From: Robert Clark on
On Mar 15, 10:02 am, Me <charliexmur...(a)yahoo.com> wrote:
> On Mar 14, 9:24 pm, Robert Clark <rgregorycl...(a)yahoo.com> wrote:
>
> > Then it is important that such a SSTO vehicle be produced even if
> > first expendable to remove the psychological barrier that it can not
> > be done. Once it is seen that it can be done, and in fact how easily
> > and cheaply it can be done, then there it will be seen that in fact
> > the production of SSTO vehicles are really no more difficult than
> > those of multistage vehicles.
> > Then will be opened the floodgates to reusable SSTO vehicles, and low
> > cost passenger space access as commonplace as trans-oceanic air
> > travel.
>
> More clueless BS.  Clark thinks he is smarter than everyone else.

[re-posted to correct typos.]

No. I'm reporting what some experts in the field have said, that it
is easier to produce a SSTO vehicle with dense fuels rather than with
hydrogen.
Some examples:

Single Stage To Orbit Mass Budgets Derived From Propellant Density and
Specific Impulse.
John C. Whitehead, Lawrence Livermore National Laboratory.
32nd AIAA/ASME/SAE/ASEE Joint Propulsion Conference.
Lake Buena Vista, FL July 1-3, 1996
Abstract
"The trade between specific impulse and density is examined
in view of SSTO requirements. Mass allocations for
vehicle hardware are derived from these two properties, far
several propellant combinations and a dual-fuel case. This
comparative analysis, based on flight-proven hardware,
indicates that the higher density of several alternative
propellants compensates for reduced Isp, when compared
with cryogenic oxygen and hydrogen. Approximately half
the orbiting mass of a rocket-propelled SSTO vehicle must
be allocated to propulsion hardware and residuals. Using
hydrogen as the only fuel requires a slightly greater fraction
of orbiting mass for propulsion, because hydrogen engines
and tanks are heavier than those for denser fuels. The
advantage of burning both a dense fuel and hydrogen in
succession depends strongly on tripropellant engine weight.
The implications of the calculations for SSTO vehicle
design are discussed, especially with regard to the necessity
to minimize non-tankage structure."
http://www.osti.gov/bridge/servlets/purl/379977-2LwFyZ/webviewable/379977.pdf

A Single Stage to Orbit Rocket with Non-Cryogenic Propellants.
Clapp, Mitchell B.; Hunter, Maxwell W.
AIAA, SAE, ASME, and ASEE, Joint Propulsion Conference and Exhibit,
29th, Monterey, CA, June 28-30, 1993.
Abstract
"Different propellant combinations for single-stage-to-orbit-rocket
applications were compared to oxygen/hydrogen, including nitrogen
tetroxide/hydrazine, oxygen/methane, oxygen/propane, oxygen/RP-1,
solid core nuclear/hydrogen, and hydrogen peroxide/JP-5. Results show
that hydrogen peroxide and JP-5, which have a specific impulse of 328
s in vacuum and a density of 1,330 kg/cu m. This high-density jet fuel
offers 1.79 times the payload specific energy of oxygen and hydrogen.
By catalytically decomposing the hydrogen peroxide to steam and oxygen
before injection into the thrust chamber, the JP-5 can be injected as
a liquid into a high-temperature gas flow. This would yield superior
combustion stability and permit easy throttling of the engine by
adjusting the amount of JP-5 in the mixture. It is concluded that
development of modern hydrogen peroxide/JP-5 engines, combined with
modern structural technology, could lead to a simple, robust, and
versatile single-stage-to-orbit capability."
http://www.erps.org/docs/SSTORwNCP.pdf

Alternate Propellants for SSTO Launchers.
Dr. Bruce Dunn
Adapted from a Presentation at:
Space Access 96
Phoenix, Arizona
April 25 =96 27, 1996
Introduction
"The most commonly proposed propellant combination for an SSTO
launcher is liquid oxygen and liquid hydrogen, at a mixture ratio of
approximately 6.0. There have been a number of studies of alternate
fuels for SSTO launchers, but they have been limited. To date, most
studies have concentrated on methane, propane and RP-1 burned with
liquid oxygen to the exclusion of other oxidizers and other fuels.
These studies have often, but not always shown lower vehicle dry
masses for hydrocarbon propellants (for the same payload size). The
lowest dry masses of all are found in dual-fuel vehicles, using dense
hydrocarbons early in the flight and hydrogen late in the ascent.
These vehicles however suffer from mechanical and structural
complexity over their single-fuel cousins, and are unlikely to
represent the least expensive way to get a defined payload to orbit."
http://www.dunnspace.com/alternate_ssto_propellants.htm

This is certainly a minority opinion that dense fuels are better for a
SSTO than hydrogen, but it has occurred numerous times in science that
the minority opinion turns out to be the correct one.

The argument for why dense propellants are better for a SSTO is quite
simple and can be understood by anyone familiar with the "rocket
equation" that describes the relationship between the exhaust
velocity and the mass of propellant for a rocket. Indeed the argument
is as about as close to a mathematical proof as you can get in
engineering.

First two key facts have to be kept in mind: 1.) the tank mass scales
by volume, *NOT* by the mass of the fluid contained. This means that
the same size and *same mass* tanks can hold about 3 times as much
kero/LOX as LH2/LOX. This is extremely important because the
propellant tanks make up the single biggest component of the dry
weight of a rocket, typically 30% to 40%, even more than that of the
engines.
And 2.) dense propellant engines such as kerosene ones typically have
thrust/weight ratios twice as good as hydrogen ones. This is key
because switching to kerosene means your fuel load and therefore gross
mass will be greater. But because of the kerosene engines better T/W
ratio, the increase in engine weight will be relatively small.
Many people get the second of these points. It's the reason why first
stages generally use kerosene or other dense propellant for example.
However, the first point most people are not as familiar with. But
it's the more important of the two because the increase in propellant
being carried far exceeds the increase needed to overcome the lowered
Isp of the dense propellants.
To see why tank mass scales with volume, take a look at the equations
for tank mass here:

Pressure vessel.
http://en.wikipedia.org/wiki/Pressure_vessel#Scaling

Note it depends only on tank dimensions, internal pressure, and
strength and density of the tank material. Then because the internal
pressure of the tanks will be about the same for the hydrogen case as
for the kerosene case, for proper operation of the turbopumps, the
kerosene filled tanks will hold about 3 times more propellant at the
same size and weight of the tanks.

Now for the calculation that switching to kerosene can result in
multiple times greater payload. The vacuum Isp for good hydrogen
engines is about 450 s, and for good kerosene ones about 350 s. This
means the mass ratio for a hydrogen SSTO is about 10 and for a
kerosene one it's about 20. These values are higher than what you
would expect based just on the vacuum Isp alone because you also have
to consider gravity and air drag, and the fact that the Isp is
decreased at sea level and low altitude.
Now suppose we switch our hydrogen-fueled SSTO for a kerosene-one
using the same sized tanks. The volume stays the same so the mass of
the tanks stays the same. But the amount of propellant is now about 3
times larger.
For the engines, since propellant mass makes up almost all the
vehicle gross weight, the gross weight will be about 3 times larger
too. So the engines will need about 3 times the thrust.
For the original hydrogen-engines the thrust/weight ratio was about
50 to 1. And since the gross mass was about 10 times the dry mass for
the hydrogen vehicle, this means the engine mass was about 1/5, or
20%, of the dry weight.
Now switching to kerosene makes the gross weight about 3 times
larger. If the kerosene engines had only a 50 to 1 T/W ratio then you
would need 3 times heavier engines so they would be at 3/5 of the dry
weight. But since the thrust/weight of the kerosene engines is twice
that of the hydrogen ones, the engine weight is 1.5/5, 30%, of the dry
weight so the vehicle dry weight is increased only by 10%, due to the
heavier engines.
Now since the mass ratio is 10 for the hydrogen case but 20 for the
kerosene, you normally need about twice the kerosene propellant for
the same sized vehicle+payload total to reach orbit. But what we
actually have is about 3 times more propellant in our kerosene
vehicle, 1.5 times more than is necessary to get the same vehicle size
and payload to orbit. The vehicle does weigh about 10% more in dry
weight, so then the total vehicle+payload weight that can now
be lifted to orbit will be 1.5/1.1 = 1.364 times higher than for the
hydrogen case.
Now for the hydrogen powered SSTO vehicles that have been proposed
the payload is a fraction of the vehicle dry weight. The 100,000 kg
dry weight of the VentureStar compared to the 20,000 kg payload
capacity is typical. Then the kerosene version of such a vehicle could
loft (1.364)*(120,000 kg) = 164,000 kg to orbit. Or considering that
our vehicle is at a dry weight of 110,000 kg with the kerosene-engine
change, the payload would be 54,000 kg, 2.7 times the payload weight
of
the hydrogen case.

As I said this is an easy calculation to do. But many people simply
won't do it. They have been so conditioned to think that Isp is the
most important thing that the assumption is hydrogen must be used for
an SSTO. It probably doesn't help matters the fact that the gross mass
becomes about 3 times as great with the dense propellants. Gross mass
has been frequently used as the measure of the cost of a launch
vehicle, which I like to call "the hegemony of the GLOW weight".
But this is actually a very poor measure to use. The reason is
propellant cost is a trivial component of the launch cost to orbit.
More important is the dry mass and complexity of the launch vehicle
for the payload that can be orbited. Then what's important is
switching to a dense propellant allows multiple times greater payload
at the same sized and similarly dry-massed vehicle.


Bob Clark


From: hallerb on
Why take along EVERYTHING for a SSTO when the vehicle could use a
airplane to get the in orbit portion to at least 50,000 feet above
most of the atmosphere, not tied to a single launch location, fly the
airplane to a convenient launch location, fuel to get to 50,000 feet
can be from tanker refueling along the way..........

granted for a really large payload a BIG HUGGER AIRLINER might need to
be a custom build, but the upsides are huge.

no risky loaded bomb launch being the first.

SSTO is just a distraction from the more important......

LOW COST TO ORBIT!!
From: J. Clarke on
On 3/21/2010 10:42 AM, hallerb(a)aol.com wrote:
> Why take along EVERYTHING for a SSTO when the vehicle could use a
> airplane to get the in orbit portion to at least 50,000 feet above
> most of the atmosphere, not tied to a single launch location, fly the
> airplane to a convenient launch location, fuel to get to 50,000 feet
> can be from tanker refueling along the way..........
>
> granted for a really large payload a BIG HUGGER AIRLINER might need to
> be a custom build, but the upsides are huge.
>
> no risky loaded bomb launch being the first.
>
> SSTO is just a distraction from the more important......
>
> LOW COST TO ORBIT!!

Why do people think that launching from 50,000 feet will help somehow?
Going into orbit is not a matter of going high, it's a matter of going
_fast_. Launching from 50,000 feet or from sea level you still need to
impart 18,000 miles an hour of delta-v. That's the hard part.



From: hallerb on
On Mar 21, 11:49�am, "J. Clarke" <jclarke.use...(a)cox.net> wrote:
> On 3/21/2010 10:42 AM, hall...(a)aol.com wrote:
>
> > Why take along EVERYTHING for a SSTO when the vehicle could use a
> > airplane to get the in orbit portion to at least 50,000 feet above
> > most of the atmosphere, not tied to a single launch location, fly the
> > airplane to a convenient launch location, fuel to get to 50,000 feet
> > can be from tanker refueling along the way..........
>
> > granted for a really large payload a BIG HUGGER AIRLINER might need to
> > be a custom build, but the upsides are huge.
>
> > no risky loaded bomb launch being the first.
>
> > SSTO is just a distraction from the more important......
>
> > LOW COST TO ORBIT!!
>
> Why do people think that launching from 50,000 feet will help somehow?
> Going into orbit is not a matter of going high, it's a matter of going
> _fast_. �Launching from 50,000 feet or from sea level you still need to
> impart 18,000 miles an hour of delta-v. �That's the hard part.

the hardest part is having enough fuel onboard to get you thru the
dense lower atmosphere.those large tanks weigh more.

with a aircraft first stage that part is taken care of by a mature
well understood technology, and since in air refueling to release
altitude would be used lots of unnecessary mass wouldnt need lifited
off the pad..

plus the aircraft with space plane could be released at the equator
gaing some margins too. and bad weather would be much less of a issue.
no more storm clouds nearing pad troubles. just fly a few hundred
miles away to a nice clear area.

its far easier to accelerate a lower mass object, the
From: Greg D. Moore (Strider) on
J. Clarke wrote:
> On 3/21/2010 10:42 AM, hallerb(a)aol.com wrote:
>> Why take along EVERYTHING for a SSTO when the vehicle could use a
>> airplane to get the in orbit portion to at least 50,000 feet above
>> most of the atmosphere, not tied to a single launch location, fly the
>> airplane to a convenient launch location, fuel to get to 50,000 feet
>> can be from tanker refueling along the way..........
>>
>> granted for a really large payload a BIG HUGGER AIRLINER might need
>> to be a custom build, but the upsides are huge.
>>
>> no risky loaded bomb launch being the first.
>>
>> SSTO is just a distraction from the more important......
>>
>> LOW COST TO ORBIT!!
>
> Why do people think that launching from 50,000 feet will help somehow?
> Going into orbit is not a matter of going high, it's a matter of going
> _fast_. Launching from 50,000 feet or from sea level you still need
> to impart 18,000 miles an hour of delta-v. That's the hard part.

Because 50,000 feet gets you above the bulk of the atmosphere which provides
a decent bonus.

--
Greg Moore
Ask me about lily, an RPI based CMC.