Re: Venturi question
- From: "Sorcerer" <Headmaster@xxxxxxxxxxxxxxxxxx>
- Date: Wed, 13 Sep 2006 13:43:36 GMT
<matt271829-news@xxxxxxxxxxx> wrote in message
news:1158151879.979616.41490@xxxxxxxxxxxxxxxxxxxxxxxxxxxxxx
| RP wrote:
| > Sorcerer wrote:
| > > <matt271829-news@xxxxxxxxxxx> wrote in message
| > > news:1158097941.649861.101980@xxxxxxxxxxxxxxxxxxxxxxxxxxxxxx
| > > | Sorcerer wrote:
| > > | > <matt271829-news@xxxxxxxxxxx> wrote in message
| > > | > news:1158004973.423968.104990@xxxxxxxxxxxxxxxxxxxxxxxxxxxxxxx
| > > | > | Hi
| > > | > |
| > > | > | It seems to be a well-established fact that the temperature
drops
| > > | > | inside a venturi tube (e.g. causing icing in carburettors). The
only
| > > | > | explanation I've been able to find is that "the expansion of
fluid as
| > > | > | it passes the throat causes a temperature decrease". I'm not
sure what
| > > | > | "passes" means here. The pressure inside the throat is lower
than the
| > > | > | pressure either side, right?
| > > | >
| > > | > No, not right. A venturi is narrower in the middle.
| > > | > The gas is squeezed down, that RAISES its pressure and
temperature,
| > > | > it cools by losing heat to the tube, but then it cools again as it
| > > leaves
| > > | > the exit upon expansion.
| > > |
| > > | The standard explanations (e.g.
| > > | http://en.wikipedia.org/wiki/Venturi_tube) say that pressure is
lower
| > > | in the narrow part of the tube.
| > >
| > > "Wikipedia does not have an article with this exact name. Please
search for
| > > Venturi tube) in Wikipedia to check for alternative titles or
spellings."
| > >
| > > Wackypedia is a disaster, any idiot can write it, and they do.
| > >
| > > Let's put it this way... As a piston falls in the engine, the lowest
| > > pressure is in the manifold, the highest is atmospheric in the air
filter.
| > >
| > > Venturi tubes are also used to measure water flow and the introduction
| > > of chlorine gas to kill bacteria; the lowest pressure is in the
reservoir,
| > > the highest at the faucet. Likewise air pressure is lowest at the top
of the
| > > atmosphere.
| > >
| > > Thus in the case of a carburettor the flow is from high pressure to
low,
| > > but in the water example it is from low pressure to high. If you say
| > > the pressure is lower in the narrow part of the tube, lower than what,
| > > inlet or exhaust?
| > >
| > > | If that really means that the density
| > > | of the gas (in terms of molecules per litre, say) is lower in the
| > > | narrow part, then the gas would be expanding as it *entered* the
narrow
| > > | part, and compressing as it *exited* the narrow part. This is what I
| > > | can't get my head round. Is it really true that the gas is being
| > > | compressed as it *exits* the narrow part??
| > >
| > > The gas is decompressed as it leaves. If you let the air out of a
truck
| > > tyre the valve will frost up. The pressure in the valve stem is
| > > slightly lower than the pressure in the tyre (100 PSI), but is much
higher
| > > than atmospheric (15 PSI).
| > > So if you have a restriction the gas or water squeezed down at
| > > the start of the tube and then drops pressure as it leaves, but
| > > in the water example the exit pressure is greater than the entry
| > > pressure.
| > > In numbers, 100 ft head of water at the faucet, 0 feet head at the
| > > reservoir which is on a hill.
| > > Faucet closed :
| > > At 50 feet, there is 50 feet head of water on each side the venturi.
| > > Faucet open:
| > > Water flows, there is then 50 feet head on the inlet side of the
| > > venturi, 49 feet head on the other, and 99 at the faucet.
| > >
| > > In other words the faucet is supporting the weight of 99%
| > > of the water, the venturi 1%.
| > >
| > > Look up Boyle's Law and Charles's Law.
| > > Androcles
| >
| >
| > I think the question is "where did the heat go?" So far we've
| > outlined three distinct cooling processes between us. Actually four,
| > because you and tadchem mentioned the vapor compression cycle
| > (refrigerator). This cooling cycle is not however due, or even remotely
| > related to the venturi effect. This would fall under the category of
| > plain old evaporative cooling instead. On the other hand evaporative
| > cooling can occur at the venturi outlet providing that the mixture
| > exiting the outlet contains liquid in some form. But this cooling
| > effect wouldn't be related to the venturi effect, it would only be
| > incidental.
| >
| > The process that you outlined isn't adiabatic. It requires a heat
| > sink. This was dubbed the "gas cycle" when it was first invented. The
| > restricted portion of the venturi would have to be maintained at a
| > temperature lower than the gas within it. If no heat sink is present,
| > then the cooling effect will only occur temporarily, i.e. until the
| > venturi and gas temps equalize.
| >
| > The adiabatic process that tadchem outlined causes cooling of the
| > entire volume of compressed gas, not just the gas at the outlet. This
| > is evident in his example of the aerosol can. It is the entire can that
| > cools rather than just the nozzle. The throttling effect (Joule-Thomson
| > process) that I mentioned causes a temperature drop that is
| > proportional to the drop in pressure, or in other words a cooling of
| > the gas exiting any orifice, be it a venturi or otherwise. Though there
| > would be some cooling within the connecting tubing and in the venturi,
| > it would be a much smaller effect than that occurring at the outlet
| > where the pressure drop is greatest. Evaporative cooling would occur
| > in similar fashion, since the throttling effect is essentially just a
| > further evaporation of the gas, so to speak. In the throttling effect,
| > even though the gas is already in vapor form, it still has internal
| > "cohesive" PE, and depending upon conditions, that PE may be either net
| > positive or net negative. The gas may cool down, or it may heat up,
| > depending upon its initial density and temperature, and of course it's
| > composition. This is one of the reasons that real gases aren't ideal.
| >
| > So take your pick, or mix and match.
| >
| > Matt, can you describe in more detail the actual system that you have
| > in mind? I'm no expert on this subject, but I might be able to describe
| > the process in terms other than this or that "effect". Basically, any
| > time a gas cools, it's because it has lost heat energy. That's a
| > bit of a tautology, but at least it tells us that the heat had to go
| > somewhere. I *think* your question is two-fold: How did the heat
| > transfer occur, and where did the heat go. Based upon your questions
| > so far, I'm really not sure what you're looking for other than a
| > better understanding.
| >
| > But now that you've brought the subject up, I'd like to know a little
| > more about it too. Maybe someone else can help us all out.
| >
| > Richard Perry
|
| Thanks for your reply Richard. The question just arose in conversation
| - the phenomenon of Carburetor icing was brought up, and it was
| suggested that the cooling was due to the venturi effect, but we
| weren't sure exactly how it happened. I've just come across another
| Wikipedia article actually -
| http://en.wikipedia.org/wiki/Carburetor_icing - which says that "Carb
| icing occurs when there is humid air, and the temperature drop in the
| venturi causes the water vapour to freeze." Unfortunately neither this
| nor any other reference I've found explains why this temperature drop
| should occur. That's really all I was interested in understanding.
|
| As you say, various different potential cooling processes have been
| mentioned. If expansion of the gas is in some way involved then I'm not
| at all sure where this is supposed to occur - you say that the pressure
| drop is greatest "at the outlet", but as I understand it the pressure
| is lowest in the narrowest part of the tube, which seems to imply that
| "expansion" would occur as the gas passes from the inlet into the
| narrow part. Is that wrong?
|
| Hmmmm!
Yes, it is wrong. You snipped the explanation so I'm not repeating it.
Androcles.
.
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- Venturi question
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- Re: Venturi question
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