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Re: Potable Water - The Third Way.
| Jere Lull | 09 Oct 2007 00:35 |
>>> Getting rid of the disssolved gases in the headspace and as bubbles >>> forming on the sides of the tube is going to be a major headache. [quoted text clipped - 10 lines] > enough that the oscillations will be damped out and you will see a slow > change to equilibrium with little or no overshoot. Though I consider this whole discussion impractical, I haven't seen anyone mention that the fresh-water side will be drawn down fairly regularly. And, of course, the sea water side will be replenished from time to time.
Suck hard enough on the fresh-water side and you get even better "vacuum" at the top. (Dissolved gasses are likely to be a problem, though.) Cool the fresh-water side and water vapor will condense there -- the whole point of the exercise.
Thinking only momentarily on a problem that I have little interest in... if the fresh-water side is evacuated to the point that the salt-water side is slightly below the top, every once in a while (or perhaps often), the fresh-water side will be empty and only the previously-dissolved gasses evacuated.
The required evacuation pumps and one-way valves sound like the problem at the moment.
 Signature Jere Lull Tanzer 28 #4 out of Tolchester, MD Xan's new pages: http://web.mac.com/jerelull/iWeb/Xan/ Our BVI pages: http://homepage.mac.com/jerelull/BVI/
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| Mark Borgerson | 08 Oct 2007 22:17 |
> > <<SNIP>> > >> You need to get back to the gas law to see where this error lies. You [quoted text clipped - 19 lines] > create a headspace by liberating dissolved gases, then let the columns > drop to create vacuum, but you will have contaminated the freshwater side. The head space is generated by the evaporation (or boiling) of some of the water in a column. It's exactly the same principle that you get it you fill a closed tube full of mercury and then invert it, placing the end in a reservoir of mercury. (We call these things barometers.) You start with no head space, but when you invert it, VOILA! head space appears as the mercury sinks to a level where the weight of the mercury equals the atmospheric pressure. You get a much better vacuum with mercury, since it has a much lower vapor pressure at room temperature.
A column of water will behave the same way. The column just has to be much taller.
Some of the historical references on water barometers mention that, despite precautions, the water in the barometer eventually got contaminated with dissolved gases and they lost their accuracy.
> > At that point, you essentially have two water barometers, > > interconnected at the top. One is salty and warm, and [quoted text clipped - 21 lines] > increases, and the column heights will drop as the pressure goes up, > with the diffusion path increasing the whole time.\ I agree with that part---except for the oscillation part. I think the processes are slow enough and the thermal and physical masses are high enough that the oscillations will be damped out and you will see a slow change to equilibrium with little or no overshoot.
Mark Borgerson
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| Keith Hughes | 08 Oct 2007 17:13 |
> <<SNIP>> >> You need to get back to the gas law to see where this error lies. You [quoted text clipped - 4 lines] > You seem to have missed the fact that I proposed filling the tubes > completely with water so that the initial head space would be zero. No, it won't be zero. It can't be. If it is, then you have a solid liquid stream, and it's just a siphon. You have to have headspace. And it has to be sufficient to maintain separation of the seawater and freshwater to prevent contamination when filling the tubes. And it has to be large enough to prevent percolation carryover when boiling is initiated.
> At that point you release the pressure on the water and it falls > to the point where water weight plus vapor pressure equals 1ATm. A solid liquid loop will not separate into two separate columns. They have to be separated by a headspace. You can heat the seawater side and create a headspace by liberating dissolved gases, then let the columns drop to create vacuum, but you will have contaminated the freshwater side.
> At that point, you essentially have two water barometers, > interconnected at the top. One is salty and warm, and [quoted text clipped - 14 lines] > as bubbles forming on the sides of the tube is going to > be a major headache. Not a headache, an impossibility (they're not really dissolved at that point though) :-) That, and the increase in pressure due to water vapor will make this an oscillating, self-quenching system. It'll require more and more heat as the partial pressures of the non-condensables increases, and the column heights will drop as the pressure goes up, with the diffusion path increasing the whole time.
Keith Hughes
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| Mark Borgerson | 08 Oct 2007 15:19 |
<<SNIP>>
> You need to get back to the gas law to see where this error lies. You > have to *create* the vacuum. That requires a HUGE increase in volume > for whatever the initial headspace is. For this to happen you need a > much longer tube to start with. You seem to have missed the fact that I proposed filling the tubes completely with water so that the initial head space would be zero. At that point you release the pressure on the water and it falls to the point where water weight plus vapor pressure equals 1ATm.
At that point, you essentially have two water barometers, interconnected at the top. One is salty and warm, and one is fresh and cold. Neither need be too much longer than 33 feet. The actual height of the water will be less than 32 feet by a factor dependent on the temperature of the water in the warm side.
The real practical problem lies in the addition of the dissolved gases in the seawater to the water vapor in the headspace. What we have here is a rather inefficient degassing column. I spent a lot of time degassing seawater while working on my MS in chemical oceanography. I was trying to measure the dissolved hydrogen in seawater, and the oxygen, nitrogen, methane, and other gases kept getting in the way!
Getting rid of the disssolved gases in the headspace and as bubbles forming on the sides of the tube is going to be a major headache. As soon as you release the pressure and start warming the seawater side, bubbles are going to form all along the tube as the temperature rises and the pressure is less than 1ATM except at the bottom of the tube.
Mark Borgerson
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| Keith Hughes | 08 Oct 2007 05:53 |
>> <snip> <snip>
>>> How do you get 33' as 1/2 of the diffusion path. >> A quick thumbnail guesstimation at where equilibrium would likely be [quoted text clipped - 22 lines] > That fills the tube completely with water--at which point you > close the tube (with a one-way valve). Uhmm, a manual valve is a manual valve. A "one-way" valve is a checkvalve, and you wouldn't need to close it.
> When you release the > pressure at the bottom end, the water falls to the point where the [quoted text clipped - 8 lines] > about 7 feet of water vapor at the top of the tube and 33 feet > of water below the vapor. Ahh, no. See below...
>> Use the ideal gas law: PV=nRT >> [quoted text clipped - 6 lines] > > What is the 1 liter to which you refer? It is an example, for illustration purposes. It's the headspace (i.e. the amount of volume *not* filled with water, prior to closing the valve and letting the water columns 'fall').
The point is, whatever your starting headspace volume is, to get anywhere near a vacuum, the *VOLUME* of the headspace must increase 100 fold. That is the relevance of the ideal gas law. If you start with a 100ml headspace, then to get a decent vacuum, the water columns have to drop to a point where the headspace is 10L. *AT THAT POINT* you have sufficient vacuum to support a water column of around 30'. But the columns have dropped significantly to achieve that vacuum, and thus the columns must be much higher, as must the initial water column height.
The *only* way the headspace volume increases is if the water columns drop significantly, and the only way significant vacuum is created is if the sealed volume increases tremendously.
> This is not a closed system---the tube is open to a reservoir at > atmospheric pressure at the bottom. [quoted text clipped - 21 lines] > Well, not much higher----only about 17.5 mmHG higher. But that IS > a lot higher than zero! ;-) No, a lot higher. You're confusing vapor pressure with the "steam" pressure during distillation. Huge difference. Vapor pressure is the countervailing force (fighting condensation as it were) on the FRESH water side of the system (and the seawater side). Vapor pressure in both columns will be about the same, so you have to boil the seawater column to get any significant vapor transfer. This results in *much* higher pressure, which lowers the columns and increases the vapor path and....
>> And don't forget, there will also be significant evaporation (due to low >> partial pressures) on the freshwater side that will be in equilibrium [quoted text clipped - 10 lines] > > AHA!, you're assuming a much higher operating temperature than me. Yes, because you're mistaking the amount of "vacuum" you'll have available when the system reaches equilibrium.
> I was assuming something on the order of 20 to 25C. Then you are assuming an almost perfect vacuum, which can't happen since the boiling Must significantly raise the headspace pressure.
> You're going > to have to add to your energy budget the heat necessary to raise [quoted text clipped - 4 lines] > If you're going to work at those temperatures and pressures, you > probably need only a 22-foot tube. You need to get back to the gas law to see where this error lies. You have to *create* the vacuum. That requires a HUGE increase in volume for whatever the initial headspace is. For this to happen you need a much longer tube to start with.
Keith Hughes
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| Mark Borgerson | 07 Oct 2007 22:49 |
> <snip> > [quoted text clipped - 30 lines] > equilibrium, you'll have close to a vacuum and close to 33' water column > heights. And a lot more empty headspace than you started with. I see the problem. I am assuming that you completely fill a 40 foot tube with water using a pump capable of providing about 16-20 PSIG. That fills the tube completely with water--at which point you close the tube (with a one-way valve). When you release the pressure at the bottom end, the water falls to the point where the weight of the water column is one atm (about 14.7PSIA) minus the vapor pressure of water at 20deg C. The vapor pressure of water at 20C is about 17.5mmHg, or about 2.3% of the 760mmHg standard atmosphere.
Since a mercury has a density 13.6, the column of water will be 13.6 * (760- 17.6)mm high. That's 10.1m high, or about 33.12 feet high. In a 40-foot tube, that would leave about 7 feet of water vapor at the top of the tube and 33 feet of water below the vapor.
> Use the ideal gas law: PV=nRT > [quoted text clipped - 4 lines] > want to reduce it to 0.147psia? then you need a 100-fold initial-volume > increase. What is the 1 liter to which you refer?
This is not a closed system---the tube is open to a reservoir at atmospheric pressure at the bottom.
I'm assuming that you start with a head space (or initial volume) of zero. You then simply have to evaporate enough water to fill the top of the tube with water vapor to the point where vapor pressure + water weight = 1ATM.
> > I'm not sure that 'diffusion' is the proper term for the motion > > of the water vapor. After all, the heat engine is providing [quoted text clipped - 12 lines] > equilibrium point with the columns much lower than the initial starting > point, and the headspace pressure much higher. Well, not much higher----only about 17.5 mmHG higher. But that IS a lot higher than zero! ;-)
> And don't forget, there will also be significant evaporation (due to low > partial pressures) on the freshwater side that will be in equilibrium [quoted text clipped - 10 lines] > 4-5psia when equilibrium is reached, which would require a temp of about > 60°C (140°F) to maintain boiling. AHA!, you're assuming a much higher operating temperature than me. I was assuming something on the order of 20 to 25C. You're going to have to add to your energy budget the heat necessary to raise the water temperature from 20C to 60C, then.
If the equilibrium pressure is really 1/3ATM, then there will be about 20 feet of water in the 40-foot tube and 20 feet of vapor. If you're going to work at those temperatures and pressures, you probably need only a 22-foot tube.
> Here in my neck of the woods, our energy from the sun ranges from about > 220-360 BTU/ft^2/Hr measured at normal incidence, depending on the time [quoted text clipped - 51 lines] > > Keith Hughes Mark Borgerson
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| Keith Hughes | 07 Oct 2007 19:25 |
<snip>
>> Yes, and this "migration" is simple diffusion. *And* you have (in the >> example above) 33' of column it has to diffuse through on the seawater [quoted text clipped - 5 lines] > > How do you get 33' as 1/2 of the diffusion path. A quick thumbnail guesstimation at where equilibrium would likely be reached. I didn't take the time to calculate the exact heights.
> I think there will be > about 33 feet of water in the column on each side Then I think you would be wrong, unless your columns are significantly longer than that, probably more like 50+ feet.
>---to provide the > weigth that pulls the pressure down. That would leave only about > 7 feet of water vapor path on each side of the column. There is no vacuum to hold the water up - the vacuum is what you are trying to *create*. The water columns will drop until there is an equilibrium point reached between the external atmospheric pressure, the height (weight as you state) of the water column, and the pressure in the headspace (the U-tube). The water columns *must* retreat, or the headspace stays at atmospheric pressure. If the tubes are long enough, and the initial column heights are high enough, then when you reach equilibrium, you'll have close to a vacuum and close to 33' water column heights. And a lot more empty headspace than you started with.
Use the ideal gas law: PV=nRT
For our evacuation purposes, nRT is a constant (#moles is constant, R doesn't change, and assume constant temperature), so if you start with a volume of 1 liter, and a pressure of 14.7 psia, and you want to reduce that pressure to 1.47psia, then you need a 10-fold volume increase. You want to reduce it to 0.147psia? then you need a 100-fold initial-volume increase.
> I'm not sure that 'diffusion' is the proper term for the motion > of the water vapor. After all, the heat engine is providing > water vapor on one side and condensing it on the other---so there > is a net mass flow and probably a small pressure differential to > move the vapor. Well, diffusion is the primary mechanism. What happens when your 'heat engine' creates water vapor? It doesn't just immediately condense on the other side. It creates pressure on the heating side, which does two things. One, it drives both the water columns *downward*, and it raises the boiling point on the seawater side (it does, however, make condensation on the fresh side more efficient as well). You can't look at this as a static system where the pressure stays the same or the column heights stay the same. It's a dynamic system, and will reach an equilibrium point with the columns much lower than the initial starting point, and the headspace pressure much higher.
And don't forget, there will also be significant evaporation (due to low partial pressures) on the freshwater side that will be in equilibrium with (and in opposition to) the condensation process. It's not as simple a system as it seems.
That's why this system *will* work, but it must work very slowly.
> Still (pun intended), you need a lot of heat to provide the energy > to evaporate the water or it will soon cool to the point where > its vapor pressure is reduced and the process slows drastically. My 'guess' would be that the system would end up operating around 4-5psia when equilibrium is reached, which would require a temp of about 60°C (140°F) to maintain boiling.
Here in my neck of the woods, our energy from the sun ranges from about 220-360 BTU/ft^2/Hr measured at normal incidence, depending on the time of year. A couple of decades ago I worked at a solar test lab and we tested all kinds of collectors, including swimming pool collectors which are unglazed (i.e. no cover over them to exclude wind). Bare copper tubes, painted black, with no wind, are about 15% efficient at solar absorption (#'s are from my old memory, so...) when the tubings' longitudinal surface is perpendicular to the incident angle. However, with a 3 mph wind (per ASHRAE 95-1981 which we used for indoor system simulations) that efficiency drops to the low single digits. When you factor in off-angle response (i.e. since the tubes won't be on a tracking mount to keep them 'aimed at the sun") the basic efficiency drops from ~15% to probably ~8%, and with the wind, between -3% to 3%. So, using only the tube as a collector is a real challenge. Probably be better using a flat-plate collector as the primary heater, but that's another major addition to the complexity.
Of course, too much heat would kill the system with over pressurization.
> The fact that the water 'boils' near room temperature does not > reduce the amount of heat required to change the water from > liquid to vapor. No, in fact the lower pressure raises it a bit. Latent Heat of Vaporization for water is inversely proportional to the pressure, albeit the change is less than 10% IIRC.
> As has been discussed, the simple idea does not address the problems > of salt buildup in the seawater side, or the addition of dissolved > gasses to the vacuum part of the loop. Non-condensables are a rate limiter for the process, unless you want to spend more energy for vacuum deaeration.
> With a large enough (or double) saltwater tube you might get a > convection cell going with the cold, saltier water sinking and > pulling up warmer seawater to the top. Certainly possible, but not easily doable.
> You could solve the dissolved gas problem by periodically pumping > both tubes up enough to displace the accumulated gases. Well, if you added a convection cell as above (another system that requires time to reach an equilibrium condition to work), then the periodic headspace purging would quench both the distillation and the seawater convection systems. In reality, the purging would be likely be very frequent given the size of tubes that would be practical.
> Now the project is getting complex enough that an RO system > starts to look attractive! Yep, sure does.
Keith Hughes
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| Mark Borgerson | 07 Oct 2007 17:14 |
> >>> Ah well, another great idea skuppered by dat old devil science :-) > >>> [quoted text clipped - 27 lines] > sides will be the same, and that diffusion path will be up to 66'. That > does not happen quickly. How do you get 33' as 1/2 of the diffusion path. I think there will be about 33 feet of water in the column on each side---to provide the weigth that pulls the pressure down. That would leave only about 7 feet of water vapor path on each side of the column.
I'm not sure that 'diffusion' is the proper term for the motion of the water vapor. After all, the heat engine is providing water vapor on one side and condensing it on the other---so there is a net mass flow and probably a small pressure differential to move the vapor.
Still (pun intended), you need a lot of heat to provide the energy to evaporate the water or it will soon cool to the point where its vapor pressure is reduced and the process slows drastically. The fact that the water 'boils' near room temperature does not reduce the amount of heat required to change the water from liquid to vapor.
As has been discussed, the simple idea does not address the problems of salt buildup in the seawater side, or the addition of dissolved gasses to the vacuum part of the loop.
With a large enough (or double) saltwater tube you might get a convection cell going with the cold, saltier water sinking and pulling up warmer seawater to the top.
You could solve the dissolved gas problem by periodically pumping both tubes up enough to displace the accumulated gases.
Now the project is getting complex enough that an RO system starts to look attractive!
Mark Borgerson
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| Keith Hughes | 29 Sep 2007 17:04 |
>>> Ah well, another great idea skuppered by dat old devil science :-) >>> >>> Bruce in Bangkok >>> (brucepaigeATgmailDOTcom) >> A 32' column of water is a continuous vacuum pump. This is just plain wrong. As a *unit of measure* 32 feet of water column equals about 13.9 psi. Meaning, if you pumped a 40' column up to a 39' height with water, equalized the headspace to atmospheric pressure (assuming 14.7psia), sealed it, then allowed gravity to *drain* the water column to a height of 2', the resulting pressure in the headspace will be about 0.8psia. Now you also have 33' of empty evacuated column.
>> As long as you put >> water (salt water) into the column it will pull down and keep a vacuum >> in the top of the column. Sorry, this makes no sense. Putting water in does not cause it to "pull down". Yes, you have supply makeup water to maintain column height lost to evaporation.
>> The fresh water distills off the top of the >> saltwater column then migrates Yes, and this "migration" is simple diffusion. *And* you have (in the example above) 33' of column it has to diffuse through on the seawater side, and however many feet of column on the freshwater side it has to traverse prior to condensation. If both columns (fresh and sea) are referenced to the same height, then the evacuated column height on both sides will be the same, and that diffusion path will be up to 66'. That does not happen quickly.
In reality, though, the columns won't be referenced to the same level, with the freshwater column being referenced (i.e. the bottom is opened to) the deck height on the boat. So the freshwater column will be, say 8' higher than the seawater column. The diffusion path is still the same, but the evacuated seawater column would then be 37', with 29' on the freshwater side.
>> as steam to the other side and distills >> in the fresh water side....also creating a vacuum. No, this does *not* create a vacuum in the sense you seem to mean. It maintains an equilibrium pressure by lowering the partial pressure of water vapor generated by the 'boiling' process on the seawater side.
This relates to the critical rate-limiting feature of the system - maintaining pressure. When you evaporate, or sublime, water into the headspace, the pressure in the headspace increases. Condensation on the other side lowers the pressure, and an equilibrium pressure will eventually be established. For any given temperature, the evaporation rate is going to be limited by the partial pressures at the headspace/water-surface interface. It's a feedback loop, More evaporation -> more water vapor molecules liberated to the headspace -> more pressure in the headspace -> slower evaporation until the pressure is reduced. And to reduce the pressure, those molecules have to diffuse up to 66'.
>> You draw off the >> fresh water on one side and pump salt water into the other side. The [quoted text clipped - 3 lines] >> boiling at low temperatures...even ice will change state to steam in a >> vacuum. The idea works. Yes, VERY slowly. You can increase *throughput* by increasing the column diameters, but how practical is that on a boat?
> It works but does it work as well as other methods that are simpler and > easier to implement. Also if you have no fresh water on hand to start > with there is no way to make it work. Not quite true...you can seal the 'freshwater' column, using only the column walls for condensation surfaces, until you have sufficient condensate collected to allow the freshwater column to be opened.
> I can see someone getting a > "Darwin Award" by accidentally spilling all there existing freshwater > supply in a failed attempt to get this contraption going. It doesn't *have* to be that way, BUT.... :-)
>> In a practical sense, I would use soft tubing for the sides and a >> solid "U" shaped piece of copper tubing for the top center with a ring [quoted text clipped - 3 lines] >> salt water and the bottom end of the fresh water tube could go to a >> small pump to remove the water without breaking the vacuum. And what's 'practical' for useability, is impractical for functionality. There are no 'soft tubing' materials I'm aware of that have anything approaching decent heat absorbance, conduction, or emissivity properties, so that will be another very significant rate limiter in the system.
> That makes no sense. You are going to have a hard time pumping water out > of the fresh water side any faster than gravity can deliver it. You actually *can't* pump faster than gravity, unless you want to suck seawater up the column on the other side.
> The > salty side OTOH, if you rely only on gravity to feed it, will become a > solid block of salt once you have evaporated enough water from it. Doubtful that you'd ever get a solid chunk of salt (and short of having a bypass circulation loop - cooling the column and further reducing efficiency - I don't see how a pump could even help the situation), but of course as the salinity increases, the boiling point increases, and at some point the process will just stall. The heat input won't be sufficient to boil the brine solution. Then you have to stop, drain, clean, and start over. How quickly this happens will depend on column heights and diameters, but it'll happen at some point. Just another rate-limiting feature.
All these rate limiters are natures way of saying that there is no thermodynamic free lunch. A low energy input system will have a low output (in terms of whatever work you want the system to do).
Keith Hughes
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| jim | 29 Sep 2007 15:09 |
> > Ah well, another great idea skuppered by dat old devil science :-) > > [quoted text clipped - 12 lines] > boiling at low temperatures...even ice will change state to steam in a > vacuum. The idea works. It works but does it work as well as other methods that are simpler and easier to implement. Also if you have no fresh water on hand to start with there is no way to make it work. I can see someone getting a "Darwin Award" by accidentally spilling all there existing freshwater supply in a failed attempt to get this contraption going.
> In a practical sense, I would use soft tubing for the sides and a > solid "U" shaped piece of copper tubing for the top center with a ring [quoted text clipped - 3 lines] > salt water and the bottom end of the fresh water tube could go to a > small pump to remove the water without breaking the vacuum. That makes no sense. You are going to have a hard time pumping water out of the fresh water side any faster than gravity can deliver it. The salty side OTOH, if you rely only on gravity to feed it, will become a solid block of salt once you have evaporated enough water from it.
-jim
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| jim.isbell | 29 Sep 2007 14:42 |
> Ah well, another great idea skuppered by dat old devil science :-) > > Bruce in Bangkok > (brucepaigeATgmailDOTcom) A 32' column of water is a continuous vacuum pump. As long as you put water (salt water) into the column it will pull down and keep a vacuum in the top of the column. The fresh water distills off the top of the saltwater column then migrates as steam to the other side and distills in the fresh water side....also creating a vacuum. You draw off the fresh water on one side and pump salt water into the other side. The salt water side is painted black to absorb sun heat and the fresh water side is painted white to reflect the suns heat. You only need a few degrees difference for distillation and the vacuum creates the boiling at low temperatures...even ice will change state to steam in a vacuum. The idea works.
In a practical sense, I would use soft tubing for the sides and a solid "U" shaped piece of copper tubing for the top center with a ring soldered to it so it could be hoisted up the mast of a sailboat. It would take a 30 to 40 foot mast to do the job. The bottom end of the salt water tube could go to a through hull for a continuous supply of salt water and the bottom end of the fresh water tube could go to a small pump to remove the water without breaking the vacuum.
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| brucedpaige@gmail.com | 28 Sep 2007 00:36 |
>>> On Sat, 22 Sep 2007 10:55:52 -0500, Brian Whatcott >>> <betw...@sbcglobal.net> wrote stuff [quoted text clipped - 25 lines] >require huge and expensive heat exchangers, in either case not >competitive. TANSTAAFL. Ah well, another great idea skuppered by dat old devil science :-)
Bruce in Bangkok (brucepaigeATgmailDOTcom)
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| Glen Walpert | 27 Sep 2007 21:25 |
>> On Sat, 22 Sep 2007 10:55:52 -0500, Brian Whatcott >> <betw...@sbcglobal.net> wrote stuff [quoted text clipped - 4 lines] > >Gravity. Wishful thinking. Where are you going to get the feedwater containing no noncondensible gasses in solution? In all real distillation plants a continuosly operating vacuum pump is required to maintain vacuum and prevent the condensers from filling with noncondensible gasses. There is no way you are going to eliminate the vacuum pumps with any kind of inverted tube arrangement.
For reasonable efficiency real distillation plants are multi-stage, where the latent heat of condensation from one stage is used to boil feedwater in the next stage, with up to 5 stages being used in larger plants (in the days before reverse osmosis made them uneconomical by comparison). Sucessive stages operate at lower pressures, and corresponding lower temperatures. The 1100 or so BTU required to boil one pound of water can thus boil up to 5 pounds of water instead.
You still need enough thermal gradient to get the heat to flow through all those heat exchangers. By using low thermal differentials between the hot and cold ends you either reduce capacity to a pittance or require huge and expensive heat exchangers, in either case not competitive. TANSTAAFL.
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| jim.isbell | 27 Sep 2007 13:54 |
> On Sat, 22 Sep 2007 10:55:52 -0500, Brian Whatcott > <betw...@sbcglobal.net> wrote stuff > and I replied: > > But what is the cheap source of getting the vacuum? I figured there > had to be a vacuum, although it was not said. But how do you get it? Gravity.
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| OldNick | 23 Sep 2007 03:39 |
On Sat, 22 Sep 2007 10:55:52 -0500, Brian Whatcott <betwys1@sbcglobal.net> wrote stuff and I replied:
But what is the cheap source of getting the vacuum? I figured there had to be a vacuum, although it was not said. But how do you get it?
>>Well no, he obviously hadn't figured that out. Nor can anybody figure >>out what is going to hold a column of water 40 ft high as was stated in [quoted text clipped - 27 lines] > >Brian Whatcott Altus OK Human bevaviour: Bestiality with a brain
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| Brian Whatcott | 22 Sep 2007 15:55 |
>> What Brian left to the reader's imagination, is that the head >> space of the tubes is at a near perfect vacuum, flooded only with >> water vapor. You might recall that a perfect vacuum will lift a >> column of water about 32 feet, on a high pressure day. Or had >> you not figured that out?
>Well no, he obviously hadn't figured that out. Nor can anybody figure >out what is going to hold a column of water 40 ft high as was stated in [quoted text clipped - 7 lines] > >-jim Well, at least this respondent Jim, is operating at shall we say the 7th grade level of science/engineering insight. Like so many other products of the domestic school system, he seems to have a severe case of self-esteem syndrome.
Still, he may be retrievable, starting with a science demonstration he may have missed. Place a beaker of water in a bell-jar and pump the air out.
When 99% of the air has been pumped out, the water in the beaker is boiling vigorously, until, in the usual way, the beaker boils dry. The beaker feels cool to the touch, naturally.
To quote him: "unless I have a cheap source of heating this won't work..."
For the $64 prize: NOW do you get it?
Brian Whatcott Altus OK
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| jim | 22 Sep 2007 15:15 |
> Dear Larry: > [quoted text clipped - 21 lines] > column of water about 32 feet, on a high pressure day. Or had > you not figured that out? Well no, he obviously hadn't figured that out. Nor can anybody figure out what is going to hold a column of water 40 ft high as was stated in the original post. The tubes may be 40 feet but the column of water will be considerably less. How much less will depend on how much energy is heating on the hot side and how much energy is cooling on the cool side. The total amount of energy needed is not going to be any different than any other distilling method. Unless you have the free or cheap sources of cooling and heating at specific temperatures this isn't going to work any better either.
-jim
> David A. Smith |
| N:dlzc D:aol T:com (dlzc) | 22 Sep 2007 01:48 |
Dear Larry:
> dlzc <dlzc1@cox.net> wrote in news:1190415672.506271.93890 > @k79g2000hse.googlegroups.com: [quoted text clipped - 13 lines] > AT 40' ASL, the boiling point must be down > to...to....211.95F! What Brian left to the reader's imagination, is that the head space of the tubes is at a near perfect vacuum, flooded only with water vapor. You might recall that a perfect vacuum will lift a column of water about 32 feet, on a high pressure day. Or had you not figured that out?
David A. Smith
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| Larry | 22 Sep 2007 01:26 |
dlzc <dlzc1@cox.net> wrote in news:1190415672.506271.93890 @k79g2000hse.googlegroups.com:
> There are ship-board distiller units that use an engine to pull a > vacuum, and the engine's waste heat to boil that water, to generate > drinking water. A little shorter... > > David A. Smith http://en.wikipedia.org/wiki/Boiling_point
"The boiling point of water is 100 °C (212 °F) at standard pressure. On top of Mount Everest the pressure is about 260 mbar (26 kPa) so the boiling point of water is 69 °C. (156.2 °F)."
AT 40' ASL, the boiling point must be down to...to....211.95F!
Larry
 Signature Search youtube for "Depleted Uranium" The ultimate dirty bomb......
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| dlzc | 21 Sep 2007 23:01 |
Dear Brian Whatcott:
> You've heard all about distilling water, and you've > heard all about reverse osmosis, but you haven't [quoted text clipped - 18 lines] > > [An engineering effort of a U of Utah group I think] There are ship-board distiller units that use an engine to pull a vacuum, and the engine's waste heat to boil that water, to generate drinking water. A little shorter...
David A. Smith
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| Brian Whatcott | 21 Sep 2007 22:35 |
You've heard all about distilling water, and you've heard all about reverse osmosis, but you haven't heard about low-cost, low energy stills: they are brand new.
Briefly: Take one forty ft vertical tube filled with saline. Take one forty ft vertical tube filled with fresh water. Connect them with a little engineering help - at the top.
The boiling point of water at sea level pressure is about 100 deg C
The boiling point of water at the top of a sealed 40 ft column of water is near ambient. So, it doesn't take much heat to boil the brackish water, and have it pass to the fresh column where it is slightly cooled to hold the near vacuum conditions at the boiling level.
[An engineering effort of a U of Utah group I think]
Brian Whatcott Altus OK
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