All items considered here are vertically-launched. The depressed trajectories flown by
horizontally-launched designs are completely different, and cannot be analyzed in this way at all. See Figure 1 (all figures at end) for the
assumed trajectory shape, and associated
bounding analysis assumptions.
I personally think reusability will “cost” the extra weight
to make the structure robust enough to fly multiple times. Otherwise,
from a rocket propulsion standpoint,
the typical rocket performance levels available to us are:
LOX-RP1……………………305-310 sec Isp
LOX-liquid-CH4…………near 350 sec Isp
LOX-LH2……………………near 460 sec Isp
1972-vintage NERVA…near 900 sec Isp
Note that NERVA is a solid core nuclear device.
I did this as a parametric bounding analysis, based on the simple rocket equation and some
convenient simplifications to support it.
The supporting calculations are summarized in Figure 2. I looked at inert structural fractions from
5% to 40% (in increments of 5%) as the independent variable, with required Isp as the dependent
variable. The parameter was payload
fractions from 2 to 10%, in increments
of 4%.
I did not look at ramjet-assist or any other type of
airbreather-assisted vertical launch.
The analysis required to support usable trade studies with airbreathers
goes well beyond this kind of rocket equation-based bounding analysis.
The basic results are presented in Figure 3 as parametric
curves. Required Isp (as the ordinate)
to accomplish a launch mission that effectively requires 8.56 km/s delta-vee, is plotted versus inert structural fraction as
the abscissa. The parameter is imposed
dead-head “payload” fraction from 2% to 10% by 4% increments.
Linear interpolation between payload fractions is clearly
permissible. Horizontal lines have been
added to represent the available Isp levels,
as described above for the four “realistic” types of rocket propulsion
listed above.
“Dead head” payload includes the real delivered payload, plus any shroud or capsule weight, as appropriate. The structural inert weight includes basic
tankage or airframe structures, plus
engines, plus any recovery equipment or propellants
that might be required.
One-Shot One-Stage
Rockets
For one-shot single-stage rocket boosters, the inert structural fractions can resemble
those of currently-flying vehicles,
two-stage or otherwise. Those range
from 5 to 10%, and are probably closer
to 5% in new designs today, at least
with dense propellants that are not “extreme” cryogenics. With that range of inerts “spotted” on the
graph, Figure 4 gives the trade study results.
The LOX-LH2 propellant choice gives the “best” results throughout
the 5-10% inerts range, provided that the
propellant volumes can be reconciled with a 5% drag loss. One might “guess” about a 7% dead-head
payload allowance, that might reconcile fairly
well with perhaps 7% inerts (very voluminous LH2 tankage with extra insulation).
Vehicles like that can carry large payload masses inside a
fairly-lightweight shroud (say near 1% of launch weight, leaving the remainder of the “dead head
payload” fraction as real payload delivered to orbit). Or,
they might carry smaller payloads inside one-way or returnable
capsules, such as Orbital’s Cygnus or
Spacex’s Dragon, respectively. For the sake of argument, assume 80% of a one-way capsule’s weight
might be real payload, and 60% of a
returnable capsule’s weight might be real payload.
For that 7% deadhead payload LOX-LH2 sizeout, if shrouded,
then about 6% of the launch weight might be real delivered payload. If instead a one-way capsule, then again about 5.6% of the launch weight
might be real delivered payload. If
instead a returnable capsule, then about
4.2% of the launch weight might be real delivered payload.
LOX-RP1 is just barely infeasible as shown in Figure 4, but 5% inerts and 4% dead-head payload is
feasible with LOX-CH4. If shrouded, then perhaps 3% of the launch weight might be
real deliverable payload. If a one-way
capsule, then about 3.2% of the launch
weight might be real deliverable payload.
If a returnable capsule, then
about 2.4% of the launch weight might be real deliverable payload.
For something comparable to a Falcon-9, the launch weight would be in the
neighborhood of 500 metric tons. The
launch price would be near $56.5M.
(Falcon-9 lists as $4300/delivered kg.)
Using these values and the percentages in the preceding paragraphs, I get:
Propellant…………….inerts%............deadhead%
LOX-LH2……………….7…………………….7
Type…………………….deliv%...............$/del.kg
Shroud…………………6……………………..1880
1-way capsule………5.6………………….2020
Returnable cap…….4.2………………….2690
Propellant…………….inerts%.............deadhead%
LOX-CH4……………….5…………………….4
Type……………………..deliv%..............$/del.kg
Shroud………………….4…………………….3770
1-way capsule……….3.2…………………3530
Returnable cap……..2.4………………….4710
Any of the LOX-LH2 configurations would then seem to offer
slight cost advantages per unit delivered payload, over the LOX-RP1 two-stage-to-orbit (TSTO)
baseline Falcon-9. (This baseline is
based on Spacex website data as of 9-24-13.)
The LOX-CH4 data are less advantageous than LOX-LH2, because of the lower Isp performance. The shroud and 1-way capsule versions seem to
offer very slight advantages over the Falcon-9 baseline, but the returnable capsule seems to be a
little less cost-effective.
Really, at this level
of analysis, all the LOX-CH4 data are
effectively the same unit price as baseline,
and the LOX-LH2 only very slightly better than baseline. This looks attractive only for a
clean-sheet-of-paper LOX-LH2 design.
Otherwise, the LOX-RP1 TSTO
baseline that we have is better.
Re-Usable One-Stage
Rockets
This is a “screwy” case.
It all boils down to what one believes that the realistic effective
inert weight fractions might be.
The trade study results are given in Figure 5, on which I have spotted the roughly 10% inert
fraction of Space Shuttle SRB’s, which
are 900-psi pressure vessels, being
solid motor cases, yet of limited demonstrated
reusability.
My own guess for the inert fractions of fully-reusable
liquid stages is closer to the 15-25% range also spotted on the figure. This “budget” includes not just the tankage
and engines, but also all the necessary
recovery equipment (such as chutes and landing legs), plus a considerable amount of retro-thrust
propellants (if a powered descent is the approach taken, as in Spacex’s “Grasshopper”).
This might actually be a “low-ball” estimate, since entry is so demanding an
environment. But it doesn’t really
matter. The curves show basic
infeasibility for all three chemical rocket choices, with the possible exception of LOX-LH2 at
only 1% “dead-head” payload. Such a
payload would have to ride the booster “naked”,
as there is no allowance available for a shroud. No capsule options seem feasible.
That leaves you only with the nuclear rocket option
“NERVA”, which at 20% inerts could
probably carry 13-14% dead-head” payload.
Actually, considering the
relatively low engine thrust/weight for NERVA-type engines, we’d be lucky to obtain 35% inerts at 2%
dead-head” payload. That would be
about a 1% real delivered payload fraction,
inside a shroud, as the only
feasible option. That’s 5 metric tons
delivered, at the “same $56.5M”
price, for about $11,000/delivered
kg. That’s not very attractive.
But, in any
event, to be re-usable means you
are flying
back to Earth an already-fired nuclear reactor engine, and you are doing this multiple times. There are some very serious safety
concerns with such an approach. I
really don’t recommend this for Earth surface launch.
The bottom line is that a re-usable SSTO booster is
technically attainable with nuclear rocket propulsion, but nobody will like the safety risks. I did not look at re-usable first stages
for a chemical TSTO system. That
is what Spacex is really looking at.
Re-Usable One-Stage
Rocket Spaceplanes
Winged rocket spaceplanes that launch by vertical takeoff
(VTO) as SSTO, but return to horizontal
landing (HL) have been a longstanding dream.
Again, the
driving assumption is what you believe a realistic inert weight fraction might
be.
Being a winged airframe,
this is the vehicle that most closely resembles an airplane as we have
known them for over a century. Most modern
transports and bombers fall in the 40-50% inert weight fraction range, with carrier-capable Navy “birds” pushing 60%
inerts. That would be for traditional
metal construction. Airframes like that
are usually designed for 40,000+ landings and takeoffs.
You cannot replace all of the metal structures with
composite materials. These are very
intolerant of heat. Not only orbital
descent, but also ascent, are rather vicious aeroheating
environments. But, the number of landings and takeoffs might be
in the 100-1000 range, which eases
somewhat the robustness (and inert weight) required of the design.
A “reasonable guess” might be half composites and half
metallic, for a minimum-credible
reusable inert weight fraction in the range of 25 to 30%. Accordingly,
I showed inert fractions from 25 to 40% on the trade study results given
in Figure 6.
All the chemical options are quite clearly infeasible. Only a nuclear spaceplane powered by some
version of a NERVA (or better) would be feasible. This brings up (again) all the safety
concerns of flying back to Earth with a fired nuclear reactor core, as discussed above for reusable rocket stage boosters.
Allowing for the low engine thrust/weight ratio of
NERVA, we might achieve 35% inerts at 2%
payload fraction. No shroud or capsule
is required, so the delivered payload is
2%. That’s 10 metric tons for a 500 ton
launch weight. Again, assume the same launch cost of $56.5M for the
500 ton nuke, and you get around
$5700/delivered kg. It does not seem to
offer any cost advantage over what we are doing right now: the Falcon-9 one-shot TSTO calculates as $4300/delivered
kg.
Options Not Considered
Here
I have not looked at airbreather-assist for VTO SSTO, or any depressed-trajectory SSTO and TSTO
systems (whether airbreather-assisted or not).
(I have actually looked at the latter,
but not in a way that I trust yet.)
The airbreathers, particularly
ramjet, require substantially-more
sophisticated performance-estimation methods than the simple rocket-equation
stuff presented here. Those are destined
for a future article.
Final Comments
One-shot VTO SSTO rocket-stage systems seem to be marginally
attractive (relative to a one-shot LOX-RP1 VTO TSTO baseline) from a delivered
payload unit cost standpoint, but only
if a LOX-LH2 system is considered in a clean-sheet-of-paper design. LOX-CH4 seems to offer no real
improvement, and one-shot LOX-RP1 VTO
SSTO seems to be essentially technologically infeasible.
Re-usable VTO SSTO rocket-stage systems appear to be
completely infeasible for all known chemical propulsion choices, relative to the one-shot LOX-RP1 VTO TSTO
baseline. A NERVA-type nuclear approach
appears to be technically feasible, but
at lower payload fraction due to the low engine thrust/weight inherent with
solid core nuclear engines. Assuming the
same basic launch cost for the same launch weight class, the unit price for delivered payload appears
to be more expensive, relative to the
one-shot VTO TSTO LOX-RP1 baseline.
Figure 2 – Basic Calculations and Related Conditions
Figure 4 – Basic Results for One-Shot One-Stage Rocket Launchers
Update 9-29-13:
For those not so familiar with rocket work, these plots can be a little confusing or misleading. First: these are for single-stage operations only. You cannot use these directly for staged vehicles. Nor can you do anything useful with these plots toward airbreathing-assist, it's just too coarse for that, although concepts can be illustrated.
For airbreathing-assist, you have to "account" for highly-variable airbreather Isp effects, how much of the thrust is airbreather, and what fraction of the whole trajectory is actually assisted by the airbreather. You also have to worry about having enough thrust to take off, and that these charts embody only vertical takeoff on a fast ascent trajectory.
Second, the slanted curves are just physics as embodied by the classic rocket equation. There's only 3 categories of vehicle mass considered here: inerts, propellant, and dead-head payload. The curves show the interplay among the three, with two explicitly shown, calculated to a fixed velocity-change requirement. None of those curves would ever change, given the same velocity requirement.
The horizontal lines represent the performance levels of typical rocket propulsion technologies. In essence, this is the influence of that portion of the mass budget that is propellant. I showed 3 chemical and one old nuclear system as a guide.
Technologies can improve, shifting these horizontal lines slightly, but chemistry has been "stalled" for decades, pretty much where it is depicted. The nuclear technology offers the most hope of improvement, but has not been seriously worked-on in 4 decades. What I show is what was cancelled right before it could be flight-tested, the variant that was most mature back then.
The vertical lines represent the effects of materials and construction techniques upon the inert weight. This has seen the most change in recent decades. The modern 5-10% inert range is now pretty typical of commercial launcher stages. Rolled textured aluminum alloy panels are what make this possible, in concert with higher-tech versions of the engines that have lower engine weight for the same thrust. Long ago, that was closer to 20% with things more like frame-and-stringer type construction.
I have to caution readers and users of these graphs that these 5-10% inert weight percentages are typical of one-shot (throwaway) stages, not anything that might be reusable. One-shot designs contend with ascent loads and ascent heating only. Descent loads and descent heating are not only worse, they are totally different in character. You have to deliberately design for them from the outset in a reusable design. You also have to have a service lifetime in mind for a reusable design, something totally different than "just-surviving-the-mission" with a one-shot design.
The early history of aircraft design is the most recent example of a technology arena where we have learned a very fundamental lesson the hard way (with many lives lost): the robustness of a long service life is simply heavier, because more materials are required to withstand the forces. There is no escaping that fact-of-life, and that is why I spotted recent modern aircraft values on the figure 6. These are basically dry weight divided by max gross weight. The difference is really both payload and fuel together. (Airplanes are different from rockets, after all.)
The 50% I show as "typical" of a long-life transport or bomber aircraft might not be representative of a reusable winged space launcher, but the 40% of the all-metal X-15 rocket airplane is a good startpoint for guessing what might be suitable for a reusable winged craft. Those are fundamentally different from "not-winged" vertical launch stages, reusable or not.
Composites typically have at least twice the strength to weight of aluminum, but are even more vulnerable to overheating. You cannot replace all the metal with all-composites, except in minimum-velocity suborbital flight, and even that is on a heat-sink transient.
I hope these comments help provide additional guidance for those wishing to use my results. I really do appreciate the comments, Google +1's, and other feedback. Thanks, and have some fun playing with this stuff. I certainly did.
--GW