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- Path: sparky!uunet!cs.utexas.edu!tamsun.tamu.edu!venus.tamu.edu!dwr2560
- From: dwr2560@venus.tamu.edu (RING, DAVID WAYNE)
- Newsgroups: sci.physics
- Subject: Re: bubble in container
- Date: 29 Dec 1992 15:37 CST
- Organization: Texas A&M University, Academic Computing Services
- Lines: 25
- Distribution: world
- Message-ID: <29DEC199215373722@venus.tamu.edu>
- References: <1992Dec28.165049.4878@novell.com> <1992Dec29.002632.22407@sfu.ca> <1992Dec29.011215.11278@novell.com> <1992Dec29.165004.23310@novell.com>
- NNTP-Posting-Host: venus.tamu.edu
- News-Software: VAX/VMS VNEWS 1.41
-
- dseeman@novell.com (Daniel Seeman) writes...
- >But the sinking part is really not central to the problem. One could just
- >anchor the bubble to the bottom of the container, fill the container with water,
- >and close it. With the help of a friendly gremlin (that lives inside the con-
- >tainer, of course ;-) the bubble would get bursted. After the system returns
- >to equilibrium, what are the differences between the initial and final pressures
- >in the container?
-
- Let's see if we can make the paradox a little clearer. Start with the
- sealed jar of incompressible fluid. Our gremlin builds a small sphere
- near the bottom of the container which naturally will contain a bit of
- fluid. Then through a tube he drains the sphere and fills it with
- air at the local fluid pressure. He then breaks the sphere and lets the
- bubble rise to the top, increasing the pressure everywhere. When the
- bubble reaches the top he reverses the procedure, surrounding it with
- a sphere, filling it with fluid, and breaking the sphere.
-
- The final state has the same fluid in the same volume but different
- pressure. In fact one can repeat the procedure ad infinitum to get
- as high a pressure as one likes.
-
- :-)
-
- Dave Ring
- dwr2560@zeus.tamu.edu
-