Practical Guige to Free Energy Devices

use of any heating fuel. This next paragraph is for Engineers, so if you don’t understand it, then just ignore
it, as the important thing is to understand what the device does, rather than exactly how it does it.
The Heat-Pump Work Cycle: The example diagram above shows the sequence of events caused by the
rotation of the disc inside the device housing. This “Pressure / Enthalpy” or “Pressure / Internal-Energy”
diagram shows the pressures and temperatures during a single pressure cycle of the device. Using nitrogen
as the gas, the cycle starts at point “1” which has a pressure of 150 psi and a temperature of sixty degrees F.
A pressure wave now hits the mix of nitrogen and the liquid. This pressure wave moves us to point “2”
where the pressure has been boosted to 540 psi which raises the temperature to 280 degrees F.
Moving to point “3” is where the wanted heat is passed throughout the gas a the liquid (performing the
heating task which is the whole object of the exercise), even though the pressure is maintained, so at point
"3" there is a pressure of 540 psi and a temperature of 138 degrees F. Next, comes a major drop in
pressure, taking us to point “4” pulling the temperature down to below freezing: 250 psi at just 4 degrees F.
At point “5” the pressure is dropped further to 150 psi, still at 4 degrees F. Point “6” takes us to 250 psi at
60 degrees F from where the cycle takes us back to point “1”, and the sequence starts all over again.
The compression takes place on leg 1 to 2 and leg 5 to 6. The actual amounts are 53.2 and 13.5
respectively, giving a Compression Total of 66.7 B/lb.
The expansion takes place on leg 3 to 4, leg 4 to 5, and leg 6 to 1. The actual amounts are 31.6, 16.6 and
18.7 respectively, giving an Expansion Total of 67.0 B/lb.
As these two are virtually identical, the overall result of a complete cycle is effectively work-free.
This work cycle can be readily performed by the Centrifuge-Type Heat Pump. This is a unit which has only
one moving part, the rotor, the working fluid, such as nitrogen, is sealed in with the rotor and circulates in
passages in the rotor. The circulation of the working fluid inside the rotor is accomplished by density control
alone, in accordance with the work-cycle shown above, and there is no work input to the working fluid
from the rotor shaft. Thus the work input for the heat transfer is nil, and a work-free heat pump results.
In the diagram shown below, an axial cross-section and an end view with sections removed, shows a typical
heat pump rotor suitable for use with the work-cycle discussed above.
In the diagram, 10 is the heated-fluid heat exchanger, 11 is the heat-supply heat exchanger in two parts, and
12 are the vanes in passages which return the working fluid from the periphery to the centre of the disc. The
work cycle process is of the non-flow type for the working fluid in this rotor, and this provides higher
performance that that in the example shown above.
11 - 59