View Full Version : Jovian System has better colony sites than moon&mars
The Jovian system is a superior target for self-sustaining colonization.
Quite a bunch of PF people (Nereid, all the mentors in earshot, and plenty of others) know the facts.
It is a beautiful and interesting system consisting of a variety of different moon-size objects within comparatively easy reach of each other. Trips between Jovian moons take only a few days.
One key fact is the availability of reaction mass for propulsion.
Europa has a thick ice shell covering its liquid water oceanic layer. Missions to the Jovian system might be equipped to take on reaction mass (water or liquid hydrogen) at Europa.
Europa ice is estimated to be many kilometers thick.
A colony with abundant nuclear electric generating capacity
could hollow out habitats in the ice, far enough below the surface
to be structurally secure.
Other moons such as Ganymede and Callisto look interesting too, and appear to have water ice.
Presumably the ice on Europa is rocky---has minerals mixed in with it.
It should not be too difficult to design a chemical plant to extract the raw materials for civilization.
Personally I would not want to go anywhere as dry and barren as mars and the moon----though mars has some lovely desert landforms, shaped in part by wind.
Natural beauty is important and the spectacular thing Europa has is a sky with the planet Jupiter in it. Jupiter diameter is 143 thousand km and the distance from Europa is 671 thousand km.
This means the angular width of jupiter is about 12 degrees.
Compare this with the full moon seen from Earth which is 1/2 degree wide. We are talking about a gorgeous planet 20 times wider than the full moon is in our sky. 400 times bigger in angular area, than the full moon. With more colors and cloudforms to make it interesting.
This is a very romantic sight.
Humans living in the ice-caves of Europa would probably go to the surface for their honeymoons. They might even reproduce prolifically because watching Jupiter and the other Jovian moons is so romantic.
Films made at Europa might have a good boxoffice on Earth.
The Jovian system would be a fun place to inhabit for many reasons, including the fact that the trip from one "planet" to the next takes only a couple of days. Each Jovian moon goes around the primary in a few days or a week. So transfer orbits have similar periods.
In the Solar system trips between planets take on the order of years,
whereas in the Jovian system trips take on the order of days. Plus reaction mass for propulsion is available in a not-very-deep gravity well. Energetically, water at Europa's surface is a lot more accessible than water at the Earth's surface. So as a supplier of propellant it is a good bargain to switch over from Earth to Europa.
I do not like the "moon-mars" initiative which seems to me a bad investment and destructive of human aspirations.
Some problems though are:
the multiple month long trip there or back,
the low levels of sunlight for producing food,
the large amount of radiation trapped in Jupiter's Van Allen belts. [are they called that there?]
Any ship designed to get people home from Jupiter would need to be HUGE. It's an enormous gravity well... \mu_{Jupiter} = 1.26e8 vs \mu_{Earth} = 3.986e5
Etc.
EDIT: fixed numbers... *&^#% website giving G with meters instead of km
I just ran numbers. If you go in, you ain't coming back out.
It takes a delta V of 19.5km/sec to escape from Jupiter's gravity at Europa's distance.
Compare with ~11.2km/sec to escape from Earth.
Using a rocket with hydrogen and oxygen as fuel and oxidizer electrolyzed from Europa's water, you'd need 80 times the mass of the rocket in propellants, regardless of size.
Ain't gonna happen.
EDIT: fixed numbers
Originally posted by enigma
It takes a delta V of 19.5km/sec to escape from Jupiter's gravity at Europa's distance.
Compare with ~11.2km/sec to escape from Earth.
I believe your number is off by around a factor of three here. Not that it matters awfully.
Rough backofenvelope Europa's orbital speed is around 13.7 km/s
so escape from Europas distance out is around 19.4 km/s
The delta V is the difference-----19.4 minus 13.7
this is only 5.7 km/sec
this delta V is a factor of 3 different from the figure you quoted of 19.5
Ach. Of course you're right.
You'd still need a bunch of delta V to do the orbital transfer to Earth's orbit around the Sun, which isn't a small number, though.
Originally posted by enigma
...Using a rocket with hydrogen and oxygen as fuel and oxidizer electrolyzed from Europa's water, you'd need 80 times the mass of the rocket in propellants, regardless of size.
Ain't gonna happen.
What you say does not sound reasonable in light of, for example, NASAs own studies of the feasibility of manned missions to Jovian moons.
These were done in a fair amount of detail and involved
optimizing so as to make considerable use of Jupiter's own gravity
and the gravity of other moons.
I do not recall any figure like the one you offer, of a delta V for escape from Jupiter gravity at Europa distance of 19.5 km/s
or a fuel payload ratio of 80. These figures seem out of line.
Also your conclusion "aint gonna happen" seems out of line compared with NASA's fairly detailed mission proposal.
Maybe not gonna happen in the future we envision now, with a misdirected program. But the future changes.
One more thing, as regards the flat statement of impossibility.
At one time NASA had a nuclear rocket development program that was based not on explosion but on using a reactor to heat propellant.
For example the reactor may heat hydrogen, or water, to use as reaciton mass. I do not consider it totally certain that NASA will never re-embark on nuclear rocket development. So your calculation with chemical booster might not apply. Another case where I question
your flat statement of impossibility.
Originally posted by marcus
I do not recall any figure like the one you offer, of a delta V for escape from Jupiter gravity at Europa distance of 19.5 km/s
or a fuel payload ratio of 80. These figures seem out of line.
You were right, I flubbed up. It isn't the delta V, merely the escape velocity. That comes from the Vis-Viva equation. The fuel ratio comes from the ideal rocket equation.
It's possible to work out nuclear thermal rockets, but that improves your Isp by a factor of 3 or so. Half the mass of the ship in fuel to leave Jupiter's gravity. You still do need huge amounts of fuel to get back home, both to decelerate on a transfer ellipse, and then to decelerate again once you get to Earth. I'm not sure if it's possible to do a reverse gravity assist, or how much velocity you could bleed off from there.
Nuclear thermal rockets are a long way from operational status, unfortunately.
Another case where I question
your flat statement of impossibility.
Impossibility may be a bit harsh. Anything is possible. I'll tone my statements down to: highly unlikely anytime in the near term.
To be fair, I would love to have our current resources going into exploration missions to the Jovian moons, but bases there? well... they're just too far away from us, IMO.
Marcus: Europa ice is estimated to be many kilometers thick. A colony with abundant nuclear electric generating capacity
could hollow out habitats in the ice, far enough below the surface
to be structurally secure
Would tidal effects of jupiter and the other moons on europa be a major concern for habitats built into the ice?
edit: Not trying to be negative, just curious. It is an exciting idea. I would love to have a 12 degree Jupiter in my sky.
Mission design people have gotten quite clever about using gravity assist and indeed a "reverse" assist is quite practical on homeward leg
you are welcome to put nuclear thermal propulsion out of mind and imagine only H2 and O2 chemical
for anyone who wants to try some back of envelope trials
here is Hohmann transfer ellipse stuff.
orbital speeds of earth and jupiter are about 30 and 13 km/s
as y'probly know
to get to jupiter (without any gravity assist shenanigans) takes a delta V kick of about 8.5 at earth
and another (to catch up with jupiter) delta V of about 5.5
that is the ellipse starts at about 38.5 peri and
gets out to jupiter at about 7.5 ap (so it needs 5.5 added to catch up)
but the catching up can be done with the help of the gravity and the orbital speed of the moons
have to go, back later
well Im back. dont know if this thread will go anywhere though
everybody understand Hohmann transfer ellipse?
delta V at earth of 8.5 km/s
added to earths orbital 30 km/s
puts you on an ellipse with aphelion at jupiter
at which point the jupiter system is coming at you
at 5.5 km/s
and Callisto for example has an orbital speed of 8.2 km/s and escape from the jupiter system from Callisto's distance takes delta V of 3.4 km/s. Mission design people PLAY with the possibilities like teenagers play with weaving in and out of traffic on the freeway.
You are coming into the jupiter system at 5.5 km and there is a lot that you can do by way of "reverse gravity assist" as enigma called it. Some people are good at this and I am often amazed by their ingenuity.
Anyway I doubt you need to supply the whole arrival delta V of 5.5 from your own engine. I think you get a lot of that out of the Jovian system. And I think it is reversible. Going or coming the cost is going to be on the order of 8.5 plus a fraction of the 5.5, on the order of 10 km/s.
the problems are extremely tough. The trip is 2.7 years on the transfer ellipse (one half of it). That is already a grave if not horrendous problem right there.
But the delta V is not all that bad.
Originally posted by Jimmy
Would tidal effects of jupiter and the other moons on europa be a major concern for habitats built into the ice?
edit: Not trying to be negative, just curious. It is an exciting idea. I would love to have a 12 degree Jupiter in my sky.
Jimmy! I didnt see that someone else had dropped in.
I bet you are right, as regards Europa. the surface looks like it breaks now and then, probably from tidal action, and liquid water comes to surface and freezes. But I dont know!!!
Maybe there is someone here at PF who knows what has been learned about Jovian moons.
As for the 12 degree Jupiter (or however many degree, I was making a quick estimate) I would love that too. It is a beautiful orb for sure.
I wonder if there is any practical way to harness natural temperature differences to generate power. Assume there is plenty of nuclear power but nice to be able to supplement or gradually replace that
Thanks for your reply Marcus. I remembered reading that the ice on Europa would crack letting water well up onto the surface. I thought it might be because of tidal forces. Wasn't sure though.
Marcus: I wonder if there is any practical way to harness natural temperature differences to generate power. Assume there is plenty of nuclear power but nice to be able to supplement or gradually replace that.
What temperature differences did you have in mind?
And in the spirit of this thread:
http://members.aol.com/jrzycrim01/images/Europa.jpg
http://members.aol.com/jrzycrim01/images/Europa2.jpg
Images captured from Celestia
How do you embed an image in a post? I thought the img tag would do it but it just displays the url.
Originally posted by Jimmy
http://members.aol.com/jrzycrim01/images/Europa.jpg
http://members.aol.com/jrzycrim01/images/Europa2.jpg
Wow
Its late and I dont know the answers anyway.
I am going to have to read something about the main Jovian moons.
regards to you,
great pictures
That's quite alright. I should get off my lazy backside and research this myself as well. This is a great thread and I hope it spawns lots of discussion. I enjoyed your ideas about colonizing the Jupiter system. The posts about Hohmann transfer ellipses was especially interesting to me. Anyway, I need to climb into bed myself.
As far as the pictures, thanks. I don't really really deserve any credit. Celestia did all the work. [:D]
Originally posted by marcus
Going or coming the cost is going to be on the order of 8.5 plus a fraction of the 5.5, on the order of 10 km/s.
the problems are extremely tough. The trip is 2.7 years on the transfer ellipse (one half of it). That is already a grave if not horrendous problem right there.
But the delta V is not all that bad.
Alright
If your Hohmann numbers are correct (I have no reason to doubt they are), I got ~8.6 times the mass of the craft in propellants. If you then add in the numbers for leaving Europa, say 5km/sec, you're up to 29 times the mass of the craft. From Callisto, using your number of 3.4km/sec, it's ~20 times the mass of the craft.
That's a lot of fuel, but if the need is there, you just design around the need. You can plug in extra gravity assists, increasing the time. You can switch to an ion drive, but you couldn't harvest the fuel in-situ. You can go multi-stage, but that would increase system complexity, and be especially risky after a 2-3 yr minimum stationed in space without operating (on the trip there, plus mission time). It's possible (someone would have to run the numbers) that at the relative distances to the sun of the Earth and Jupiter that a bi-elliptic transfer may save fuel. It would add much time to the trip, unfortunately. Not a good alternative for manned return missions.
One really big problem I can see is you'd have to design cryogenics systems for the propellants that are built to operate for 6 years without a failure. That's a huge engineering feat. Add that to the potential for outgassing, as well as course correction and Earth re-entry delta V...
Humans in space are messy.
Originally posted by enigma
Humans in space are messy.
Oh yes, that is the main point, is it not?
I've always favored robotic space exploration over manned.
Machines do better in space and the robot probes have consistently
produced far more interesting information at less cost.
My point is that IF a decision is made at the policy level to
promote manned space ventures with extended stays (which might in itself be a wrong decision) then there are better ways to spend the money and lives----worthier manned space ventures, I mean.
I wont bother to reply to your points which seem to be general arguments against putting people into space (with all the extra equipement and fuel that entails). Because the premise is that we do that. Assuming we are to have extended stays on the Lunar/Martian surface or on some other body instead, lets compare relative merits
russ_watters
Jan22-04, 10:01 AM
Originally posted by marcus
What you say does not sound reasonable in light of, for example, NASAs own studies of the feasibility of manned missions to Jovian moons.
These were done in a fair amount of detail and involved
optimizing so as to make considerable use of Jupiter's own gravity
and the gravity of other moons. You have any info on that? It seems pretty far fetched. I'd be awfully surprised if the study went beyond the "gee, wouldn't it be cool if..." level.
The biggest hurdle I see is the size of the rocket due to the length of the trip. "Enourmous" doesn't even begin to describe it. Getting to the moon took only a few days and as such, life support wasn't that big of an issue. Getting to mars (just getting there, not doing anything or coming back) takes a good 6 months and the minimum total duration of the trip is about 2.5 years. Just getting to Jupiter would take more like 5 years. A ship with provisions for supporting a crew for that length of time would be huge - something to make Clarke's "Discovery" look like a dingy.
I'm thinking $100 billion for a trip back to the Moon (Apollo style - no base), $1 trillion for Mars, and $10 trillion for Jupiter. Awful, awful ideas.
I base this all on a key assumption: existing or near-future technology. Barring a quantum leap in propulsion technology (even scaling up ion propulsion would require at least a 10 order of magnitude improvement), we'd have to haul/make hydrogen and oxygen.
Originally posted by russ_watters
You have any info on that? It seems pretty far fetched.
Just getting to Jupiter would take more like 5 years.
You are saying using jupiter and its moons gravity is far fetched but this has already been done. Several probes have been there and taken pictures. When they go in, the paths is optimized to take advantage the system's own gravities, those of the moons as well as the primary. Gravity assists are demonstrated technology and have been used with some finesse on a number of missions.
You are wrong about the 5 years. At least according to my CRC handbook which gives Hohmann ellipse data. Half the period of the transfer ellipse Earth-to-Jupiter is about 2 and 3/4 years.
It is not 5. There is a significant difference.
this information is available to anyone who has the standard handbook of physics and chemistry. Probably also on the web.
As for the manned-mission studies done by NASA, I went down to the Engineering Library at the nearest educational institution. There is shelf after shelf of thick NASA books working out feasibility and grubby details of various missions that were considered when Manned Space was fashionable. IF they actually do revive Manned Space to a real significant extent then a lot of that that grubby detailed stuff becomes relevant again
It sure as hell was not limited to the "gee wouldnt it be cool" level. They were doing serious homework (in the years after Apollo). And that homework is sitting down at the library waiting for someone to blow the dust off.
russ_watters
Jan22-04, 01:27 PM
Originally posted by marcus
You are saying using jupiter and its moons gravity is far fetched but this has already been done. Sorry, I could have pared down the quote a little better - I was referring to the study. You are wrong about the 5 years. At least according to my CRC handbook which gives Hohmann ellipse data. Half the period of the transfer ellipse Earth-to-Jupiter is about 2 and 3/4 years. Fair enough. I pulled that out of the air. 2 3/4 years one way is still quite significant.
And I am still dubious about what these studies found. When manned spaceflight was "fashionable," they'd no doubt be willing to spend a hundred grand studying everything that popped into a mission planner's head, but I don't think that means they ever considered it a reasonable possibility. It might just mean they wanted to know.
I'm looking for this type of info. So far, I found some on MARS. (http://www.washtimes.com/world/20040111-112632-7636r.htm) It includes an estimate of $1 trillion for a single mission. THIS (http://www.usatoday.com/news/science/2003-12-04-moon-usat_x.htm) one says the cost of Bush I's Mars mission would have been $400 billion. That seems overly optomistic since it also says the original Apollo program cost $150-$175 billion in today's dollars (anyone think any government program ever meets its budget?). THIS (http://www.asi.org/adb/m/02/07/apollo-cost.html) one has some specific info on the early space program's costs.
Originally posted by marcus
well Im back. dont know if this thread will go anywhere though
everybody understand Hohmann transfer ellipse?
delta V at earth of 8.5 km/s
added to earths orbital 30 km/s
puts you on an ellipse with aphelion at jupiter
at which point the jupiter system is coming at you
at 5.5 km/s
and Callisto for example has an orbital speed of 8.2 km/s and escape from the jupiter system from Callisto's distance takes delta V of 3.4 km/s. Mission design people PLAY with the possibilities like teenagers play with weaving in and out of traffic on the freeway.
You are coming into the jupiter system at 5.5 km and there is a lot that you can do by way of "reverse gravity assist" as enigma called it. Some people are good at this and I am often amazed by their ingenuity.
Anyway I doubt you need to supply the whole arrival delta V of 5.5 from your own engine. I think you get a lot of that out of the Jovian system. And I think it is reversible. Going or coming the cost is going to be on the order of 8.5 plus a fraction of the 5.5, on the order of 10 km/s.
Okay, it doesn't quite work that way.
That difference of 5.5 km/sec only takes into account the relative velocity difference between the ship and Jupiter. Since the ship will be traveling slower than Jupiter you more or less place it in front of Jupiter and let the Planet "catch up". The thing is that as Jupiter catches up the ship will fall towards Jupiter due to Jupiter's gravity. Which means that by the time the ship reaches same distance form Jupiter as Europa is it will have a much larger relative velocity to Jupiter than 5.5km/sec.
In order to match orbit with Europa you must take into account all of the 5.5 km/sec and all but 1.4km/sec of the 5.6 km/sec gained by the fall into the Jovian system.
For a transfer from LEO to LEO (Low Earth orbit to Low Europa Orbit you need a total delta V of about 16 km/sec.
Add to this up to .9 km/sec for the broken plane manuever to match orbital inclinations of the planets.
As you said, some of this can be made up through gravity assists by fly-bys of the other Jovian moons, but to make significant inroads you would need to multiple passes. This could add quite a bit to your mission time.
Originally posted by Janus
As you said, some of this can be made up through gravity assists by fly-bys of the other Jovian moons, but to make significant inroads you would need to multiple passes. This could add quite a bit to your mission time.
You are right that it would add time. As I recall (and this was some time ago) there were multiple passes within the Jovian system. It is hard to reconstruct from memory because maneuvers using the gravity of several moons are sophisticated.
As to how much time it would add, since the typical orbit period in the system is around one week, is hard to say. One might guess a week or two.
My understanding is that gravity assist has been used in robot probe maneuvers within the Jovian system, so no big mystery about its application there.
Why dont the two of us, and whoever else wants, figure out a simple gravity assist for getting rid of some fraction of that 5 km/s. then we can see later how the pros did it, if I can ever find that article.
so we are approaching the Jovian system at 5.5 km/s
or if you prefer we are on a tangent ellipse and it is overtaking us at 5.5 km/s. But I shall think in Jovian coordinates from here on.
the first moon we use is probably Callisto
Its orbit speed around Jupiter is 8.2 km/s and escape from that distance is 11.6 km/s
So when we are in as far as Callisto we are going 12.8 km/s.
We do a flyby of Callisto while it is sunwards of Jupiter so that it parallels our 12.8 with its 8.2. We are both going in the same direction and we are passing Callisto at 4.6 km/s.
So we do a hyperbolic flyby around Callisto.
To understand what we are trying to do think of how it would be if Callisto were much denser so that we could swing around it in a hairpin turn, reversing direction. then we would be at Callisto distance (where circular orbit velocity is 8.2, but we would be going 4.6 km/s in the contary direction. So the net is 3.6 km/s in the same direction as Callisto, let's say 4 km/s. Since circular orbit velocity at that distance is 8.2 we would be falling inwards toward the planet, in an elliptical orbit around Jupiter.
This would have gotten us into Jupiter orbit essentially without expenditure of fuel and in one flyby maneuvre.
But Callisto is not dense enough that you can do a hairpin at 4.6 km/s. So we need a second encounter with a Jovian moon. This is where good mass data and mission design expertise comes in, neither of which I have. But perhaps you or someone else can supply some.
In effect a craft can go into the Jovian system like a pinball goes into a bunch of bumpers and cancel part or all of its unwanted speed relative to Jupiter by a series of flybys.
So if one eventually wants to get to Europa then one would not necessarily think of going directly there, but might well consider first passing either Callisto or Ganymede (by now this kind of indirection must be almost second nature among mission designers)
Does anyone have recent data on the masses of the Jovian moons and escape velocities. What I have is a bit out of date. Let's consider next using Ganymede for the first encounter, instead of Callisto
Escape velocity for any object at any distance from it is:
\sqrt{\frac{2*\mu}{r}}
Where \mu is G times the mass of the object, and r is distance from the center in km.
The calculations necessary are enormously difficult... certainly more than I would care to do for fun.
Again we are approaching the Jovian system at 5.5 km/s
(or it is catching up with us)
this time we focus on Ganymede.
Its orbit speed around J is 10.9 km/s and escape
from its distance from J is 15.4
Again we square 15.4 and square 5.5 and add them and take square root
(as before). I get 16.3 km/s.
The mission is timed so that Ganymede is sunwards of J so that it is going "backwards" at 10.9 km/s.
Our 15.4 is roughly in the same direction (this is just an approximate calculation) and so we are passing Ganymede at a speed of
about 5 km/s.
If we could whip around Ganymede in a hairpin turn so that we reversed direction our new speed would be in the same direction as Ganymede but only 5.9 km/s instead of Ganymedes 10.9.
So our new orbit, instead of being a circle like Ganymede's, would be an ellipse and we would be falling in towards the inner moons, Europa and Io et cetera.
But again, Ganymede is not dense enough for a tight turn. It is the most massive of the moons and has, I believe the highest escape-from-surface velocity. This is what you need for a tight turn. So a Ganymede flyby might be the most useful way to get introduced to the Jovian system. Since I dont have the best data on masses of the Jovian moons I will just leave it there---hope someone else can
take it further.
Anyway I'm skeptical that you need a whole bunch of reaction mass to take care of that 5.5 km/s with which you encounter Jupiter. I think engaging with the Jovian system at that end is more a matter of finesse. Glad of any comments!
Originally posted by enigma
Escape velocity for any object at any distance from it is:
\sqrt{\frac{2*\mu}{r}}
Hello enigma! Glad you are on board or at least somewhere off in space watching[;)]
I have already taken the escape velocity formula into account in the above discussion. A useful equivalent form is to say that it is equal to the circular orbit velocity multiplied by the square root of 2.
So the circular orbit velocity at Callisto distance is 8.2 and this means that escape from Jupiter from Callisto distance is 1.414 times that or 11.6 km/s.
This allows us to calculate how much speed an inbound craft will pick up if it is aiming for a Callisto flyby.
The effect of the MOONs' gravity is comparatively small until you get near them.
We are doing a very rough-and-ready back-of-envelope style of mission design here. Anyone who wants to can try it and get a rough approximate idea of the potential of gravity assist in the system.
If someone can supply a recent table of masses and orbit radii for the main moons it would help. ("semi-major axis" not radius of course)
For now here are the main data I'm using. Here are circular orbit speeds for the four big moons (from my old handbook)
Io 17.3 km/s
Europa 13.7 km/s
Ganymede 10.9 km/s
Callisto 8.2 km/s
I sure wish someone with more recent data would update these.
From these circular orbit speeds one can readily estimate what escape speed from Jupiter is, starting at that distance. Just multiply by squareroot 2.
A few things about the Galilean moons ...
A nice site is JPL's Galileo one; it has all kinds of goodies about Jupiter, the inner moons, and the mission, including this, packed with facts about the moons:
http://galileo.jpl.nasa.gov/moons/moons.html
Snippets:
- all Galilean moons have synchronous rotation, so Jupiter will appear to stand still in the sky (or be below the horizon) on all moons.
- Io in particular is in a fierce radiation zone (like the van Allen Belts, as enigma said), and there's a flux tube connecting it with Jupiter, carries millions of amps?
- the tidal locking is what keeps each of the inner three in its orbit (look at the periods - 1.77, 3.55, 7.15 days)
- tidal heating gives Io its spectacular volcanos (surely one of the more awesome sights), and also Europa its ocean; jury's still out re relative importance of tidal heating for Ganymede to keep its ocean
- IMHO, Callisto may be a better place to start - not as deep in the well, undifferentiated (so likely to have more rocks and metals around)
- Galileo used gravity assist to a considerable extent to change orbits (still needed rockets, of course); with four moons there's a lot of choice
Originally posted by marcus
Hello enigma! Glad you are on board or at least somewhere off in space watching[;)]
[;)]
This allows us to calculate how much speed an inbound craft will pick up if it is aiming for a Callisto flyby.
How's that?
This really isn't a simple problem. You pick up or bleed off speed because the center of gravitational attraction is moving away from you as you pass it. I haven't gotten into the nuts and bolts of gravity assists in a full year of orbital dynamics and space navigation classes, much less jumping around from moving moon to moving moon, all of which are moving about the moving Jupiter reference frame. I just checked, and my (very in-depth) textbook doesn't cover the topic either.
I don't know how much detail the CRC you looked at has, so I'll just post the full form of the energy equation, just in case (not meaning to insult if this is old-hat). That way you can do away with circularizing the orbital velocities.
\epsilon = \frac{V^2}{2}-\frac{\mu}{r}=-\frac{\mu}{2a}
That relates velocity to distance from Jupiter. It will have some (small) effect due to the eccentricity of the orbit, particularly for Callisto and Ganymede. You also get escape velocity by plugging in infinity for a.
I also found this (http://www.the-planet-jupiter.com/moons-facts-sheet.html) website which gives some of the orbital parameters, but not enough to place each moon's position relative to Jupiter or each other (it's missing argument of perigee, right ascension of the ascending node, and a reference true anomaly).
Originally posted by enigma
[;)]
...
I also found this (http://www.the-planet-jupiter.com/moons-facts-sheet.html) website which gives some of the orbital parameters, ...
thanks! turns out my figures were not so bad
agree with yours to the indicated accuracy, it looks like
http://www.the-planet-jupiter.com/moons-facts-sheet.html
source is NASA Goddard
Here's what they give for orbit radius thousands of km, and for siderial period days
Io 421.6 ******** 1.769138
Europa 670.9 ******* 3.551181
Ganymede 1,070 ******* 7.154553
Callisto 1,883 ******* 16.689018
those are practically the same as what I used, except for rounding, so the average orbit speeds should come out about the same
Here's what they say for moon mass and radius, so we can get the escape-from-surface velocities
Io 893.2 ****** 1821.6
Europa 480.0 ******** 1560.8
Ganymede 1481.9 ******* 2631.2
Callisto 1075.9 ******* 2410.3
units are E20 kilograms for the mass, and kilometers for the radius
Someone want to post the escape velocities? It gives a handle on how much use you can make of gravity assist from that moon.
Originally posted by marcus
Here's what they say for moon mass and radius, so we can get the escape-from-surface velocities
Io 893.2 ****** 1821.6
Europa 480.0 ******** 1560.8
Ganymede 1481.9 ******* 2631.2
Callisto 1075.9 ******* 2410.3
units are E20 kilograms for the mass, and kilometers for the radius
Someone want to post the escape velocities? It gives a handle on how much use you can make of gravity assist from that moon.
\mu's [km^3/sec^2]
Io: 5957
Europa: 3201
Ganymede: 9884
Callisto: 7176
Gives surface escape velocities of [km/sec]:
Io: 2.55
Europa: 2.02
Ganymede: 2.74
Callisto: 2.44
I still don't see how you're going to back out gravity assist potential without knowing the geometry of the trajectories...
Originally posted by enigma
...surface escape velocities of [km/sec]:
Io: 2.55
Europa: 2.02
Ganymede: 2.74
Callisto: 2.44
thanks! these agree except possibly in the second decimal place
with ones I was just now thinking of posting:
Io: 2.56
Europa: 2.02
Ganymede: 2.74
Callisto: 2.45
Glad for the agreement.
Your question about the possibilities for gravity asst. at the Jupiter end of the trip.
Obviously the full potential depends on the configuration of the system at the time of entry and the specifics involve geometric detail. I'm interested in quick rough guesstimates.
As Nereid already indicated in this thread, considerable use has already been made of gravity in the Jovian system and opportunties are good because there are a lot of massive objects (close together and going different speeds). The 1995 Galileo mission probably used gravity assist in the system a lot, not to mention 3 or 4 others that have been thru that neck of the woods.
From the rough guesstimates already done, I can see why the 5.5 km/s that you enter the system with might not be too hard to shed gravitationally. And for that matter, if your destination is Callisto, say, a good bit of the escape energy at Callisto's distance might also be shed.
(Once out of the earth's well) I'm guessing that the delta V cost of getting into orbit around Jupiter is mainly the initial 8.5 km/s kickoff at our end. Too sleepy to think more about it tonight tho.
What about Titan, the satellite of Saturn, that will be reached in January 2005 by The Cassini-Huygens probe?
http://saturn.jpl.nasa.gov/index.cfm
Titan has plenty of methane lakes, and I personally think that they will find life there. Is Titan profitable like a base for a human colony?
Originally posted by meteor
... methane lakes, and I personally think that they will find life there...
Meteor, I can't respond to the issue of "profitable" (either scientifically or economically).
I tend to think of the colonization urge as a healthy species urge, like sex, building houses, art and music. Things that
healthy people naturally want to do.
I would find living on Mars or the Moon depressing. But then I dont appreciate the state of Texas either.
I wouldnt like Titan becasue of the permanent fog and extreme cold---a most dreary possible climate.
A liquid water phase (like Europa's) is intrinsically around zero Celsius, a temperature I can understand. I would not mind a zero
Celsius ice cave environment as long as there was plenty of electric lighting. the prospect is a bit like Antarctica or Greenland, under the ice. Reminds me of where they built that neutrino telescope AMANDA 2.
But a liquid methane phase (like Titan's) is pretty scary for me to contemplate. And the atmosphere is so opaque one would never see the stars.
The question you need to ask, I think, is not "Would you like to do Science there?"
but
"Would you like to raise children there?"
In space, Science is something done via robotic extensions, surrogates, probes.
Titan could be of considerable scientific interest, and need to be investigated on scientific grounds. But it does not strike me as attractive for colonization.
What other large moons does Saturn have and what are they like, do you know?
Originally posted by marcus
thanks! these agree except possibly in the second decimal place
with ones I was just now thinking of posting:
[EDIT: I've thrown in the corresponding maximal circular orbit velocities----escape divided by sqrt 2]
Io: 2.56********1.81 km/s
Europa: 2.02********1.43 km/s
Ganymede: 2.74********1.94 km/s
Callisto: 2.45************1.73 km/s
Glad for the agreement.
The surface escape velocity from a body gives a quick handle
on the greatest deflection angle you can get by flying by it.
Even more convenient is that esc. speed divided by sqrt 2, the
surface circular orbit speed, or the maximal circular orbit speed.
The conventional notation is that the deflection angle theta
is half the total deflection. So to speak you get theta on the
way in and another theta on the way out. Just trig convenience.
The quick and dirty says
tan \theta = \frac{circspeed^2}{incoming speed^2}
So the smallness of these escape velocities makes it look unpromising. If I approach Ganymede at 4 km/s and swing close by it, I dont get deflected very much. Too bad. But mission designers still do this kind of maneuver so it must be worth something.
"Low Ganymede Orbit" speed is around 2 so squaring that speed and the incoming 4 km/s gives
tan \theta = \frac{4}{16}
tan theta = 1/4
theta is 14 degrees
total deflection from the encounter is 28 degrees
Enigma will be chuckling---see I told you so.
But I know that mission designers use the Jovian moons' gravity to save fuel. So I have to think harder about how this is done.
Maybe someone who knows something about it can help.
If one knew the configuration of the moons very precisely one might be able to program TWO or maybe even three flybys. each one deflecting some. So that it added up, in effect, to the idealized oneshot "hairpin turn" thing imagined earlier.
some grav. assist links:
http://cdeagle00.tripod.com/omnum/flyby.pdf
http://www.go.ednet.ns.ca/~larry/orbits/gravasst/gravasst.html
A better formula for the maximum turn angle is
2arcsin \frac{1}{1+rv_{oo}^2/\mu}
2arcsin \frac{1}{1+rv_{\inf}^2/\mu}
where r is the planet radius and v-sub-infinity is
the speed at infinity, and mu is the usual GM thing
with the dimensions cubic length over square time
So, if we're talking colonization, not a long-term research facility, how do we go about it? Do we remotely terraform first, then send people to fine tune the environment, or do we send people in to try to do terraforming? How would you terraform one of these moons?
I suppose, if there are oceans, that's a good start. We'd need to create an atmosphere. We'd want it to be richer in CO2 and methane to enhance greenhouse warming. We could analyse the ambient chemistry of the oceans, and select organisms that might survive and reproduce. More likely, we'd need to geneticly engineer organisms that could consume what exists, and produce the necessary environment. This would have to be done in stages. When the environment changes significantly, the next engineered organism is introduced, and so on.
Njorl
The temperature on the surface of Europa is -180o C. It is much the same on the surface of all Galilean moons, except near the volcanos of Io, where the lava temperature has been measured at >1,000o C.
The ice shell on Europa is ~20 km thick, though it may be as thin as 4km in places. In comparison, the lowest temperature recorded on Earth was at Vostok station (Antarctica), -100 oC. Lake Vostok (also in Antarctica) has a 4km thick layer of ice above it.
http://www.lpi.usra.edu/research/europa/thickice/
All the major moons of Jupiter and Saturn are fascinating targets for serious scientific studies.
Terraforming is contraindicated on almost all gas planet moons - they're mostly ices. Of course, if you like living in Antarctica or on the Greenland ice cap, terraforming without melting the ice is OK. The exception is Io. Millions of years of tidal heating have driven off the volatiles (just like for Mercury, Venus, Earth and Mars), leaving a rocky (silicate-based minerals) crust with an iron core.
I agree with marcus that there could be great satisfaction living on Europa or Callisto, but perhaps the primary group interested would be those who found living at Amundsen or Vostok in winter the pinnacle of their earthly existence.
Only Rhea and Iapetus may count as significant other sites for colonies in the Saturn system, and they both have a diameter less than half that of Europa's.
Originally posted by marcus
...some grav. assist links:
http://cdeagle00.tripod.com/omnum/flyby.pdf
http://www.go.ednet.ns.ca/~larry/orbits/gravasst/gravasst.html
A better formula for the maximum turn angle is
2arcsin \frac{1}{1+rv_{oo}^2/\mu}
2arcsin \frac{1}{1+rv_{\inf}^2/\mu}
where r is the planet radius and v-sub-infinity is
the speed at infinity, and mu is the usual GM thing
with the dimensions cubic length over square time
Enigma has thoughtfully tabulated some mu numbers for the Jove moons
mu's [km^3/sec^2]***********radius [km]
Io: 5957***********1823
Europa: 3201*********1561
Ganymede: 9884**********2631
Callisto: 7176*************2410
So I will recalculate the maximum turn at Ganymede, coming in at 4 km/s
2arcsin \frac{1}{1+2631*4^2/9884}
this time I get 22 degrees, not such a rough approximation, a bit more complicated but the right formula
Nereid I insist on being able to grow tomatos
so there has to be a lot of electric lighting down in the ice cave.
Be sure to put on warm clothing when you go sightseeing on the surface.
Using Enigma's mu numbers for the Jove moons again
mu's [km^3/sec^2]***********radius [km]
Io: 5957***********1823
Europa: 3201*********1561
Ganymede: 9884**********2631
Callisto: 7176*************2410
This time let's calculate the maximum turn possible at Callisto, coming in slower this time, at 2 km/s
2arcsin \frac{1}{1+2410*2^2/7176}
this time I get just over 50 degrees
I conclude that v-at-infinity has to be comparable to the escape velocity of
the orb if you want the turn to be a substantial angle.
This grav. assist link
http://cdeagle00.tripod.com/omnum/flyby.pdf
gives a formula for the maximum turn angle
2arcsin \frac{1}{1+rv_{oo}^2/\mu}
which is equivalent to
2arcsin \frac{1}{1+v_{inf}^2/v_{circ}^2}
where v-sub-infinity is the speed at infinity
where v-sub-circ is the circular orbit speed at surface
Again entering the Jovian system at 5.5 km/s this time lets go in to Io distance (may be reserved for robot ships because of radiation)
at which point speed is 25 km/s
Io orbit speed is 17.3 km/s
So if our speed parallels Io (the configuration is right at time of entry) we are passing Io with a v-infinity of around 8 km/s.
But Io's v-circ is 1.81 km/s (from a table a few posts back)
comparing these looks uninteresting
It turns out we can streamline the whole proceedure. Here are circular orbit speeds around Jupiter for the four big moons
Io 17.3 km/s
Europa 13.7 km/s
Ganymede 10.9 km/s
Callisto 8.2 km/s
And here are the circular orbit speeds around each moon, at its surface.
Io 1.81 km/s
Europa 1.43 km/s
Ganymede 1.94 km/s
Callisto 1.73 km/s
The basic given is that a ship comes into the J system at 5.5 km/s relativie to Jupiter.
I think that should be enough to work with and get maximum turn angles. Will see.
Originally posted by Jimmy
What temperature differences did you have in mind?
And in the spirit of this thread:
http://members.aol.com/jrzycrim01/images/Europa.jpg
http://members.aol.com/jrzycrim01/images/Europa2.jpg
Images captured from Celestia
Here's a shot of Ganymede (doesnt have J in it, you may have something more out of the ordinary)
http://www.ifa.hawaii.edu/faculty/barnes/ast110/gwas/ganymede.jpg
I was thinking of the temperature difference between the say 275 degree Kelvin sub-ice ocean and the say 120 degree surface.
Nereid gave an estimate of 5 km or so ice thickness IIRC so those
two different temperatures are not so near each other!
Do you have a picture of Callisto?
My Galileo printouts from NASA say that Callisto is unusual in not having an iron core---not having undergone differentiation.
This means the ironcompounds and other rock is more mixed up with the ice. that could be good.
The nasa book on the system says Galileo found that Io, Europa and Ganymede all have iron cores (!) so underwent quite some differentiation. Makes Callisto very interesting (closer to primordial planetary material) I suspect. I will try to find a picture.
Here's what I found. It is big (filling more than two of my screens) while in the process of downloading. So I have to scroll around to see it all. But then my computer adjusts it down to half the screen size to make it all fit (something I dont know how to circumvent)
http://www.solarviews.com/raw/jup/callisto.gif
there is an interesting large impact bruise near what seems to be the south pole. a fracture system of concentric circles.
the small craters expose what looks like ice---spots of high albedo.
Hey team! Didn't a post a really cool link a while back in this thread? All you ever wanted to know about the Galilean moons, but were afraid to ask, from the friendly folk at Galileo/JPL! More images than you can ever use too.
Callisto has two impact basins, Asgard and Valhalla - they're huge, have several concentric rings, etc. Similar structures can be found on Mercury (Caloris), the Moon (Orientale), Mars (Hellas), ...:
http://www.solarviews.com/cap/index/impactbasin1.html
Originally posted by marcus
The Jovian system is a superior target for self-sustaining colonization.
[BUNCH SNIPPED]
I do not like the "moon-mars" initiative which seems to me a bad investment and destructive of human aspirations.
In Hell Nasa techs and engineers etc. will be homeless, afflicted with some kind of mental illness and/or unable to adapt to a society that does not allow any other way of living, they will be cold and hungry and have jobs that are dehumanizing and aren't worth doing and I, I will be living on an ivory tower of number crunching autistic geekazoids and managers sending gleaming ships packed with everyones money into space and when those in the pits reach up a hand asking for relief from their misery I will say, "nope, sorry, too busy with my work and prestigee which I need to keep that marvelous wife, in tow and anyway, some day, a hundred years from now, I'll be able to let YOU live on another planet where food, shelter and money appears like magic at your feet..." if I acknowledge your existence at all.
Originally posted by Nereid
...
The ice shell on Europa is ~20 km thick, though it may be as thin as 4km in places.
http://www.lpi.usra.edu/research/europa/thickice/
...
All the major moons of Jupiter and Saturn are fascinating targets for serious scientific studies.
...
...
I agree with marcus that there could be great satisfaction living on Europa or Callisto, but perhaps the primary group interested would be those who found living at Amundsen or Vostok in winter the pinnacle of their earthly existence.
...
Nereid, great link about the 19 km thick ice (floating on the saltwater ocean). Your article had something about a brave soul who was practicing ice-diving, to see how it might be on Europa (!)
Glad you mentioned Callisto in same breath as Europa. Callisto now seems even more interesting because supposed to be undifferentiated.
Your link mentions a proposed Europa orbiter mission. Have you more info on proposed missions to J moons.
The point is, even if the future may be being trashed, yet the past proposals contain interesting parameters and can be enlightening to read.
I would like to see a proposal for a Callisto mission, especially if it had some practical detail to learn from.
Today I learned that the Galileo JOI burn only gave them 643 km/s
They needed less than one km/s to snag Jupiter
because they briefly went in deep (even inside Io orbit).
the history of Galileo mission is incredible. it began as a mars mission and was switched to venus. then they said try going to J.
but NASA had some bad trouble and the only booster available was only
big enough to go to Venus with. So they fired it and sent Galileo the long way round:
to flyby Venus (grav. assist)
back to flyby Earth (grav assist)
around again and flyby Earth (grav assist)
and finally it has enough go to get-up to Jupiter
(like driving the Freeway with a Lawn-mower engine)
Incredible epic story of doing more with less.
And then when they get there (approaching J with something like
5 km/s) they only need a delta-vee of 0.6 km/s to snag it.
and from then on all the maneuvers are gravity assist
never used the main engine again after the first loop.
I want to see how somebody proposes to put a machine down on Callisto
Oh, now I see the NASA link you mean, about getting the horses to drink.
Originally posted by Nereid
A few things about the Galilean moons ...
A nice site is JPL's Galileo one; it has all kinds of goodies about Jupiter, the inner moons, and the mission, including this, packed with facts about the moons:
http://galileo.jpl.nasa.gov/moons/moons.html
Snippets:
- all Galilean moons have synchronous rotation, so Jupiter will appear to stand still in the sky (or be below the horizon) on all moons.
- Io in particular is in a fierce radiation zone (like the van Allen Belts, as enigma said), and there's a flux tube connecting it with Jupiter, carries millions of amps?
- the tidal locking is what keeps each of the inner three in its orbit (look at the periods - 1.77, 3.55, 7.15 days)
- tidal heating gives Io its spectacular volcanos (surely one of the more awesome sights), and also Europa its ocean; jury's still out re relative importance of tidal heating for Ganymede to keep its ocean
- IMHO, Callisto may be a better place to start - not as deep in the well, undifferentiated (so likely to have more rocks and metals around)
- Galileo used gravity assist to a considerable extent to change orbits (still needed rockets, of course); with four moons there's a lot of choice
Ah HAH! You mentioned the bit about Callisto being undifferentiated!
I just realized that about her yesterday evening. Really makes that moon special!
Both for science and for possible eventual habitats.
Iron and aluminum ores near the surface, mixed with ice.
Forget terraforming. Takes centuries.
the moons are interesting, even if not terraformable.
but must have plenty of electric light down in the cave so that
plants can grow.
melting a pocket of liquid water far enough down under the ice to be safe (creating an accessible sub-ice lake) and giving that lake a big lightbulb to keep it warm and liquid, could make a place for sea-life (even if we couldnt live there)
so then you and I would go there and live like Eskimos (PC Inuit) on shrimp and walrus blubber. In effect we would fish thru the ice for whatever would grow in an illuminated underground lake
then we'd build an igloo of course. TS Eliot wrote a song about it with climate assumptions a bit different: (any old isle is just my style, under the bam under the boo under the bamboo tree) Igloos keep you nice and warm.
Who needs terraforming if you have lots of ice? (Old Inuit proverb)
I just read a 1995 account by Tod Barber of the Galileo team written 70 days before the craft entered the jovian system
http://www.planetary.org/html/news/Galileo/hot-top-galileo-jup02.html
it's exciting, a leaking oxidizer check valve was suspected
nitrogen tetroxide and the monomethyl hydrazine fuel are hypergolic
Tod says the first thing they planned on arrival was get a gravity assist from Io!
and only afterwards proceed to perijove and the JOI burn
that was what that first flyby of Io was about
passing forwards of a planet you give it some of your energy
passing astern of it you take energy from it
so they passed some 600 km in front of Io and it helped slow them.
the 49-minute JOI burn slowed them an additional 0.6 km/s (another document says 643 meter per second) these are tiny delta-vee amounts
then on the first loop they went out to apojove at 200 Radii and did another burn of I guess around 0.4 km/s to fatten the oval and raise the perijove up to 11 Radii. That was the socalled PJR (perijove raise)
They captured jupiter with a total of only about one kilometer per second delta-vee. After the JOI and PJR burns the main engine was never used again. Everything after that was done with the gravity assists derived from flybys of the moons.
All that stuff is reversible. So you could get OUT of the jove system by gravity assist and be on your way to earth with about one km/s of delta-vee.
at earth you might use atmospheric braking for some of the 8 km/s
or might rendevous with some other craft in LEO, like a shuttle.
What this says to me is that the delta-vee for a round trip is not as great as one might suppose at first. Galileo got to Jupiter starting with only enough boost to slow it down enough so it would fall in towards the sun as far as Venus. That is about 3 km/s. It did not even need the boost of 8 km/s one would assume for a transfer ellipse.
When it got there is just needed one km/s to get into orbit around jupiter and start doing flybys of the moons.
So I guess to get to jupiter one can do it with 3 + 1
then since it is reversible the return trip is 1 + 3
so that is a round trip for under 10 km/s
Say that is a mothership that does not ever land. It carries a lander to land on and take off from a moon. The lander needs fuel but that is a separate question. I am talking about the mothership trucking out and back and cruising around in the jovian system
Btw. the Galileo craft massed 2 tons and had two sections----rotating and non-rotating. the main engine was in the rotating part and the gyros and cameras in the non-rotating. I am getting to appreciate the design.
It seems like a good idea for a long-distance craft to rotate, as Galileo did. At least one section of it.
The 400 newton main engine was made by Messerschmidt (MBB).
Nitrogen tetroxide and Monomethylhydrazine. Sexy chemicals such as
hotrodders dream of. Kept aboard Galileo for 5 or 6 years stable in their separate tanks but ignite spontaneously whenever they come in contact.
Who can calculate the payload ratio if you want 10 km/s and are using Tet and Monomethyl. How much of the truck has to be fuel and how much can be payload. It would be nice to know that, I think.
Originally posted by marcus
So I guess to get to jupiter one can do it with 3 + 1
then since it is reversible the return trip is 1 + 3
so that is a round trip for under 10 km/s Is the second 3km/s necessary? After applying the 1km/s to get out of Jovian orbit, you are on an ellipse that crosses Earth orbit (since that is where the last gravity assit was done on the way there). Some delta-v may be necessary to be captured by Earth but it might be possible to burn it off with a double lunar gravity assist.
Originally posted by Cecil
Is the second 3km/s necessary?...
I wonder about this too. The Apollo missions used atmospheric braking on the return and I dont know to what extent thrust played a role, if it did at all. I think they may have approached the earth essentially at escape velocity and made a dive (at the right angle) thru the atmosphere. This seems pretty extreme, but I dont seem to recall that they went into LEO first or anything.
It seems conceivable to me that humans could do the Jove-Earth leg with the 1 km/s delta-vee to get out and onto an earth-crossing orbit, as you suggest. Just need the right kind of re-entry vehicle and the slowing down can happen in the atmosphere.
So maybe the minimum round trip delta-vee is 3+1+1
a lot less than what we thought when we began discussing it.
That said, suppose the bus that takes people on the J. tour is some big rotating hotel. If you dont spend the fuel to put that in LEO or some orbit when you get back, then that tour-bus is expended.
You can either let the bus go on by and have the people ride back in a little re-entry vehicle. Or you can slow the bus down and store it in LEO---hitch it to a space station or leave it for some future use. So the decisions make the problem more complicated.
I guess I am partial to the simplest form of the problem where you just say what is the minimum delta-vee for a round trip, not attempting to re-use anything.
If some people actually wanted to go live on Callisto, one would not be thinking so much of the problem of getting them home (although return could be provided for). Instead one would probably be thinking of a number of robot-ship one-way trips for machinery and supplies, setting down at some base on Callisto.
Only after a lot of unmanned tonnage had made the trip out there and was waiting on the ground, would you finally let the people travel.
And you might use more delta-vee for them to make the trip faster
(as well as sending them in a rotating cabin to keep them healthy).
But the unmanned supply trips out could be slow and use only the 3+1 km/s which we mentioned----or whatever it is Galileo used---plus whatever is needed to land on Callisto.
It does not seem a heck of a lot different from setting supplies and equipment down on the moon, delta-vee-wise, although the voyage takes a lot longer.
Originally posted by marcus
I wonder about this too. The Apollo missions used atmospheric braking on the return and I dont know to what extent thrust played a role, if it did at all. I think they may have approached the earth essentially at escape velocity and made a dive (at the right angle) thru the atmosphere. This seems pretty extreme, but I dont seem to recall that they went into LEO first or anything.
Apollo didn't do a re-orbit maneuver once they got to Earth. They did a small maneuver to get themselves into the right path for the ballistic re-entry.
They screamed into the atmosphere at over Mach 25.
That's the reason why the half-angle of the Apollo re-entry module was around 45 degrees compared to Gemini's 20. It needed the flow from the front of the heat shield to seperate almost immediately so it wouldn't heat up the nadir sides too much.
Originally posted by marcus
Who can calculate the payload ratio if you want 10 km/s and are using Tet and Monomethyl. How much of the truck has to be fuel and how much can be payload. It would be nice to know that, I think.
From a quick search on the performance of such engines I come up with a mass ratio of 25. (fully fueled ship vs fueled depleted ship)
I'll have to run some numbers to see if that can be theoretically brought down any by engine design parameters (combustion chamber pressure etc.
Originally posted by marcus
Who can calculate the payload ratio if you want 10 km/s and are using Tet and Monomethyl. How much of the truck has to be fuel and how much can be payload. It would be nice to know that, I think.
MMH/N204 has a vacuum Isp of ~333. N204/Hydrazine is slightly better at 340, but has tighter thermal restrictions.
Source:
http://www.astronautix.com
10,000 = - Isp * g_0 * ln \frac{M_0}{M_0 + M_P}
M_P = 19.1 * M_0
Not very good.
Originally posted by Janus
From a quick search on the performance of such engines I come up with a mass ratio of 25. (fully fueled ship vs fueled depleted ship)
Janus, this is very welcome input! Both you and Enigma have used the
rocket equation in this thread. Others of us might well be interested in a mini-tutorial showing how to do the payload fraction calculation.
Would you be willing to provide a basic explanation? As I recall one needs only to know the exhaust velocity (from Tet and Monomethyl in this case) and the desired delta-vee.
This set of problems is only gradually getting into focus for me, and perhaps others. I see now that
1.Callisto would be an interesting moon to explore and that
2.even if one imagines eventual manned missions the interesting case to look at, for propulsion requirements, is the one-way unmanned trip, and
3. the experience with Galileo suggests two parts: the initial boost out of low-earth-orbit into transjupiter orbit (or some indirect path involving gravity assists) which could use some less storable fuel, and then a second part for JOI, maneuvering and landing.
--------------
Nereid originally suggested Callisto might be interesting because undifferentiated. Richer chemistry maybe. risk of carbon monoxide?
well lets start by considering unmanned missions
Even if one imagines manned missions might eventually occur they would presumably be preceded by unmanned shipment of equipment and supplies. I am intrigued by the thought that a shipment might be done with something like 3+1+2 where the initial 3 is with non-storable fuel.
In any case, roughly what exhaust velocity should one assume for the fuel and oxidant used in Galileo
Well OK, Eric Weisstein's Mathworld
http://scienceworld.wolfram.com/physics/RocketEquation.html
gives it
\Delta v = u*ln(M_0/M)
where u is the exhaust velocity and M_0/M is the ratio
of the initial to the final mass
The exhaust velocity for MMH/N2O4 is about
3100 meters per second.
For JOI and maneuvering in the system suppose one allows
2000 m/s (twice what Galileo apparently got from its main engine)
2000 = 3100*ln(M_0/M)
I get a mass ratio of about 1.9, in that 2 km/s case,
that is, you boost the thing out of LEO and after it does its Jupiter-capture and all its maneuvering it weighs about half of what it did when it left low-earth-orbit.
some sources
http://dutlsisa.lr.tudelft.nl/Propulsion/Data/Rocket_motor_data.htm
http://fti.neep.wisc.edu/~jfs/neep533_lect41_chemRkt_99.html
for liquid hydrogen and oxygen the exhaust velocity seems to
be around 4400 meters per second
does any one have different figures. If that is right for LH2/LOX
and if 3100 is right for MMH/N2O4, then I have to say I am
impressed with the latter pair of chemicals-----storable and still
quite a good exhaust velocity.
Originally posted by marcus
where u is the exhaust velocity and M_0/M is the ratio
of the initial to the final mass
Just FYI, you won't find terribly much information giving the exhaust velocities of engines. It is tied up into the specific impulse, Isp.
Isp * sea level acceleration = exhaust velocity.
You will also sometimes see it listed as a characteristic exhaust velocity, 'c'. 'c' is the velocity which the propellant would have if you expand it out the nozzle to an infinite area, which of course, you can't do. It's just the theoretical limit for a specific fuel. If that's all you find, it's usually a decent first cut unless the nozzle is really crappy.
Isp changes with ambient pressure because of the pressure difference between the front of the rocket and the engine outlet. That accounts for 'sea-level' and 'vacuum' Isp.
Originally posted by marcus
does any one have different figures.
Check the astronautix website. They have statistics on practically every rocket, fuel combination, and mission ever built.
Originally posted by enigma
Check the astronautix website.
thanks for the link. I went to it earlier, when you gave the link, but was confused by the menu---couldnt see any menu item for propulsion data (may have been staring me in the face, it happens)
the Dutch page http://dutlsisa.lr.tudelft.nl/Propulsion/Data/Rocket_motor_data.htm
seems pretty good though
how does it compare with astronautix?
BTW I got curious about the TU-Delft site and looked further up
in the directory
http://dutlsisa.lr.tudelft.nl/Propulsion/Rocketpropulsion.htm
"In this lecture series the basics of space propulsion are delt with to a level sufficient for selecting the best propulsion system for a given space mission and to perform a preliminary dimensioning and sizing of the system. The lecture series consists of 8 lecture hours of 45 minutes each and forms part of a compulsory lecture series on the basics of space engineering given in the first three years (undergraduate program) of the study for aerospace engineer at TU-Delft, faculty of aerospace engineering."
I guess TU-Delft is the technical university at Delft in the Netherlands. The site has a lot of pages and so far I've only checked out a couple.
Originally posted by marcus
the Dutch page http://dutlsisa.lr.tudelft.nl/Propulsion/Data/Rocket_motor_data.htm
seems pretty good though
how does it compare with astronautix?
If you look at the bottom, it cites the astronautix website. [;)]
when you get to the main page, look at the links on the right. It has performance characteristics based on rocket/fuel/etc.
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