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- Newsgroups: sci.space
- Path: sparky!uunet!utcsri!helios.physics.utoronto.ca!neufeld
- From: neufeld@helios.physics.utoronto.ca (Christopher Neufeld)
- Subject: Re: Solar sailing
- Message-ID: <By6HCp.Gw0@helios.physics.utoronto.ca>
- Sender: news@helios.physics.utoronto.ca (News Administrator)
- Organization: University of Toronto Physics/Astronomy/CITA
- References: <By32vF.GD6.1@cs.cmu.edu>
- Distribution: sci
- Date: Mon, 23 Nov 1992 16:48:24 GMT
- Lines: 46
-
- In article <By32vF.GD6.1@cs.cmu.edu> roberts@cmr.ncsl.nist.gov (John Roberts) writes:
- >
- >Most proposed solar sails are reflective, not black. That's because the
- >principles of conservation of momentum show that reflecting the beam of
- >light can greatly increase the thrust of the sail. The best results
- >are with a 100% reflective sail perpendicular to the beam of light (theta = 0);
- >that doubles the thrust.
- >
- Well, yes, for certain definitions of 'best results'. Unless your
- sail+payload has a very low mean mass per unit area, though, the net
- force on the sail is still going to be sunward. Since the solar pressure
- falls off as the square of distance just the way gravity does, the effect
- of setting the sail at normal incidence to the sun is the same (from a
- mathematical point of view) as instantaneously reducing the mass of the
- sun while maintaining the position and velocity of the spacecraft fixed
- over that instant. The result is a new orbit which circumscribes the old
- one and is tangent to it at the point where the sail was unfurled. This
- new orbit, of course, is closed, like any bounded orbit in an inverse
- square field. Now, for some trajectories this is desirable, but for most
- it probably will not do.
- The usual trick is to set the sail at an angle to the spacecraft-sun
- line. Since the radial component of the thrust does no net work over one
- complete orbit (to first order, it helps a bit to second order if the
- sail is not at normal incidence), the sail should be set at an angle to
- maximize the tangential thrust. This angle is about 35 degrees for a
- perfectly reflecting, planar sail. The sail can be angled to thrust along
- the velocity vector or against it, and the orbital energy of the sail can
- be raised or lowered this way, allowing the sail to move sunward just as
- easily as it moves outward.
- A higher generation sail might be designed with a collector area at
- normal incidence to the sun but which focusses the light onto a small
- secondary reflector which can be steered rapidly to new directions. The
- sail can be smaller for a given thrust. There will be some weight and
- design penalties on making the reflector (which has to handle a very high
- power flux) and making a sail which can focus accurately onto the second
- reflector.
-
- >John Roberts
- >roberts@cmr.ncsl.nist.gov
-
-
- --
- Christopher Neufeld....Just a graduate student | Don't let your mind
- neufeld@helios.physics.utoronto.ca Ad astra | wander -- it's too little
- utzoo.utoronto.ca!generic!cneufeld | to be let out alone.
- "Don't edit reality for the sake of simplicity" |
-