The illustration speaks for itself!
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Search code 15112025
Search keywords bad
government, idiocy in politics
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The illustration speaks for itself!
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Search code 15112025
Search keywords bad
government, idiocy in politics
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The International Space Station (ISS) is due to be retired
and de-orbited sometime during 2030. It
replacements are very likely to be commercial stations. The question arises: in what orbit should these new space
stations be located?
This is an important question, because they will all be located in one or
another low circular Earth orbit (LEO), in
order to stay out of the Van Allen Belt radiation (roughly about 900 miles = 1400
km up). Plane changes in low circular
Earth orbit are very costly to achieve, in terms of rocket delta-velocity (dV)
requirements.
This is because the plane change dV requirement (direction
only, with no speed change) is dV =
2*V*sin(angle change/2). At typical LEO
speed (around 7.8 km/s), a 10 degree plane
change costs about dV = 1.36 km/s. A 20
degree change costs 2.7 km/s. A 30
degree plane change costs about 4.0 km/s.
It gets worse very quickly, the
bigger the plane change angle.
The “right” answer to this important question depends
upon what you really intend to do with these new space stations. If you want them to support human or robotic missions
to the moon and planets, the ISS
orbit is just flat wrong, and by
a large amount!
Such missions need to be flown from an orbit near the plane of the moon’s orbit, or the planes of the orbits of the planets. All the planes of the various planets’ orbits about the sun are rather close to the plane of the Earth’s orbit about the sun, called the “ecliptic plane”. This situation is illustrated in the figure.
All these possible destinations do not require large
plane changes, if mounted from Earth orbits
inclined somewhere close to a band between the Earth’s equatorial plane and the
ecliptic plane, a band that also
contains the orbit of the moon about the Earth.
The plane of the ISS is at 55 degrees inclination to the
Earth’s equator, set there to enable
easy access for the Russians from launch sites in Russia. That’s a 60+ degree plane change to go
elsewhere, at least dV = 7.8 km/s! Earth surface escape is only 11 km/s!
That high ISS inclination is just plain wrong for
easy access to the moon or planets.
It always was. An equatorial
orbit about the Earth has the very lowest velocity requirements to reach from
an equatorial launch site, but all the
orbits in the equatorial-to-ecliptic band are fairly easy to reach, from pretty much any launch site in the US.
So, if you really want these future space
stations to actually successfully support future missions to the moon and
planets, manned or robotic, you want them to be in this band of
low-inclination orbits about the Earth.
Simple as that!
What might such mission support be? Well,
perhaps assembly by docking together a lunar or
interplanetary craft, at a space station
using remote manipulator arms, from components
sent up from Earth. This is an approach
well documented by the experience of building the ISS from the Space Shuttle
with its arm, and by the experience ever
since of using the ISS arm to dock supply and crew vehicles.
These lunar or interplanetary craft could be fueled
for their missions, using propellants previously
sent up by tanker vehicles from Earth,
and kept in tanks at the space station for such a purpose. We would need a way to load and unload
cryogenic propellants for this job,
since many such craft will need them. So far,
only room temperature storable propellants have been transferred in
weightlessness, using expulsion bladders
inside the tanks. You cannot do that
with cryogenics! No materials have
the necessary very large elongation capabilities, at such low temperatures!
SpaceX wants to do this tanker vehicle transfer with cryogenic
oxygen and methane in their “Starship” soon,
using ullage thrust. That approach
does alter the orbit, something not
tolerable when operating at a space station.
But there might be an easy way to do that cryogenic transfer
job, without spinning huge vehicles, or without applying any ullage thrust that
alters their orbits. See the
article “Tank Design for Easy Cryogenic Transfers In Weightlessness”, posted 26 July 2025 to this site (search code:
26072025, search keyword: space program). As the article indicates, this concept is undergoing the patent process. A patent is pending.
You
turn the system on, wait several
seconds, then start the propellant
transfer pump. No ullage thrust gets
applied, and no vehicles or space
station are spun up. There are no unwanted
forces at the tank mountings, applied to
anything!
The notion of elliptic departure and capture was explored in
the posting “Elliptic Capture”, dated 1
October 2024 this site. The notion of space
tug assist was first explored in the article “Tug-Assisted Arrivals and Departures”, dated 1 December 2024 this site. The search codes for those articles are
01102024 and 01122024, respectively. Both share the search keyword “space program”.
This selection of proper space station orbits, an effective cryogenic propellant transfer
tank, the notion of elliptic orbit departure
and arrival, and a reusable space tug
stage, together make possible a space
program of cost effectiveness that dwarfs anything ever seen before! And THOSE FOUR THINGS are what really needs
to happen!
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Search code DDMMYYYY 11112025
Search keyword space
program
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This article is for people who know little about high speed flight vehicles. It gets across some key concepts about:
#1. frontal thrust density and top speed capabilities,
#2. how the same inlet components are used quite differently
in ramjet versus turbojet installations,
#3. why achieving combined cycle engine designs can be so
difficult, and
#4. how heat
protection is the true driving issue for high-supersonic and hypersonic flight.
There are other articles posted here and available
elsewhere, that go into considerably
more detail about these topics. But this
one tries to illustrate the basics, to
get started.
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Get Acquainted Info: High Speed Vehicles
There are many concepts to understand about high-speed flight. Frontal thrust density is a very important issue. And, there is no “magic” to waveriders. See these 2 illustrations:
The number of propulsion nozzles at the back of a vehicle also
seriously affects frontal thrust density.
This applies to both rockets and airbreathers (of any type). See:
The over-simplified behavior of inlets on a supersonic ramjet vehicle is shown:
But, it is the basic as-illustrated
inlet behavior above, that drives supersonic
ramjet performance. Ramjet takeover from
the booster needs to occur no lower than shock-on-lip speed. The lower the shock-on-lip speed is, the smaller the booster can be, leaving more room for ramjet fuel and the
nonpropulsive items. Considerably higher
speed is still efficient:
For supersonic flight,
gas turbine engine installations use the same supersonic inlet
components, but they use them quite differently! These are usually low-bypass
“turbojets”, and they are usually fitted
with afterburners.
Unlike the ramjet,
which when operating properly, accepts
a fixed scooped air massflow from the inlet, the turbojet demands a variable air
massflow corresponding to its rotor speed(s), determined in turn by the throttle control
setting. The turbojet inlet has to vary
the captured air massflow to match engine demand, which inherently requires subcritical inlet operation,
with variable-but-significant amounts of
spillage around the cowl lip.
The dominant pressure-rise feature in a turbojet
installation is the compressor, not the
inlet! (The only pressure rise feature
in a ramjet is the inlet.) See:
High speed flight involves lots of aero-heating. Adjacent and captured air temperatures are
high. As you go hypersonic, shock impingements multiply heating rates
substantially. See:
Shown just below are the heating rates to, from,
and within, any given piece of
exposed material. There is steady-state
equilibrium (applicable to hypersonic cruise),
and there is transient behavior (applicable to atmospheric entry), to worry about.
Radiation occurs only when there is a view of something hot
or cold from the affected surface. The
emissivity “e” can make radiative transfer either inefficient if low, or efficient if high. It varies between 0 and 1. (The sigma represents Boltzmann’s constant.)
For convective transfer,
heating rates can be to, or
from, the surface. The “film coefficient” h is larger near
stagnation zones, and smaller on lateral
skins. The values of h all decrease as
the air thins drastically at very high altitudes.
Thermal conduction can be to, from,
or within the piece. The
conduction within acts to set the temperature distribution of the piece from
one end to the other. The other two
determine how much heat enters or leaves the piece. See:
It should now be obvious that the main enabling factor for
high supersonic, or especially
hypersonic, flight is really thermal
management, more so even than
propulsion.
And “scramjet propulsion”,
whether combined-cycle or not,
does not make your job any easier,
because it is geometrically incompatible with ramjet and gas turbine, including even most of the inlet. In fact, combining any of these propulsive cycles, including rocket, is difficult at best, because of the severe geometric
incompatibilities, not to mention the speed-of-application
differences. See:
The two that do combine well are rocket and ramjet, for the “integral rocket ramjet” (IRR):
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For posting on “exrocketman”
Search code DDMMYYYY: 02112025
Search keywords: aerothermo, airplanes,
ramjet
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The ravings of a trained mind.