Return-path: X-Andrew-Authenticated-as: 7997;andrew.cmu.edu;Ted Anderson Received: from beak.andrew.cmu.edu via trymail for +dist+/afs/andrew.cmu.edu/usr11/tm2b/space/space.dl@andrew.cmu.edu (->+dist+/afs/andrew.cmu.edu/usr11/tm2b/space/space.dl) (->ota+space.digests) ID ; Tue, 7 Nov 89 04:25:22 -0500 (EST) Message-ID: Reply-To: space+@Andrew.CMU.EDU From: space-request+@Andrew.CMU.EDU To: space+@Andrew.CMU.EDU Date: Tue, 7 Nov 89 04:25:03 -0500 (EST) Subject: SPACE Digest V10 #218 SPACE Digest Volume 10 : Issue 218 Today's Topics: Jupiter Balloon data ---------------------------------------------------------------------- Date: 7 Nov 89 08:29:24 GMT From: agate!typhoon.Berkeley.EDU!gwh@ucbvax.Berkeley.EDU (George William Herbert) Subject: Jupiter Balloon data This is the promised Jupiter Balloon data. Please treat this all as an unpublished manuscript for a scientific proposal or paper. Frank and I are finishing calculations and intend to publish and would be upset if someone stole it all :) The proposed balloon is simple in concept. Using a nuclear heat source, probably a small reactor, as a pure heat source, we propose to manufacture a hot-hydrogen balloon for long term scientific probing into the jovian atmosphere. Our assumed balloon used a thin double wall envelope of somewhat (about 50%) thinner walls than current materials. With a insulative gap of hydrogen to minimize heat loss. The SP-100 reactor was taken as standard for the project. Stripping it of all but it's core and heat transfer equipment lowers its weight to a little less than a ton. It gives a pure heat output of about 2 megawatts (extrapolated from published data). Given that the maximum heat useage is where the loss equals the output, we derived a formula for surface area versus interior temperature, and the corresponding bouyancy for a given radius. Our test case (off quick calculations) was a fourty meter radius balloon. It gave a estimated 15 tons lift, allowing for errors and some fudge factor (all conservative). With a reactor weight of one ton, and a envelope at around three tons (perhaps more like five to six being conservative) and necessary structure, we got a useful load of four to eight tons. This is not the optomization point for the design, either. Making the balloon larger and lowering internal temp. raises the bouyancy a lot. A seventy meter radius balloon would have closer to thirty tons lift. It should be obvious that the limit is not the liftable weight but the weight we can toss to Jupiter. Including an ablative shell, the above balloons are truly massive. Getting them to jupiter is more of a hassle than making them work, IMHO. -george william herbert [this article and the abstract preceding it are copyright frank crary and george william herbert. we ask that you not publish it or use it as the basis for a published article. feel free to show the idea around, though. you heard it here first!] ------------------------------ End of SPACE Digest V10 #218 *******************