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Dan Davidson - Practical Guide to Free-Energy Devices

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a<strong>to</strong>ms than hydrogen so we can generalize and treat aether flow around<br />

in a<strong>to</strong>m as generally radial with flow either <strong>to</strong>ward or away from center<br />

of the a<strong>to</strong>m. If we look at the flows closely, we would find that these<br />

flows are vortexing or spinning in<strong>to</strong> and out of the nucleus. (See figure<br />

1.4.1-1)<br />

A complex a<strong>to</strong>m with many orders of aetheric<br />

stress vortex flows (lines).<br />

A simple a<strong>to</strong>m like hydrogen would have only<br />

one vortex line in and out.<br />

Figure 1.4.1-1. Cross Section of Vortex Stress Flows of<br />

Complex A<strong>to</strong>m.<br />

1.4.2 Shape Power of a Line<br />

The next level of geometric complexity is the line. In this instance we<br />

have an aggregated collection of a<strong>to</strong>ms <strong>to</strong> form a line (i.e., from 2 or<br />

more a<strong>to</strong>ms strung <strong>to</strong>gether <strong>to</strong> form a line).<br />

First, let us consider the aetheric flows around two a<strong>to</strong>ms next <strong>to</strong> each<br />

other which would be the simplest possible line. The aetheric flows in<br />

between the two a<strong>to</strong>ms would either connect and aether would flow from<br />

one a<strong>to</strong>m <strong>to</strong> the next or the flows would repel and the flows would squirt<br />

out perpendicular <strong>to</strong> the radial line between the two a<strong>to</strong>ms. The rest of<br />

aetheric flows would form a lozenge type radiation around the<br />

combination of the two a<strong>to</strong>ms.

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