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Science fiction concepts |
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| Mar17-06, 11:48 PM | #1 |
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Science fiction concepts
In case the name didn't give it away, I like science fiction. A while ago (more than a year ago) I decided to look into space combat from a scientific standpoint. After spending huge amounts of time procrastinating from real work by looking up laser efficiencies, theoretical maximums for focusing particle beams, physical constants for a number of potential armor materials, and so on, I find that there are things about the physics that Google simply won't tell me. So I'm hoping some of you might be able to help me with these questions. (I'll probably have more, too - this is just the list I came up with now.)
Some of these answers might be complicated - I think I can handle it, if you are all nice and use small words. I am a PhD student, but in zoology. I've had a brush or two with physics, science is no stranger, but my territory is the ecology of grasshoppers, not something even remotely related to the subjects I'm asking questions about. Anyway, thanks in advance for the help. 1) How does one compute acceleration per meter of barrel length for a railgun or coil (gauss) gun (also called a mass driver)? Clearly, each additional meter of length gains you less acceleration, since it has less time to act on the projectile. Equally clearly, higher velocities give you a greater chance of hitting a maneuvering target. And, of course, at a certain point the barrel length just gets ridiculous, even for a zero-drag environment. Before someone points out the obvious, I know that railguns and gauss guns are really different beasts - I'm looking for an equation for each. 2) What is a plasma mirror? Something I read suggested that a plasma mirror reflects any light below the mirror’s frequency. What does this mean? Is it true? If so, can a plasma mirror withstand intense blasts (weapons-grade pulsed lasers, for instance)? (And is a plasma mirror related to a "plasma window"?) 3) How do you calculate the speed at which a gas or plasma expands? For instance, if you lose containment on your spacecraft’s fusion reactor, how do you calculate how rapidly the no longer contained plasma takes to expand? 4) I assume there must be a way to take known physical properties of a material (density, possibly distance between nuclei and bond strength as well) and calculate how well it stops particle and EM radiation (of, obviously, known characteristics, since x-rays and hypervelocity charged particles have separate characteristics). How does one do that? 5) To keep things all about the plasma, a question about beam spread. If you are busy letting plasma blast out of an electromagnetic bottle, either to provide propulsion, or to burn your enemies to cinders, how does one calculate beam spread? For a particle beam, I’d look at particle velocity from heat, time to target, and calculate how far off the beam axis a particle could wander from thermal issues in that time. But for a plasma beam, the thermal velocity is the (potentially insanely high) velocity of the “bolt” itself. A well-designed mag bottle should be coming as close to possible to forcing every last ionized particle to fly out along the beam axis, with no wandering. 6) Is there any way to take a known set of shapes with known mass colliding at a known velocity and determine from that information the impulse of the collision? 7) There’s a design out for a magnetic sail spacecraft that is supposed to be shoved around by a beam of plasma shot from elsewhere. I’m aware of the basic interactions of charged particles and magnetic fields, but in this case something is puzzling me. Does the sail stop the beam? Initially, I assumed the beam would “splash” against the sail, electrons going one way, ions going (slightly less readily) another. Then I did some calculations (which, I am sure, were awful for numerous reasons) that suggested that no reasonable field could exert the forces to cause that much charge separation, and that the charge separation would keep the beam together, and let it barrel on through the sail. So what really happens? |
| Mar18-06, 12:30 AM | #2 |
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1. Have you taken high school physics yet? That's just the distance equation with f=ma in it: d=1/2 (f/m)t^2. Solve for time and plug back in to find velocity.
2. Sounds like technobabble. 3. Static pressure and Bernoulli's equation (convert static pressure to velocity pressure). 4. Not sure - density is a key though. 5. For a particle stream, there should be little or no dispersion. 6. Mass vs spring constant - shape isn't all that important. 7. Not sure. |
| Mar18-06, 12:48 AM | #3 |
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Ok, let me rephrase the question - what are the forces involved? For the gauss gun I'd need to know the force on a ferromagnet in a given magnetic field, and I can't find that anywhere. My bad on that - I should have phrased the question correctly the first time. I've tried to vet concepts pretty thoroughly - I'm not going to ask about gravity lances, FTL drives, or force fields, because those are just silly. I have, however, run across concepts in the literature that people seem to just assume their readers understand. Thanks for the other info. I'll look up Bernoulli's equation tomorrow. |
| Mar18-06, 01:11 AM | #4 |
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Science fiction concepts |
| Mar18-06, 04:04 AM | #5 |
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I don't think plasma mirrors exist, possibly under a different name. There is no such thing as weapons-grade pulsed lasers either, don't try and apply sci-fi too much to reality. ![]() |
| Mar18-06, 10:52 AM | #6 |
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ovoleg - thanks for the link.
Anyone know what it is for a gauss gun? I've gathered that they are actually better, but harder to build. That whole "no rails to explode outward and corrode with every shot" thing. And there's always the old designs for the "porcupine bomb" nuclear bomb pumped x-ray laser cluster (http://en.wikipedia.org/wiki/Laser_applications, which includes mentions of several laser weapon projects). Now, maybe radiating and absorbing radiation are linked nicely, but if so, I missed it, and I beg your indulgence. If you've got some calculations on the inefficiencies, I'd love to see them. I've been keeping reams of calculations in an Excel spreadsheet to compare various ideas given certain baselines. Imagine both systems as tubes of bouncing ping-pong balls. A particle beam blasts air down the tube, hurling all the ping-pong balls out. Some of them may have been bouncing in a direction perpendicular to the tube axis - they will exit with that velocity intact, and move off the "beam" axis. A plasma beam just lets some of the balls bounce out. To do this, though, they have to have fairly specific velocities (direction-wise), or they won't make it out of the tube. I'd expect different beam spreads because of this. Maybe I'm wrong - but if you could explain away my logic, I'd be convinced I was. |
| Mar18-06, 10:57 AM | #7 |
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Ok..since everyone seems to think that plasma mirrors are something I got out of a sci fi book, let me provide a link to technical article about using plasma mirrors to reflect high-intensity lasers.
http://www.clf.rl.ac.uk/Reports/2001-2002/pdf/92.pdf That's the phenomenon I want explained. |
| Mar18-06, 12:19 PM | #8 |
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With regards to the "magnetic sail". I've heard of people designing sails which are then pushed by a laser beam, but not plasma... where did you see this?
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| Mar18-06, 12:45 PM | #9 |
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I've already posted this link http://www.newscientist.com/article.ns?id=dn6543 but maybe it isn't working for you. The bottom of this Wikipedia article discusses using a particle beam to push a mag sail. http://en.wikipedia.org/wiki/Magnetic_sail More on the plasma beam end of things. http://www.ess.washington.edu/Space/magbeam/ And one last link. http://www.iee.org/OnComms/Circuit/b...etic_beams.cfm |
| Mar18-06, 07:46 PM | #10 |
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![]() Radiation coming from nuclear reactors is different from solar flares' radiations and electromagnetic radiation. You would need some sort of dense, highly reflecting material, because if it absorbed all the radiation it would probably end-up heating-up a bit. I don't know what to use. I can't think of anything available nowadays. Unless of course you were thinking of armoring for the spaceship, then you could probably used some very dense material like depleted uranium to absorb it all. Because you're out in space, excess heat can radiate off without worrying about somebody wearing it getting burned. Assuming you got a great thermal insulator such as aerogel. Cool links. I'll read them all.
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| Mar18-06, 10:27 PM | #11 |
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Of course, what I really want to understand is how plasma changes from reflecting to absorbing to transmitting. Sounds like there's great potential to deal with incoming EM radiation, but without knowing the physics, it's hard to guess what might be realistic. I think fullerenes look like the best armor in terms of deflecting kinetic weapons and dealing with the thermal effects of energy weapons. However, what I really want are some calculations. One of the issues is with particle beams - unlike most lasers, they dump their energy across a path into the armor, not on the surface. This means that, for certain beams and armor thicknesses, much of the beam energy will strike PAST the armor layer. Some calculations on beam penetration would help me establish whether you need 1 km of armor (in which case, forget it, particle beams are just killers) or 3 cm. I expect that high-frequency lasers (x-ray, for instance) may also penetrate armor some distance without having to blow through it. I also suspect that neutronium would make nice rad shielding, but I'm trying to stay within reasonable realism limits. |
| Mar18-06, 11:01 PM | #12 |
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Plasma mirror here: http://www.nrl.navy.mil/pao/pressRel...=1996&R=35-96r
Sounds like it's just a plasma tv screen on top of the emitter, enabling beam control by varying to opacity. |
| Mar18-06, 11:23 PM | #13 |
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| Mar19-06, 05:10 PM | #14 |
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Recognitions:
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I don't think the opacity is varying per se.
I believe the situation is that a plasma will reflect waves of low frequency, and transmit waves of high frequency. The frequency at which this transition occurs (reflection vs transmission) depends on the characteristics of the plasma - essentially it's electron density. Thus our ionosphere reflects radio waves, but transmits light. A denser plasma will thus reflect light as well as radio waves, which is apparently what the laser people are taking advantage of. See for instance: http://image.gsfc.nasa.gov/poetry/ask/a10013.html I think the technical term for this frequency is "plasma frequency", but I'm really not positive. You might also try talking about this topic on rec.arts.sf.science (that's a usenet newsgroup). |
| Mar19-06, 10:49 PM | #15 |
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Does each pixel have its own chamber, or is it just a big one? http://www.oz.net/~coilgun/mark1/spread2.htm http://www.oz.net/~coilgun/mark1/spread3.htm http://mgc314.home.comcast.net/velocity.htm |
| Mar20-06, 07:07 PM | #16 |
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Looks like the data on the frequency here will let me backtrack to figuring out what that is in real (and engineering) terms. Incidentally, there's no way of actually generating gravity, right? Aside, of course, from bringing a lot of mass along with you. Still, looks like these are the equations I need, once I sort through the specifics to find the generalities. |
| Mar22-06, 10:42 PM | #17 |
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