United States, Associate Fellow - Edward Mitchell

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Welcome to your new Lab space. You can start working on this space by editing this page. Tell everyone about your waterfuel research, what you're building, have built in the past, and how you hope to go about improving it next. You can add pictures in-line to illustrate your description, to depict your test setup, experiments, instrumentation, circuits, etc. The more you tell others about your work, the more they will want to post about theirs, and, before long, somebody will end up telling you that one piece of information you needed to get there first… ;-)

Version 1.5 last modified by David L. Wenbert, Executive Director The H2earth Institute on May 20, 2007 at 09:42 PDT. Initially created by David L. Wenbert, Executive Director The H2earth Institute.

Comments

Edward Mitchell – May 19, 2007 12:36 PST

This is where I will post most of my work on the water for fuel program. I will try and keep things neat and oderly but no promises.

Edward Mitchell – May 20, 2007 09:42 PST

The effects of a vacuum on electrolysis Here is the math of the process: at 1 ATM and 298K the energy requirments are; W = PΔV = (101.30 x 10^3 Pa)(1.5 moles)(22.4 x 10^-3 m^3/mol)(298K/273K) = 3.715 KJ (this is part A to B on the graph area under the curve)

At .2 ATM and 298k the energy requirments are; W = PΔV = (20.260 x 10^3 Pa)(1.5 moles)(22.4 x 10^-3 m^3/mol)(298K/273K) = 0.7431 KJ ( this is B to C on the graph area under the curve)

At .1 ATM and 298k the energy requirments are; W = PΔV = (10.130 x 10^3 Pa)(1.5 moles)(22.4 x 10^-3 m^3/mol)(298K/273K) = 0.3715 KJ (end of graph)

Notice the change in energy needed to break water down . And to think I figured this out all on my own, this is my addition too Faradays works.

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