Subject: Space-tech Digest #136

Contents:

   Fuel-rich mixtures and specific impulse (7 msgs)
   Deep search for asteroids (2 msgs)
   Reactors banned in NEO? (4 msgs)

------------------------------------------------------------

Subject: Re: P2-E pressurization via propellant heat transfer 
Date: Mon, 16 Nov 1992 19:15:05 EST
From: John F Carr <jfc@grouse.dsg.dec.com>

> BTW, it looks like the mole fraction of hydrogen or helium that would
> dissolve in propane at 298 K and 7.5 MPa are about 6% and 3%,
> respectively.

What affect would dissolved He have on Isp?  The molecular weight of
the exhaust would be lower, but the temperature would also be lower.

------------------------------

From: henry@zoo.toronto.edu
Date: Tue, 17 Nov 92 14:10:48 EST
To: space-tech@cs.cmu.edu
Subject: Re: P2-E pressurization via propellant heat transfer 

>What affect would dissolved He have on Isp?  The molecular weight of
>the exhaust would be lower, but the temperature would also be lower.

No general answer can be made without calculation.  Such effects are
often beneficial, in moderation.  Almost all fuel/oxidizer combinations
yield optimum exhaust velocity (i.e. Isp) when run fuel-rich, for this
very reason -- a small loss in temperature is more than compensated for
by the drop in exhaust molecular weight.  (Note that it's usually the
decomposition products of the fuel, not the fuel itself, that appear
in the exhaust, so this works even with high-MW fuels like kerosene.)
The effect is particularly marked when hydrogen is involved, given its
very low MW.

I wouldn't be at all surprised if a bit of helium helps performance
noticeably.  However, it's unlikely to be cost-effective, given the cost
and scarcity of helium.  (One reason why I would hesitate to rely much
on helium is that the US government controls the major sources of it,
so it implies yet another set of bureaucrats who can shut you down.)

                                         Henry Spencer at U of Toronto Zoology
                                          henry@zoo.toronto.edu   utzoo!henry

------------------------------

Date: Tue, 17 Nov 92 20:09:45 EST
From: John Roberts <roberts@cmr.ncsl.nist.gov>
Disclaimer: Opinions expressed are those of the sender
	and do not reflect NIST policy or agreement.
To: space-tech@cs.cmu.edu
Subject: Fuel-rich mixtures and specific impulse

>>What affect would dissolved He have on Isp?  The molecular weight of
>>the exhaust would be lower, but the temperature would also be lower.
>No general answer can be made without calculation.  Such effects are
>often beneficial, in moderation....

[Followup to a very old post to sci.space]

I would very much like to see these calculations. I've tried to calculate
it in several different ways for hydrogen-oxygen mixtures, and it invariably
comes out that you gain in specific impulse but lose on total impulse if
you replace some of your onboard oxygen with an equal mass of hydrogen.

The first time I calculated this, I treated the exhaust as a hydrogen-water
mixture moving at a uniform velocity. The second time, I used the specific
impulse of the two gases, calculated the extent to which each would be
heated, and treated the exhaust velocities of the two as independent.
(I did use the simplifying assumption that all of the energy of combustion
goes into velocity of the exhaust. I don't know whether the extent to which
this departs from reality causes a problem, but I've seen Paul Dietz use this
assumption in his calculations, so if that invalidates the results, you can
blame Paul. :-)

In both cases, the effective specific impulse (by which I mean impulse per
unit of oxygen burned) turned out greater than that of a stoichiometric(?) 
mixture. However, there's also less oxygen to burn, which offsets the
improved Isp to some extent. Expressing it as a formula to show total
impulse as a function of the amount of oxygen replaced with hydrogen,
in both cases I came up with the result that the greatest total impulse
is achieved when *none* of the oxygen is replaced (in other words, the
stoichiometric mix gives the greatest total impulse).

As I said before, if there are more sophisticated calculations which show
that this is not really the case (and ideally show what the optimum mix
really is), I would really appreciate seeing them.

(Books on rocket propulsion are in somewhat limited supply here, but I
haven't found anything which would disprove my calculations.)

If there is some reason that the oxygen tank is required to be spherical,
so that (for instance) the chosen diameter of the Shuttle external tank
limits the amount of oxygen that can be brought along, but the length of
the hydrogen tank is not constrained, then I agree that making the hydrogen
tank a little bigger and bringing along a little extra hydrogen can improve
the total impulse. (And of course it prevents the engines from burning up.)
But if oxygen tank shape and engine erosion are not constraints, you would
do better to add hydrogen *plus* a corresponding amount of oxygen.

As Clint Eastwood would say, go ahead - prove me wrong! (But please show
the math. :-)

John Roberts
roberts@cmr.ncsl.nist.gov

------------------------------

Date: Tue, 17 Nov 92 21:21:35 -0500
From: dietz@cs.rochester.edu
To: roberts@cmr.ncsl.nist.gov
Subject: Re:  Fuel-rich mixtures and specific impulse
Cc: space-tech@cs.cmu.edu

John,

  To see what's going on here, let's look at the thermodynamics
of the situation.

  Inside the rocket's combustion chamber is a higher pressure, high
temperature mix of chemicals.  Because it is at high temperature, the
gas is not, in general, composed only of the lowest energy mix of
components (water, for example, in the case of hydrogen + oxygen).
Instead, it also contains H2 and O2, hydroxyl radicals, atomic
hydrogen and oxygen, and so on.

  As the gas expands out the nozzle, it cools.  Some of the energetic
components react to form more stable molecules.  This releases energy,
which retards the cooling of the gases.  The more the gas expands, the
cooler it gets, and the more of this latent energy that is converted
to kinetic energy.

  In a real rocket, the gases are still hot or have not fully reacted
by the time they leave the nozzle.  This reduces performance over the
theoretical upper bound.

  Stoichiometric hydrogen/oxygen would produce a very hot gas, with a
lot of energy going into dissociating molecules.  If you add some
extra hydrogen, this reduces the temperature so that more of the
latent energy becomes available.  As it turns out, in real engines the
extra energy (and lower average molecular weight) improves Isp, up to a
point.  Just how much depends on the pressure ratio of the engine.

	Paul F. Dietz
	dietz@cs.rochester.edu

------------------------------

From: henry@zoo.toronto.edu
Date: Tue, 17 Nov 92 22:50:41 EST
To: space-tech@cs.cmu.edu
Subject: Re: Fuel-rich mixtures and specific impulse

>... several different ways for hydrogen-oxygen mixtures, and it invariably
>comes out that you gain in specific impulse but lose on total impulse if
>you replace some of your onboard oxygen with an equal mass of hydrogen.

I have difficulty understanding how that could happen.  Specific impulse
is impulse per weight of propellant.  If you keep weight constant and
improve specific impulse, how can you lose total impulse?!?  Something
is fundamentally wrong with any calculation producing that result!

Sutton (Rocket Propulsion Elements) outlines the process in chapter 6
(Chemical Rocket Propellant Performance Analysis):

Determine initial combustion-product composition, given known pressure,
pre-combustion composition, and thermodynamic properties.  That is, find
the product composition that minimizes Gibbs free energy.  This assumes
complete combustion to equilibrium, but that's usually a good assumption;
experimentally-determined combustion efficiencies are 94-99%.  Gibbs free
energy is
		G = sum for j=1 to n of (mu sub j * n sub j)

where n sub j is percentage of molecules of substance j and mu sub j is
free energy for substance j:
		mu sub j = U + pV - TS

where S is entropy, U is internal energy, and typically you look this
up in a table as a function of temperature for the relevant substance,
and then correct for pressure.  Don't forget intermediate products;
Sutton's example for RP-1/LOX shows not just CO2, H2O, and H2, but also
CO, OH, H, O, and O2.

Then expand isentropically to the nozzle exit-plane pressure, making some
kind of assumption about reaction rates during expansion.  "Frozen"
expansion assumes a reaction rate of zero so the initial composition
is unaltered; "shifting" expansion assumes infinite reaction rates so
the gas is in equilibrium at every point (note the possibility that
components with high boiling points will condense into liquid or solid).
Anything intermediate is inordinately hard to handle because little is
known about reaction rates under such conditions.  Real results usually
fall between the frozen and shifting cases, which typically aren't too
far apart.  I seem to recall that one reasonably-good heuristic is to
assume shifting flow to the nozzle throat and frozen thereafter.

Conservation of entropy now gives you the exit temperature.  From that
and known gas properties we get enthalpy (thermal energy) change, and
from that and conservation of energy we get kinetic energy content at
the exit plane.  Hence, finally, average exhaust velocity and specific
impulse.

No analytic shortcuts for all this are apparent.  You have to grind through
it with computerized assistance and lots of tables of thermodynamic
properties of gases.  It's something I have not done myself, so I can't
comment knowledgeably on difficulties.

The typical result is 3-12% overoptimistic, much of which is probably
nozzle losses of various kinds.

>If there is some reason that the oxygen tank is required to be spherical,

Nope, and in fact it isn't, quite.  The lower end is more or less
hemispherical, but the upper end forms the nose of the External Tank.
It's closer to a sphere than to a cylinder, but not very spherical.

                                         Henry Spencer at U of Toronto Zoology
                                          henry@zoo.toronto.edu   utzoo!henry

------------------------------

Date: Wed, 18 Nov 92 00:46:53 EST
From: John Roberts <roberts@cmr.ncsl.nist.gov>
Disclaimer: Opinions expressed are those of the sender
	and do not reflect NIST policy or agreement.
To: space-tech@cs.cmu.edu
Subject: Re: Specific impulse

>I have difficulty understanding how that could happen.  Specific impulse
>is impulse per weight of propellant.  If you keep weight constant and
>improve specific impulse, how can you lose total impulse?!?  Something
>is fundamentally wrong with any calculation producing that result!

Sorry - it's been a long time since I did the calculations, and I worded
it badly. Does this sound any better: given the initial assumptions I used
(now shown to be somewhat shaky!), and assuming the same rate of oxygen 
consumption as for a stoichiometric-mix rocket with equal combined mass
of hydrogen and oxygen, it is indeed true that exhaust velocity and mass
flow are greater in the hydrogen-rich rocket, but since the total amount
of oxygen brought along is less, the rocket fires for a shorter period of
time, and my calculations work out that the total impulse (thrust multiplied
by time of firing) is less for the hydrogen-rich rocket. (That's still not
very precise, but hopefully it's a little better.)

>Sutton (Rocket Propulsion Elements) outlines the process in chapter 6
>(Chemical Rocket Propellant Performance Analysis):

I'll try again to see if I can find that book.

Thanks to you and Paul for your replies. If I understand them correctly,
the main problem with my calculations is that the initial assumption of
100% conversion of thermal energy to useful kinetic energy within the
rocket engine is not valid, due in large part to the finite length of
the rocket nozzle, so other factors such as the chemical properties of
the exhaust components at various temperatures become predominant. (Is 
that about right?)

Would it be reasonably safe to assume that if for some reason a rocket
engine in space were made with an extremely long nozzle, then the
specific-impulse advantage of a hydrogen-rich rocket would become
less pronounced?

John Roberts
roberts@cmr.ncsl.nist.gov

------------------------------

From: John F Carr <jfc@grouse.dsg.dec.com>
Subject: Re: Fuel-rich mixtures and specific impulse 
Date: Wed, 18 Nov 1992 11:29:31 EST

> No analytic shortcuts for all this are apparent.  You have to grind through
> it with computerized assistance and lots of tables of thermodynamic
> properties of gases.  It's something I have not done myself, so I can't
> comment knowledgeably on difficulties.

I did some such calculations when I took MIT's rocket propulsion course.  I
don't remember it being very hard, but we only worked with very simple cases
(hydrogen + oxygen).  I wouldn't want to try computing the exhaust velocity
of a hydrocarbon burning engine without a computer and a good program.

I remember the instructor telling us that many of the reaction rates and
thermodynamic properties of intermediate products of hydrocarbon burning
were unknown.

------------------------------

To: space-tech@cs.cmu.edu
Subject: Deep search
From: can2can@ziggys.cts.com (Tim Edwards)
Date: Sun, 15 Nov 92 08:37:10 PST

A radar situated at each of the trojan points would give us a good chance
of seeing around the Earth and Moon, and not missing anything in this
vicinity.  A chirp-radar sends a long pulse, that is frequency modulated,
then uses the frequency modulation of the echo to time compress it. The
result is a good 'power in the pulse to peak power handled' factor, 
combined with exelent resolution in range.  A phased array antenna alows
the signal beam to be aimed without physical movement of the array.
The pahased array antennas that I am familliar with involve a _lot_ of
slotted wave guides, piped into the circuitry. If the dimensions are
adjusted for the dielectric constant, we should be able to have the tubes
built as solid, with a core of pyroceramic so there is never a question
of leakage/contamination, then a layer of whatever metal is availible,
and a{glass finish to slow the evaporation of the metal.  Raw materials
to be lunar, we know where the lunar resources are without needing
the radar first to track planetesimals.  The radars will give us a lead
to the resources of the planetesimals, which seem to be quite different
from lunar resources.

              can2can@ziggys.cts.com - BBS (619)262-6384
                 Ziggy's Den Of Iniquity 

------------------------------

Date: Mon, 16 Nov 92 15:09:06 +0000
From: Dominic Herity <dherity@zinfandel>
Subject: Re: Deep search

> A radar situated at each of the trojan points would give us a good chance
> of seeing around the Earth and Moon...

I feel as if I walked into a room in the middle of a converstaion.
Maybe I did. Apologies in advance if these points have been covered.

I gather the reason for the radars is to detect near earth asteroids.

What kind of range are we talking about? To get 24 hours warning of something
coming at a relative speed of 50km/s, you'd need to see it at 4.3 million km.
Anything less wouldn't be much use, I guess. 24 hours wouldn't be any use
either unless you had a response pretty well rehearsed. :-)
200 times that range would catch almost everything inside Jupiter's orbit,
which gives enough time to figure out a response after detection.

Why not put the radars on Earth ? It would be much cheaper. Since the earth
rotates every 24 hours and shorter notice isn't much use, nothing  relevent
is going to hide behind it. Since the moon travels its own diameter every
33 minutes, so nothing will hide behind that either. The only way I can
imagine a dinosaur killer hiding is by coming straight out of the sun.

Best Regards
Dominic Herity

------------------------------

Date: 17 Nov 1992 16:27:30 -0500 (EST)
From: "GORDON D. PUSCH" <PUSCHG@crl.aecl.ca>
Subject: Reactors banned in NEO?

Henry Spencer <henry@zoo.toronto.edu> writes:
> Nuclear power might be the right technical solution but it has 
> obvious political problems at present...  

I vaguely remember that at one point there was talk of getting reactors
*banned* inside of Mars's orbit in general, and within the Earth's Van-Allens 
in particular. (Gamma-ray astronomers were particularly keen on this --- 
the weak-decay positrons from the unshielded reactors aboard Soviet ``Cosmos''
satelites remained trapped in the Van Allen belt, and were ``polluting'' the
electron-positron annihilation line when they struck gamma-ray observatory-
satelitess.) 

1) Is there currently an international agreement banning reactors from 
   near-earth orbit? (maybe I should really post this to sci.apace, sorry!)

2) Given that most reactors in orbit are unlikely to have more than "shadow-
   shielding," do trapped reactor-produced positrons in the Van-Allens pose 
   a hazard to anything other than gamma-astronomer's careers? Anybody know
   what the typical lifetime of a Van-Allen electron is? (It should put an 
   upper bound on the positron lifetime.)

Gordon D. Pusch  <puschg@crl.aecl.ca>

------------------------------

Date: 17 Nov 1992 17:17:38 -0500 (EST)
From: "GORDON D. PUSCH" <PUSCHG@crl.aecl.ca>
Subject: P.S. to "Reactors banned in NEO?"

Before anybody fires back the "Space is *BIG*. Really, *really* *BIG*" line
from _Hitchhiker's_: the positrons tend to remain trapped on the flux-tube
they were emitted onto. Since the magnetosphere more-or-less corotes w/ the 
earth at low lattitudes, that means a reactor in near-circular orbit tends 
to fill a thin shell w/ positrons (and electrons) --- except at GEO, where 
it just fills the flux-tube it's on (modulo effects due to misalignment of
magnetic- and spin-poles, and deformation and convection of the magnetosphere 
plasma due to solar-wind pressure). Such trapped positrons really *do* exist
and are observable; I read a paper about them in _Nature_ a few years ago.

Gordon D. PUsch  <puschg@crl.aecl.ca>

------------------------------

Subject: Re: Reactors banned in NEO? 
Date: Tue, 17 Nov 92 14:50:55 -0800
From: gwh@lurnix.COM

There are no agreements about reactors anywhere.
For a long time, the Russians were putting up radar
ocean recon sats that were nuclear reactor powered
and in LEO; one fell on Canada a while back, you
might recall, after it's reactor jettison system
(designed to put the reactor in high, stable orbit)
failed.

There has been no serious talk of banning reactors
from near the earth.  Nuclear propulsion is universally
disliked for near-earth applications, but transfer vehicles
and anything going further out are fine.  Nuclear reactors
are not affected.  Physicists may not like it, but they're
not running the whole space program (thankfully 8-).

Nuclear bombs are banned, in any form, in space.
The test ban treaty saw to that.  Which theoretically
nails down any "Orion" vehicles... 8-) As if anyone
would build one unless they were desperate enough to
violate a treaty anyway.  Which is likely scienci fiction
not space-tech 8-)

-george

------------------------------

Date: 18 Nov 1992 11:38:04 -0500 (EST)
From: "GORDON D. PUSCH" <PUSCHG@crl.aecl.ca>
Subject: Re:  P.S. to "Reactors banned in NEO?"

Samuel J. Pullara <avenger@wpi.WPI.EDU> writes:
> I think he meant: How long does a positron last before it is annihilated
> by an electron in the Van Allen Belts?

No, I meant what I said; I'd have to work it out to be sure, but my gut
feel is that the Van-Allen electron density (and therefore the annihilation 
rate) is so small that the positron will get scattered into the loss-cone 
long before it annihilates --- that's why I said it would put an *UPPER*
bound on the lifetime, which annihilation will reduce somewhat.

Gordon D. Pusch  <puschg@crl.aecl.ca>

------------------------------

End of Space-tech Digest #136
*******************
