home *** CD-ROM | disk | FTP | other *** search
- Path: sparky!uunet!cis.ohio-state.edu!ucbvax!SLEEPY.NETWORK.COM!logajan
- From: logajan@SLEEPY.NETWORK.COM (John Logajan)
- Newsgroups: sci.physics.fusion
- Subject: The importance of being chained
- Message-ID: <9207290006.AA08478@sleepy.network.com>
- Date: 29 Jul 92 00:06:42 GMT
- Sender: daemon@ucbvax.BERKELEY.EDU
- Lines: 70
-
- Tom Droege reports an apparent 9mW average difference between
- bosons on and off.
-
- If we postulate that the source of the 9mW of heat is D+D=>He plus
- 24MeV, we find that that implies a minimum of 1.2 Curies of
- activity (A Curie is 3.7E+10 events per second.)
-
- However, Tom's boson source is nowhere near one Curie. In fact,
- it is marked 0.5 microcurie -- one two-millionth of a Curie. He
- further suggests that the source is old and is only a fraction of
- its marked activity, he speculates as low as (or lower than) 0.008
- microcurie. This is less than one 150-millionth the number of
- events required to generate the observed heat on a one-for-one
- basis.
-
- It doesn't take a rocket scientist to see that some sort of chain
- reaction *must* be appealed to. [Standard disclaimer about the
- reliability of the original data, etc.]
-
- An average gain per trigger event of less than 1.0 will never
- account for the gain of 150 million. An average gain of exactly
- 1.00000 will not account for it either.
-
- Only gains greater than an average of 1.00000 can hope to account
- for the net gain of 1.5E+8. And gains greater than, yet very
- nearly, 1.00000 are improbable due to the arbitrary geometry of
- the Pd cathode surface which presumably "leaks" doomed chain
- events.
-
- The only logical conclusion to be drawn is that the gain is
- greater than 1.0000 by some significant amount. But that leads to
- further requirements. If the event times are on the order of
- picoseconds, all the pending event opportunities will be consumed
- in a fraction of a second. If these be all the D's in the Pd
- lattice, we ought to have a serious nuclear explosion rather
- than tiny quantities of excess heat.
-
- I see two general possibilities to explain the absence of mushroom
- clouds in Orlando and Batavia.
-
- One is that at any given time there are only a very few pending
- event opportunities -- a fraction of the available D's. They all
- do go off in a very quick chain reaction flash, but their numbers
- are relatively small. A fraction of a second later after the
- previous flash, new event opportunities arise, and the relaxation
- oscillator can be triggered to fire again. Sort of like the early
- German V-1 "buzz bomb." (Depending upon the rate of relaxation,
- an RF "signature" might arise from this hypothetical mode.)
-
- A modification of this is to postulate that there is always a
- continuum of event opportunities appearing in the lattice, and
- these overlap the firing of their predecessors. The chain is
- controlled, then, by the rate of event opportunity creation, just
- as a rocket engine self-ignites new fuel. (This would be a
- continuous "burn" and might have no RF "signature.")
-
- The second possibility is that event opportunities can assume bi-
- stable states. One state is the ground state, and one state is
- the excited state. The excited state halflife is (apparently) on
- the order of minutes or hours -- if the statistics do actually
- show a "lag" effect.
-
- The problem with the bi-stable state theory is that it ought to
- still lead to a runaway condition, although the onset of such
- slowed to hours or days. There is no evidence yet of such an
- ongoing runaway condition. So I have to conclude that the bi-
- stable is not present, or is further controlled by some secondary
- mechanism. In any case the evidence is ambiguous.
-
- -- John Logajan
-