[ExI] Physical limits of electromagnetic launchers
Anders Sandberg
anders at aleph.se
Sat Jun 2 20:46:44 UTC 2012
On 02/06/2012 15:39, Keith Henson wrote:
> I have seen arguments that more than a small fraction of c gets into
> abrasion problems. Out between galaxies this may be less of a problem
Would love to get some proper numbers on this. I have heard the
arguments, but not seen any proper calculations.
I suspect a series of Whipple-shields in front of the vehicle can fix a
lot of the abrasion problem.
> If you do want to consider power, then I need the mass of the probe
> objects. Small enough, bacteria size, electrostatic works better than
> magnetic acceleration.
In our case the standard probe payload mass is about 30 grams, if I
remember right. We also have an extreme case of 500 tons, but that is
not something we take very seriously.
> If I recall correctly, lasers are good out to a light year, and since
> they can levitate objects on earth, they can accelerate at 1 g or
> better. I think that's 0.1 c.
Yes, a lot of laser propulsion systems could be done in this scenario. A
Dyson shell is pretty good phased array.
> The problem is slowing down at the target. Of course there is
> Drexler's method for that but it does take foresight.
Which one was that? Eric suggested a moving railgun that fired the
payload backwards, possibly even repeating in order to seed along its
line of travel. In our model we assume the payload to be a small rocket
(fission, fusion or preferably antimatter), although for intergalactic
colonisation over long distances the expansion of the universe can be
used to shed velocity!
> A nice fresh G type star can make it from one galaxy to the next using
> a hemisphere of light sails to convert the star into a fusion-photon
> drive. But you have to be really patient.
It is nice when you have plenty of luggage.
--
Anders Sandberg,
Future of Humanity Institute
Philosophy Faculty of Oxford University
More information about the extropy-chat
mailing list