Path: utzoo!utgpu!jarvis.csri.toronto.edu!mailrus!ames!haven!uvaarpa!mcnc!thorin!lhotse!symon From: symon@lhotse.cs.unc.edu (James Symon) Newsgroups: sci.space Subject: Re: Sanger Message-ID: <7284@thorin.cs.unc.edu> Date: 16 Mar 89 15:36:24 GMT References: <1989Mar14.172237.29235@cs.rochester.edu <7234@thorin.cs.unc.edu> <78@enuxha.eas.asu.edu> Sender: news@thorin.cs.unc.edu Lines: 23 In article <78@enuxha.eas.asu.edu>, kluksdah@enuxha.eas.asu.edu (Norman C. Kluksdahl) writes: > I have done some back-of-the-envelope calculations to check out the > advantages of speed at release of the orbital vehicle. (Note: these > are only rough calculations, intended only to demonstrate a point). > > In all cases, it is assumed that the payload is released at an altitude > sufficiently large to neglect most air frictional effects. . . . You don't mention the mass ratio for standing start at sea level (considered common knowledge I suppose, but I'm just a voyeur) but your numbers suggest to my envelope-back that the benefits of added speed at launch probably don't warrant the investment in a Mach 5 launch vehicle. > . . . Still, air launch does promise something--I read that OSC's > Pegasus gains about 15% in usable payload by air launch at Mach 0.8. And that's still down in pretty thick air, isn't it? So how about Mach 0.0 at 125,000 ft. under a set of monster balloons? jim symon@cs.unc.edu {decvax uunet}!mcnc!unc!symon