. Some of these elements may not be in the best places — some we may have to seek in the stars themselves — but we can get at them; no overall shortages are to be expected. We must therefore conclude that the terraforming of extrasolar planets is indeed feasible.
7.6 Pellet Streams for Orbit Modification
It would obviously be tidier if we could shift each terraformed planet into a suitable stable orbit, where earthlike conditions could be obtained without having to mess around with solettas and sunshades.
Within our solar system Venus is too close to the Sun and too hot. We could move it out to the orbit of Earth in as little as thirty years, pushing off hard against the other planets (Fig 7.1). The near-relativistic pellet streams of the dynamic compression members generate enormous forces, even though their total mass is modest.
The energy required comes partly from light sail windmills round the Sun, but mainly from the orbital energy of the planets. There's a sort of free-lunch effect here: once we start pushing against, say, Mercury, orbital energy from Mercury's motion boosts the kinetic energy of the mass-streams; energy is then transferred into the orbital motion of Venus with high efficiency. Just pushing against the Sun (Fig 7.2) would be much less effective, because the angle through which the compression member acts would be very small.
Even if we decide not, to use this technique within our own solar system, it should certainly prove useful elsewhere. Its particular merit is that it enables full planetological terraforming to be achieved.
8. SCENARIO — FUTURE HISTORY 2000 - 2200 AD
[Note: written 1993 on assumption (not prediction) of projects' immediate commencement; add appropriate number of years for actual start date.]
2000 Space Hotel constructed in Low Earth Orbit. Soon caters for 100,000 people a week.
2010 First settlements on Mars. Surveys performed. Lunar City, Lunar mining. Colonies at L4 and L5.
2020 Terraforming of Mars begins. Construction of mirrors in Mars orbit. Asteroid mining. Cylindrical colonies at L5. First starship departs for a-Centauri.
2021 Mars soletta and aerial lens deployed Regolith vaporisation commences.
2022 Selected plant life distributed over Mars. Photosynthetic transformation of air begins.
2030 Little Switzerland built — radius 80 km. Missions to e-Eridani and other stars.
2040 Terraforming of Venus begin Heat pipes emplaced in Venusian atmosphere. PDL built — radius 160 km.
2050 First aerial colonies on Venus. Sunshade deployed Supra-uranian strip habitat commenced
2060 Carbon dioxide rain reaches Venusian surface. Archipelago built — radius 320 km. Suprajupiter strip habitat commenced
2070 Devolatilisation of Martian regolith completed. Suprasaturn strip habitat commenced Extrasolar habitats built by colonists.
2080 Terraforming of Mars completed Sapphire colony of radius 640 km. Rapid transit in-system at continuous one gee.
2100 First ground stations established on Venus. Lage scale mining of outer planets.
2130 First tent colonies established on Venus. Rupture of Enceladus commences. Diamondia built — radius 2560 km.
2160 Carbon dioxide oceans on Venus now covered. Sky-canopy deployed. Icefall commences. Photosynthesis of atmosphere proceeds Supra-Uranus is now 2000 km wide.
2190 End of Icefall. Canopies dismantled. Terraforming of Venus completed
>2200 Interstellar colonisation continues. Terraforming of extrasolar planets.
9. BLUE SKIES
That's more or less it for custom planets. Except for those planets of gold I mentioned.
Unfortunately, there's not enough gold in the asteroids, the cores of gas giants, or even the atmospheres of stars. To satisfy our lust we must seek out, the neutron stars, where mass transmutation of the elements goes on. Neutron stars are the philosophers' stone of the universe.
To mine a neutron star (Fig 9.1) we use the powerful magnetic fields of the star itself and an energy beam spearing down to the magnetic pole. Now we can guide the near-relativistic jet of neutron star material through a clever mass spectrometer arrangement to yield streams of pure elements. By tuning the beam, we can obtain any element we want. it becomes as easy to build a planet of gold as a planet of muck. And if you want a miniaturised personalised, private star — just assemble a moon of uranium and stand back!
Star-mining lets us build even bigger supramundane planets. Around ordinary stars we build multi-layered suprastellar planets (Fig 9.2). With some 10,000 layers the total area is around three billion Earths — that's for a G3 star like the Sun. Even larger are suprahole planets, powered by material falling into a black hole of a few solar masses up to galactic masses. There may be a 3 x 10 8 solar mass black hole at the centre of our own galaxy, which we could use as the underbody for planets 1014 times the size of the Earth. Even greater masses may be found in the core of cluster-dominant elliptical galaxies.
Eventually, in this sequence of ever larger supramundane planets, we come to Supraself (Fig 9.3), which has no underbody, for its gravity is generated by its own mass; each shell is dynamically supported within the gravity of the shells beneath. Supraself has a mass of about 2 x 10 12 solar-masses, as massive as the largest galaxies. The outer shell is about 1.2 light years in radius, and 14 square light years in area, which is quite a lot of land to find in one chunk. And of course that's only the first layer; there's another 30 million shells below that. The total habitat area is thus about 2 x 10 23 Earths. I guess even Americans, would take a fortnight or more to "do" Supraself!
At this size we have to be careful to avoid gravitational collapse, as some of the layers lie very close to their event horizons. Considerable space-time distortions occur around Supraself — it takes General Relativity to describe the geometry and analyse the physics. Thus time in the heart of Supraself is running 2500 times slower than in the universe at large, and even on the outer shell the stars in the sky are strongly blue-shifted.
Well, that's about the biggest planet in the current catalogue, and all I have for you today. Perhaps the next stage should be the Custom Universe, or, Move over Gods!
* * *
REFERENCES
D. Adams, "The Hitch Hiker's Guide to the Galaxy', Pan Books, London, 1979.
S. J. Adelman "Can Venus be Transformed into an Earth-like Planet?", JBIS, 35, 3-8 (1982).
14 M. Averner & R. D. MacElroy (eds.), "On the Habitability of Mars", NASA SP-414, Washington, (1976).
A. Berry, "The Next Ten Thousand Years", Coronet Books, Hodder and Stoughton, Bungay, Suffolk, (1976).
J. Billingham & W. Gilbreath (eds.), "Space Resources and Space Settlements", NASA SP-428, Washington, (1979).
P. Birch, "Orbital Ring Systems and Jacob's Ladders - I", JBIS, 35, 475-497 (1982).
P. Birch, "Orbital Ring Systems and Jacob's Ladders - II, JBIS, 36,115-128 (1983).
P. Birch, "Orbital Ring Systems and Jacob's Ladders - III", JBIS, 36, 231-238 (1983).
P. Birch "Dynamic Compression Members", JBIS, 42, 501-508 (1989).
P. Birch, "Supramundane Planets". JBIS, 44, 169-182 (1991).
P. Birch, "How to Spin a Planet", JBIS, 46, 311-313 (1993).
P. Birch, "How to Move a Planet", JBIS, 46, 314-316 (1993)
P. Birch, "Terraforming Venus Quickly", JBIS, 44, 157-167 (1991).
P- Birch, "Terraforming Mars Quickly", JBIS, 45, 331-340 (1992).
P. Birch "Can Population Grow Forever?", JBIS, 38, 99-105 (1985),
P. Birch, "Human Expansion into the Galaxy — Correspondence", JBIS, 35,142-143 (1982).
B.C. Clark, "Survival and Prosperity using Regolith Resources on Mars", JBIS, 42, 161-166 (1989).
H. Clement, "Mission of Gravity", VGSF, London, 1987 (Copyright Street and Smith Publications, 1953).
D. R. Criswell, "Solar System Industrialisation— Implications for Interstellar Migrations" in R. Finney & E. M. Jones (eds), 'Interstellar Migration and the Human Experience', University of California Press, Berkeley, (1985).
F. J. Dyson, "Terraforming Venus — Correspondence", JBIS, 42, 593 (1989).
F. J. Dyson, "The Search for Extraterrestrial Technology" in R. E. Marshak (ed), 'Perspectives in Modern Physics', Interscience Publishers, New York, (1966).
J. T. Early, "Space-based Solar Shield to Offset Greenhouse Effect", JBIS, 42, 567-569 (1989).
M. J. Fogg, "The Terraforming of Venus", JBIS, 40, 551-564 (1987).
M. J. Fogg, "Terraforming Venus — Correspondence", JBIS, 42, 593-596 (1989).
M. J. Fogg, "The Creation of an Artificial Dense Martian Atmosphere", JBIS, 42, 577-582 (1989).
R. A. Freitas, "Terraforming Mars and Venus using Machine Self-replicating Systems (SRS)", JBIS, 36, 139-142 (1983).
J. Grey (ed), "Space Manufacturing Facilities (Space Colonies)" Proc. Princeton/AIAA/NASA Conference, 1975, aiaa New York, (1977).
T. A. Heppenheimer, "Colonies in Space", Warner, New York, (1977).
C. S. Lewis, "Out of the Silent Planet", Bodley Head, London, (1938) & Pan Books, London, (1952).
J. E. Lovelock & M. Allaby, "The Greening of Mars", Warner, New York, (1984).
C. P. McKay, " Terraforming Mars", JBIS, 35, 427-433 (1982).
C. P. McKay, O. B. Toon & J. F. Kasting, "Making Mars Habitable", Nature, 352, 489-496 (1991).
C. P. McKay & C. R. Stoker, "The Early Environment and its Evolution on Mars", Rev Geophys., 27, 189-214 (1989).
C. P. McKay & S. S. Nedell, "Are there Carbonate Deposits in the Valles Marineris, Mars?", Icarus, 73, 142-148 (1988).
T R. Meyer & C. P McKay, "The Resources of Mars for Human Settlement", JBIS, 42, 147-160 (1989).
B. B. Mandelbrot, "The Fractal Geometry of Nature", W. H. Freeman, New York. (1982).
L. Niven "One Face" in 'Convergent Series', Orbit-Futura, London, (1980).
J. E. Oberg, "New Earths", NAL New York (1981).
G. K. O'Neill, "The High Frontier", Morrow, New York, (1977).
J. E. Pournelle, "The Big Rain" in 'A Step Further Out', Star Books, W. H. Allen, London, (1980).
C. Sagan, "The Planet Venus", Science, 133, 849-858 (1961).
C. Sagan " Planetary Engineering on Mars", Icarus, 20, 513-514 (1973).
J. L Simon "The Ultimate Resource", Princeton University Press, Princeton, (1981),
A. G. Smith " Transforming Venus by Induced Overturn", JBIS, 42, 571-57 6 (1989).
* * *
FIGURE CAPTIONS
Section 3
Fig. 3.1 Economics
Fig. 3.2 Population in space — doubling time is ~3 years and population growth rate ~25% per annum.
Fig. 3.3 Scenario predictions for population and habitat area.
Fig. 3.4 Lunar City/Base in subsurface cavern.
Section 5
Fig. 5.1 Mars Mirror system — Soletta Geometry and Light Paths (source "Terraforming Mars Quickly", JBIS, 45, 331-340 (1992) (fig.1))
Fig. 5.2 Aerial Mirror Lens and Regolith Melt (source "Terraforming Mars Quickly", JBIS, 45, 331-340 (1992) (fig.2))
Fig. 5.3 Domed City Colony on Mars (source "Terraforming Mars Quickly", JBIS, 45, 331-340 (1992) (fig.3))
Fig. 5.4 Surface Centrifuge within Domed City (source "Terraforming Mars Quickly", JBIS, 45, 331-340 (1992) (fig.4))
Fig. 5.5 Mars After Terraforming (source "Terraforming Mars Quickly", JBIS, 45, 331-340 (1992) (fig.5))
Fig. 5.6 Venus Mirror System (source "Terraforming Venus Quickly", JBIS, 44, 157-167 (1991) (fig.7))
Fig. 5.7 Cooling by Shading and the use of Heat-Pipes (source "Terraforming Venus Quickly", JBIS, 44, 157-167 (1991) ( combined figure from figs 1 & 2))
Fig. 5.8 Cooling Venus with Heat-Balls
Fig 5.9 Thermally Insulating for Carbon Dioxide Oceans (source "Terraforming Venus Quickly", JBIS, 44, 157-167 (1991) (fig.4))
Fig. 5.10 Ice-Moon Trajectories Near Venus (source "Terraforming Venus Quickly", JBIS, 44, 157-167 (1991) (fig.3))
Fig. 5.11 Colony on Venus after Cooling (source "Terraforming Venus Quickly", JBIS, 44, 157-167 (1991) (fig.5))
Fig 5.12 Two kinds of Floating Colony (source "Terraforming Venus Quickly", JBIS, 44, 157-167 (1991) (fig.6))
Fig. 5.13 Track of Reflected Sun Across Venus' Sky (source "Terraforming Venus Quickly", JBIS, 44, 157-167 (1991) (fig.8))
Section 6
Fig. 6.1 Parts of Habitat — Generic Descriptions
Fig. 6.2 Large Cylindrical Space Colony
Fig. 6.3 General Layout of Geosphere and the Provision of Landscaped Surface Relief (source "Supramundane Planets", JBIS, 44, 169-182 (1991) (fig.4))
Fig. 6.4 Fractal Architecture and Building Blocks (source "Supramundane Planets", JBIS, 44, 169-182 (1991) (fig.5(b) and (a) i.e. order reversed))
Fig. 6.5 Macaroni Habitats
Fig. 6.6 A Supramundane Planet (source "Supramundane Planets", JBIS, 44, 169-182 (1991) (fig.1))
Fig. 6.7 Geometry of Rotating Supramundane Planets (source "Supramundane Planets", JBIS, 44, 169-182 (1991) (fig.2))
Fig. 6.8 Illumination of Supramundane Planet (source "Supramundane Planets", JBIS, 44, 169-182 (1991) (fig.6))
Fig. 6.9 Damage Limitation (source "Supramundane Planets", JBIS, 44, 169-182 (1991) (fig.3))
Fig. 6.10 Construction and Extension of Supramundane Habitats (source "Supramundane Planets", JBIS, 44, 169-182 (1991) (fig.7))
Fig. 6.11 Mining Jovian Moons and Planets (source "Supramundane Planets", JBIS, 44, 169-182 (1991) (fig.8))
Fig. 6.12 Ramscoop for Mining Suns (source "Supramundane Planets", JBIS, 44, 169-182 (1991) (fig.9))
Section 7
Fig. 7.1 Transferring Angular Momentum to Other Planets (source "How to Move a Planet", JBIS, 46, 314-316 (1993) (fig.2))
Fig. 7.2 Moving Venus with Dynamic Compression Members (source "How to Move a Planet", JBIS, 46, 314-316 (1993) (fig.1))
Section 9
Fig. 9.1 Neutron Star Mining
Fig. 9.2 A Suprastellar Planet
Fig. 9.3 Supraself
the whole brilliant article.
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Why would you expect that to generate excess energy in this system when it doesn't generate excess energy when we do that in the lab?
We'll probably need fusion reactors just to get far enough out of the Solar System to build it, we'll also need the ability to take apart the planet Jupiter and use its material to build a Dyson shell. One problem with the Dyson shell is that it cannot hold its weight under the star's gravity, so one way to solve this problem is not to have a star in the center, we could just have a fusion reaction. Since we don't hve the weight of a star's material to compress the core to achieve fusion, we just achieve fusion through other means. 6.2*10^11 kg per second. The mass of Jupiter is 1.9*10^27 kg and Jupiter is mostly made of hydrogen. So this fusion reactor can run for 3,064,516,129,032,258 seconds or 97,175,168 years, not quite as long as the Sun, but 97 million years is quite a long time for humans, and there was talk of turning Jupiter into a star, but Jupiter doesn't have enough mass to be a natural star, it needs at least 80 times it mass to be a star, some have talked of dropping a mini-black hole into it, but it would not have a constant output if you did that. using it as fuel for a giant fusion reactor would seem to be the best solution. We could have the energy output of a second Sun for 97 million years. It would be helpful if there was another Jupiter further out from the sun, as we would want to minimize tidal forces.
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Indeed, in order to turn Jupiter into a star ( fusor ) one needs to increase its mass 13 times ( for brown dwarf ).
ORRRRR...
to increase deuterium concentration 13 times in it.
This could be done by self-replicating Neutron bombs exploding deep inside its thick Hydrogen masses and breeding more and more deuterium till it lits up.
---
About the fusion, indeed you do not need the gravity vs. pressure to be as much as with gravity confinement fusion. It is massively inefficient.
What you ( Tom ), depict is enormous intertial ( electrostatic ) reactor which reactor walls are habitat.
Why not!
I do not have idea about how deep the eletric charge well needs to be to fuse p-p, but why not ...
Though, one does not need at all such spheric configuration to achieve this effect. The reactor, hydrogen mining, habitat ( you posit it zero gee one ), is not necessary to be held together.
Electricity for running the ICRs may come from the electricity of Jupiter or other gas giant. The reactors could be in orbit and not necessary to be hermetically enclosed at all ... In best case scenario s.o. just tweeks the electric fluxes into a configuration where the p-p happens and to exploit the output of the hotspot.
Pinpoint nova.
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An enclosed sphere does contain all its output, and it will have the same output as the Sun, it will be good to be a safe distance away such as 1 au, You have about 1400 watts per square meter and about one billion times the surface area of the Earth, the problem with building it around the Sun is that I would collapse under the Sun's gravity as little as it is at 1 au, move it into interstellar space, and you have very little gravity, more precisely little difference of gravity. With it around the Sun all parts of it are pulled toward the Sun, in interstellar space its all pulled in the same direction by the Sun and so it is in free fall. There are other things such a sphere could do. It could generate a giant laser which could propel light sails to nearby stars. It could be a giant computer. Perhaps a series of inner spheres could absorb the gamma rays a reradiate it as visible light.
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Why not just build a supramundane shell around a Jovian, get the fuel from the underbody, and beam power to orbiting suns?
Use what is abundant and build to last
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If you want to generate the entire output of the Sun, You need something the size of a Dyson Sphere. Unlike the Sun, you eventually use all of the hydrogen of Jupiter and convert it to Helium. The Sun only fuses a fraction of its total hydrogen supply during its lifetime. Basically you are colliding proton beams and fusing them to Helium at the center of the shell! I suppose a target, say a ball of iron the size of the Moon might be a good idea. Fire proton beams at it and the collision will generate enough heat to cause fusion, the thing would output the energy of the Sun in the form of gamma rays. perhaps a series of inner shells would convert that to visible light by the time it reached the Dyson. We could have it just outside the Solar System in orbit around the Sun, perhaps at 100 au from the Sun does that sound far enough?
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Maybe a small quantum singularity would fit the bill. At small masses (a few million tonnes) these tend to evaporate very rapidly. It may be possible to keep the singularity in equilibrium, such that the rate of matter additional balances the rate of evaporation. Something like 90% of the matter injected would be converted into harvestable energy. If the singularity is surrounded by hydrogen, radiation pressure would effectively control the rate of new mass addition. The hydrogen envelope would also absorb the x-rays from the acretion disk, converting them into lower frequency light.
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Proton-Proton fusion seems sufficient but the cross section is very small. But imagine particle accelerators hurling protons at a target at the center of the Dyson Sphere. Use Deuterium-tritium fusion reactors to provide the initial power for these particle accelerators. Just need the output of the entire Sun for a few seconds, channel this into the particle accelerators. Or perhaps you can create a mini black hole at the center. Create a high enough density, and a black hole will form. On the other hand a high enough temperature might just melt matter into energy, this would be direct matter conversion, it requires very high temperatures though. It protons together hard enough and they turn to gamma rays, and the gamma rays precipitate out matter and antimatter particles, which then collide with each other and produce gamma rays. So matter + energy --> energy + energy, you end up with more energy than you started out with so long as the original energy is recovered efficiently enough.
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Alternatively, a solar sail stat lite could focus the light of a star onto a distance empty Dyson Shell with a hole on the side. Another mirror next to the Dyson focuses the incoming sunlight through the hole and a mirror in the center of the Dyson reflects the light onto the inner surface of the sphere. No fusion is required in this example, and the sphere is far enough away from the star so there is no worry about gravitational effects, its surfaces are in weightlessness.
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If you are going to do that, why not consider Proxima Centauri?
http://en.wikipedia.org/wiki/Proxima_Centauri
A nuclear reactor that will last?
The mixing of the fuel at Proxima Centauri's core through convection and the star's relatively low energy-production rate suggest that it will be a main-sequence star for another four trillion years,[18] or nearly 300 times the current age of the universe.[
That should be enough time for the human race
I suggest that as the star is variable and puts a lot of energy out in dangerous radiation and solar wind (I think) the "Sphere" should try to utilize those energy sources.
It is not ruled out that it may have objects in orbit around it.
Searches for companions orbiting Proxima Centauri have been unsuccessful, ruling out the presence of brown dwarfs and supermassive planets.[20][21] Precision radial velocity surveys have also ruled out the presence of super-Earths within the star's habitable zone.[22][nb 3] The detection of smaller objects will require the use of new instruments, such as the proposed James Webb Space Telescope.
I am not interested in habitable zone planets in this case. In order to retain a Nitrogen atmosphere on a planet around this star, the further away the better, up to the point of atmospheric collapse due to cold. But such a cold Earth/Venus/Mars/Titan may or may not exist.
Your idea might be suitable for this star to supplement the natural objects in orbit (If any). I would consider an incandescent method. Concentrate heat from the star on a point of the shell, where high temperature metals are used, and allow that to glow inside of the shell. The inside of the shell being a vacuum at that location. Perhaps a glass enclosure to reflect the heat wavelengths back to the glowing point, and to allow a spectrum closer to that of our sun. Then perhaps inside the rest of the shell, whatever is useful to the inhabitants whatever they become. If like humans, then greenhouses for plants?
Last edited by Void (2014-06-21 19:39:17)
I am starting to ask seriously "Why do I do this?"
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Actually more massive stars like Sirius would be better. A star's luminosity increases faster than its mass. One has to get fairly close to Proxima to be within the habitable zone, the solar sail statlite would have to be thinner and lighter in order to hold itself against the stronger gravity of Proxima. Sirius is brighter and not too much further away, an probably doesn't have habitable planets because of Sirius B. We could put reflecting statlite solar sails close in so its not as affected by the gravity of Sirius B and make a giant "search light" pointed at Sol Sin Since this is ordinary light it will spread with distance until it reaches the value of 1400 watts per square meter, and at that point, we place an Empty Dyson Sphere with a hole in its side to let in the light, probably something like the Island One Mirror geometry would work best, it doesn't actually rotate as its too big. For day and night we alternately open and close the holes.
Now imagine that this sphere is 2 au in diameter and only rotates slightly, not enough to centrifugal force to be noticible, so its a weightless environment. The rings in front and back are removed, and the north hemispheric end cap is removed so sunlight can shine directly on the South. Atmosphere is sandwiched between an inner transparent sphere and the outer sphere, providing a 50 km layer of breathable atmosphere in weightlessness. The further one moves away from the inner transparent sphere the more the starlight is filtered and the cooler it gets. Since their is little gravity the atmospheric pressure doesn't change much, you just get more water clouds between yourself and the light source, but you still get a lot of surface area, on the order of one billion Earths. The sphere is the default to get the maximum area for the minimum amount of building material.
And for 1 gravity areas the inner habitable surface of the Dyson shell can be dotted with open air Island One Spheres, each one 600 meters in diameter and spinning for 1 g at its equator, mounted on masts oriented toward the source of light within the Dyson.
Last edited by Tom Kalbfus (2014-06-22 11:02:31)
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Would building a Dyson sphere be worth it: We ran the numbers.
https://arstechnica.com/science/2023/03 … -a-planet/
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I think most star systems have insufficient material for a Dyson Sphere. But for fusion systems, the most important parameter for a sustainable reaction is confinement time. As plasma scales up, confinement time naturally increases. Whilst Earth based reactors are failing to reach breakeven at power levels of ~100MW, we don't need to scale to the power output of the sun to achieve a decent net energy return. In space, without gravity and with free vaccum, this should be easier.
"Plan and prepare for every possibility, and you will never act. It is nobler to have courage as we stumble into half the things we fear than to analyse every possible obstacle and begin nothing. Great things are achieved by embracing great dangers."
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For Calliban re #16
Your suggestion of building a small sun reminded me of Arthur C Clarke's vision of igniting Jupiter.
That seems to me like a poor use of a perfectly good planet.
What is the minimal mass your concept could use to achieve a sustained reaction?
Just because Nature shows one sure fire way to make a sun doesn't mean that's the ** only ** way to make a sun.
I'm a bit skeptical your vision could be achieved with mass much less than Jupiter, but you might well be on to something important.
(th)
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Follow up for Calliban .... This topic (your suggestion) reminds me of a hypothetical discussion I vaguely remember from a time long ago and far away .... a rod that extends out from a center point would tend to have a center of gravity where pressure might reach levels needed for fusion. Perhaps a hybrid system, combining magnetic fields and gravity might succeed in producing a useful fusion process without needing a Jupiter sized mass.
Mars_B4_Moon brought this ancient topic back into view. I'm hoping to find time to go look at the opening of the topic.
(th)
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Follow up for Calliban .... This topic (your suggestion) reminds me of a hypothetical discussion I vaguely remember from a time long ago and far away .... a rod that extends out from a center point would tend to have a center of gravity where pressure might reach levels needed for fusion. Perhaps a hybrid system, combining magnetic fields and gravity might succeed in producing a useful fusion process without needing a Jupiter sized mass.
Mars_B4_Moon brought this ancient topic back into view. I'm hoping to find time to go look at the opening of the topic.
(th)
For inertial confinement fusion, the Lawson Criterion for ignition can be expressed as:
Rho x R > 1gram/cm2
Where R is the compressed radius of a pellet and Rho is compressed density.
https://en.wikipedia.org/wiki/Lawson_criterion
So scaling up the system will definitely make ignition technically easier. On Earth, there are limits to the practical size of powerplants. Capital cost scales up as size increases. And a powerplant producing more than a few GW ends up dominating local grid capacity. But for a powerplant producing tens of GW of power, ignition would be technically much easier if we could afford the capital cost. There are other physics advantages to larger systems. Although not captured within the triple product formula, neutron heating will add more energy to the system at large scales.
I have often wondered about using a very large fusion reactor as the power source for synthetic fuel production. In this situation, scaling down would be less important, because liquid fuels can be shipped out to any customer on Earth. So a power output of 10GW or even 100GW could be fully utilized without any grid compatibility problems. We could even have a hybrid arrangement, with say 10GW going into the grid and 90GW going into a fuel synthesis plant.
Last edited by Calliban (2023-03-29 01:59:39)
"Plan and prepare for every possibility, and you will never act. It is nobler to have courage as we stumble into half the things we fear than to analyse every possible obstacle and begin nothing. Great things are achieved by embracing great dangers."
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For Calliban re discussion of large scale fusion ....
I found a reference yesterday that showed that the minimal mass required for ignition of fusion using gravity is far above the mass of Jupiter.
The Apache Internal error blocked my attempt to post the snippet. I even changed to a completely different browers and opened an entirely new logon session, but the result was the same.
Apache has once again blocked the snippet ... this is getting to be mildly annoying.
For SpaceNut ... the error occurred a 8:25 local time, so the UTC value would have been 12:25.
I sure hope you gain access to the Apache Error Log soon!
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Retry:
While my post #18 appears to have inspired addition thinking about large scale traditional fusion designs, I am hoping to pull you back (at least for a moment) to consider gravity as a confinement system. Gravity is by far the best confinement system for fusion. Atoms held in a gravity field cannot escape except by fusing to release photons which ** can ** escape. At present, (to the best of my knowledge) humans are unable to create gravity fields of any kind. All humans can do (again, as far as I know) is to assemble matter and let Nature take charge of producing gravity.
I'll try the quote again:
quote omitted
The problem with a fusion reactor of this size is that it will ONLY produce photons as useful output, but if the mass were in the form of a small object of some kind (not a black hole of course) then the photons produced could be captured and converted to useful forms of power.
The quote above does not include information about Jupiter and Saturn, but they are both much smaller than .08 solar mass.
To achieve a mass of .08 solar equivalent in a small volume would be quite a feat, but it would certainly be handy as a power source. All that would be needed would be a steady supply of hydrogen, and it should keep producing photons.
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I'll try the quote again:
Mass Needed to Create a Star - The Physics Factbook - hypertextbook
hypertextbook.com › facts › KellyMaurelus
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Now I'll try the single line that appears to be causing the Apache Server error...
Both theory and observations concur in defining a minimum protostellar mass for the ignition of the hydrogen fusion to be around 0.08 solar mass.
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For Calliban (now that the battle with Apache is over) ...
The only way (to my knowledge) that humans can currently achieve a mass equivalent of .08 solar is by gathering that much matter and enlisting Nature to take care of the details.
However, gravity is thought by some to involve curvature of space.
In your post about Inertial Confinement Fusion, it seems to me that you may be thinking about the thought (by some) that acceleration is equivalent to gravity.
Inertial Confinement Fusion (as currently practiced, and again as far as I know) involves momentary acceleration (deceleration in this case) which produces conditions equivalent to .08 Solar Mass for a brief period of time.
A Real Universe mass of .08 Solar equivalent has the distinct advantage of stability with respect to the outside. Conditions inside such a mass are necessarily chaotic, but at least the mass is able to hold itself together for a period of time. Conditions can occur (I understand) that make such a mass unstable, but perhaps if humans have created such a mass in the first place, they can maintain favorable conditions for successful operation for an extended period.
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For SpaceNut .... just for the heck of it, I'm going to paste the offending snippet again, and this time I'm going to perform the Submit at a precise time.
I have Time.is/UTC running nearby, so I'll be able to set the time of the Submit with precision. Time was UtC 12:45:00
Mass Needed to Create a Star - The Physics Factbook - hypertextbook
hypertextbook.com › facts › KellyMaurelus
Both theory and observations concur in defining a minimum protostellar mass for the ignition of the hydrogen fusion to be around 0.08 solar mass.
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