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- From: kpearce@magnus.acs.ohio-state.edu (BULLDAWG)
- Subject: Re: Metals in liquid Nitrogen !!
- Message-ID: <1992Dec11.200321.6333@magnus.acs.ohio-state.edu>
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- Organization: The Ohio State University
- References: <10DEC199219275429@trentu.ca> <1992Dec11.171454.3158@magnus.acs.ohio-state.edu> <Bz3y9A.6Jn@helios.physics.utoronto.ca>
- Date: Fri, 11 Dec 1992 20:03:21 GMT
- Lines: 132
-
- In article <Bz3y9A.6Jn@helios.physics.utoronto.ca> neufeld@helios.physics.utoronto.ca (Christopher Neufeld) writes:
- >In article <1992Dec11.171454.3158@magnus.acs.ohio-state.edu> kpearce@magnus.acs.ohio-state.edu (BULLDAWG) writes:
- >>In article <10DEC199219275429@trentu.ca> lchardon@trentu.ca (PETIT PAPA NOEL.) writes:
- >>>
- >>> I'm sorry if this has been discussed here before, but I'm quite
- >>>puzzled by the following:
- >>>
- >>>Sure enough, somebody pulled out a penny and dropped it in a
- >>>full styrofoam cup. What happens is the following:
- >>>The nitrogen will boil for some time, like it boils when you drop anything
- >>>in it,
- >>>but then suddenly it will boil really hard, about 3 times more
- >>>violently than it did before, for about half a second, and then it will
- >>>just gently bubble away (When the metal is in thermal equilibrium with it,
- >>>i guess...).
- >>
- >>But at this point, the metal makes a phase transition from one kind of
- >>metal crystal to another (bcc to alpha).
- >>
- > I doubt that. It's very quick in the case of copper in liquid
- >nitrogen. You need to move atoms around the crystalline lattice on the
- >time scale of seconds, and at quite low temperatures. I'd expect the
- >deformation of the lattice to powder many metals.
- > Also, the later bubbling is much stronger than even the room
- >temperature copper produces when first dropped into the liquid nitrogen.
- >It seems that this is consistent only with your theory if the phase
- >transition heats the copper up to substantially more than room
- >temperature. I'm trying to imagine a phase diagram where phase A is
- >stable at T1, and at T2 it goes to phase B, liberating enough energy to
- >heat it to T3 > T1. It seems unlikely.
-
- Sorry, but it is true. Phase transitions can (and are observed in labs
- down the hall from mine) and do occur in microseconds. The rearrangements that
- you refer to are on the order of _tenths_ of _angstroms_.
-
- Go back to fundimental chemistry. Phase changes are generally exothermic.
-
-
- >
- >>Whenever a substance under goes a phase trnsition it gives up heat.
- >>
- > Demonstrably false. Ice doesn't give up heat when changing phase to
- >water.
-
- You have missed the point. Water going to ice gives up heat (delta H of
- freezing). A phase change in copper will give up heat (going to a
- thermodynamically more stable form at lower temperature).
-
- To assert that the copper must _heat_ _up_ (become hotter) because of the
- phase change (and thus be impossible) is strictly ignorant of phase
- change processes that have been well characterized for over 100 years!
- When a phase change occurs, heat is liberated (or absorbed) in exactly
- the amount that is being removed (or added) to the sytem until the entire
- system completes the phase change. This is the origin of the so-called
- phase transition temperature halt. (note that an ice-water mixture is always
- pretty close to 0 C at equilibrium regardless of the proportion of water/ice).
-
- Anyway, I can go on until I am blue in the face about thermodynamics. Go pick
- up a book on it, _Physical_Chemistry_ by Arfkin is a good start.
-
- >
- >>>
- >>> WHY ???????????????
- >>
- >>
- >>> WHY JUST METALS ???
- >>
- >>Well, just about anything will work, but metals have phase transitions at
- >>lower temperatures so that most of the bubbling from cooling off is gone.
- >>
- > I disagree.
- >
- > Here's what I believe, and I put copper sample holders into liquid
- >nitrogen sometimes several times a day, always seeing this effect. As
- >another poster remarked, when the copper is first put into the liquid
- >nitrogen it forms a vapour barrier which prevents the liquid nitrogen
- >from coming into good mechanical contact with the copper. To do this it
- >need only balance the hydrostatic pressure of the liquid nitrogen, a
- >couple of percent of atmospheric pressure for common laboratory dewar
- >depths (unlike your counterexample of trying, I believe, to levitate an
- >iron block on a drop of nitrogen). The copper cools until the liquid
- >nitrogen can come touch it. At this point the heat transfer rate goes way
- >up (as evidenced by the thermocouple in my experiment (which does not,
-
- But at this point you would be right back to "levitating" the LN2 away from
- the object and you would see according to your assertion, cycles of fast
- bubbling, slow bubbling, fast, slow, etc which is _not_ seen.
-
- >BTW, show some huge heat spike from the latent heat of a phase
- >transition)).
-
- As above, you would not see a heat spike, you would see a slowing down of the
- cooling momentarilly (with the new fast bubbles).
- In fact, since the situation is far from equilibrium,
- you probally wouldn't see the eutectic halt unless you had a _very_ fast
- thermocouple and meter and indeed I would be hard pressed to say how you could
- seperate the fast cooling from the LN2 from the eutectic halt that adds some
- heat to the over all process.
-
- > Nitrogen boils furiously for a while, and with my
- >experiment, in which the copper isn't fully immersed in the liquid
- >nitrogen, you can see that the liquid is now touching the metal, where
- >before it obviously wasn't.
-
- I have done the same experiment myself in the lab (today, I just happen to
- use LN2 as a coolant for my experiments), and I only see the situation
- you describe when the sample is near LN2 temparture. But if you look
- carefully, you will see that _between_ where the bubbles are breaking the
- surface, the LN2 is touching the surface.
-
- > Why does this happen only with metals? In order to be obvious there
- >has to be a long time between immersion of the object in the nitrogen and
- >the time when the surface of the object reaches a temperature which
- >allows nitrogen to touch it. This implies a high heat capacity (not
- >really true of metals) and/or a high thermal conductivity (very true of
- >metals). The high thermal conductivity of the copper means that the whole
- >penny has to be cooled down before the nitrogen can touch it, rather than
- >just a thin surface layer, as would be the case for styrofoam or wood.
- >
-
- Ken Pearce,
- just a grad student in Physical Chemistry }:)
-
-
- >
- >--
- > Christopher Neufeld....Just a graduate student | Entropy isn't what it
- > neufeld@helios.physics.utoronto.ca Ad astra | used to be.
- > utzoo.utoronto.ca!generic!cneufeld |
- > "Don't edit reality for the sake of simplicity" |
-
-
-