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style="font-size:11.0pt;font-family:Georgia;color:black">F<sub>g</sub>
= -<span style="mso-spacerun:yes"> </span></span><span
style="font-size:11.0pt;font-family:Georgia;color:black"><span
style="mso-spacerun:yes"> </span><span
style="mso-spacerun:yes"> </span>φ –
(1/c)∂A<sub>g</sub>/∂t<span style="mso-spacerun:yes"> </span></span><span
style="font-size:11.0pt;font-family:Georgia;color:black"><span
style="mso-ignore:vglayout;position:
absolute;z-index:2;left:0px;margin-left:286px;margin-top:1px;width:14px;
height:16px"><span style="mso-ignore:vglayout;position:
absolute;z-index:2;left:0px;margin-left:286px;margin-top:1px;width:14px;
height:16px"></span></span>= <span style="mso-spacerun:yes"> </span></span><span
style="font-size:11.0pt;font-family:Georgia;color:black"><span
style="mso-spacerun:yes"><span
style="mso-ignore:vglayout;position:
absolute;z-index:2;left:0px;margin-left:286px;margin-top:1px;width:14px;
height:16px"></span> </span></span><span
style="font-size:11.0pt;font-family:Georgia;color:black"><span
style="mso-spacerun:yes"><span
style="mso-ignore:vglayout;position:
absolute;z-index:2;left:0px;margin-left:286px;margin-top:1px;width:14px;
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_x0000_s1033" height="16" width="14"></span> </span>-</span><span
style="mso-ignore:vglayout;position:
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style="font-size:11.0pt;font-family:Georgia;color:black"><span
style="mso-spacerun:yes"> </span></span><span
style="font-size:11.0pt;font-family:Georgia;color:black"><span
style="mso-spacerun:yes">
</span><span style="mso-spacerun:yes"></span>φ – (φ/c<sup>2</sup>)∂v/∂t<span
style="mso-tab-count:3"> </span>(2)<o:p></o:p></span></p>
<p class="MsoNormal"><span
style="font-size:11.0pt;font-family:Georgia;
color:black"><o:p> </o:p></span></p>
<p class="MsoNormal"><span style="font-size:10.0pt;color:black">Where
: φ = the
gravitational <span style="mso-tab-count:3">
</span>And
A<sub>g</sub> = (1/c) ∫(ρ∙<b style="mso-bidi-font-weight:normal">v</b>/r)
dV<o:p></o:p></span></p>
<p class="MsoNormal"><span style="font-size:10.0pt;color:black"><span
style="mso-tab-count:1"> </span><span
style="mso-spacerun:yes"> </span>c = the speed of light
const.<span style="mso-tab-count:2">
</span>Where: V = volume of
the Universe<o:p></o:p></span></p>
<p class="MsoNormal"><span style="font-size:10.0pt;color:black"><span
style="mso-tab-count:1"> </span><span
style="mso-spacerun:yes"> </span>v = the velocity of a test
mass<span style="mso-spacerun:yes"> </span><span
style="mso-tab-count:3"> </span>ρ<span
style="mso-spacerun:yes"> </span>=<span
style="mso-spacerun:yes"> </span>the
Universe mass density<o:p></o:p></span></p>
<p class="MsoNormal"><span style="font-size:10.0pt;color:black"><span
style="mso-tab-count:1"> </span><span
style="mso-spacerun:yes">
</span>A<sub>g</sub>=the sum over all mass currents<span
style="mso-spacerun:yes"> </span><span
style="mso-tab-count:2"> </span>v<span
style="mso-spacerun:yes"> </span>= the velocity vector of
the density<o:p></o:p></span></p>
<p class="MsoNormal"><span style="font-size:10.0pt;color:black"><span
style="mso-spacerun:yes"> </span><span
style="mso-tab-count:7">
</span>r<span style="mso-spacerun:yes"> </span>= the distance
to the test mass<o:p></o:p></span></p>
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<br>
<br>
<br>
Eq. 2 come from Sciama's work based upon Lorenz Relativity in which
a gravitational vector potential Ag is added to the gradient.<br>
Sciama assumed the time derivative sum could be solved by assuming
all masses in the universe flow in the opposite direction as the
particle of interest with velocity "v", this allows the required
summation to be carried out and reduced to the single time
derivative which is then the acceleration ascribed to inertia. What
this shows it that inertia is a gravitational interaction which is
also suggested by the Lense-Thirring Effect. When Einstein heard
about this he coined the phrase "Mach's principle" , but later Mach
criticized General Relativity and Einstein dropped the association.
<br>
<br>
Since the second term drops off as 1/r it is of much longer range
that the gravitational force which drops off as 1/r^2<br>
Thus when gravity imposes limits as to what we can see , the
possibility exists that multi-verse interaction from mass
influences local phenomena. Remember gravity is weak, but inertia is
what balances the electric force in Bohr's atomic model. So if we
recognize inertia as a force not an intrinsic static property of
particles, then random fluctuations due to quasi random motions of
universe masses could introduce random perturbations in orbits - and
the statistical nature f Quantum Mechancs would have an ontological
explanation.<br>
ERic Reiter (see paper from conference) suggests Sommerfelds Loading
Theory rather than photon in the EM field projection can be
demonstrated with his experiment. Loading theory says energy build
up in detectors randomly and EM waves push some detectors over the
top to fire randomly. Sommerfeld introduced the fine structure
constant relating electric and gravity, so random long range
inertial influences on top of loading theory would explain QM
statistics.<br>
<br>
I found Sciama's paper at
<p class="MsoNormal" style="margin-left:27.35pt;text-indent:-27.0pt"><span
style="font-size:10.0pt">[23] Sciama D. W., <span
style="mso-spacerun:yes"> </span>“On the Origin of Inertia”,
M.N.R.A.S.,
Vol.113, p.34, (1953)<o:p></o:p></span></p>
<p class="MsoNormal" style="margin-left:27.35pt"><span
style="font-size:
10.0pt;mso-ansi-language:SV" lang="SV">URL:
<a class="moz-txt-link-freetext" href="http://exvacuo.free.fr/div/Sciences/Dossiers/Gravite-Inertie-Mass/Inertie/Sciama/D%20W%20Sciama%20-%20On%20the%20origin%20of%20inertia.pdf">http://exvacuo.free.fr/div/Sciences/Dossiers/Gravite-Inertie-Mass/Inertie/Sciama/D%20W%20Sciama%20-%20On%20the%20origin%20of%20inertia.pdf</a><o:p></o:p></span></p>
<br>
I think I have a copy somewhere I can send you. <br>
<br>
Best<br>
Wolf<br>
<pre class="moz-signature" cols="72">Dr. Wolfgang Baer
Research Director
Nascent Systems Inc.
tel/fax 831-659-3120/0432
E-mail <a class="moz-txt-link-abbreviated" href="mailto:wolf@NascentInc.com">wolf@NascentInc.com</a></pre>
<div class="moz-cite-prefix">On 5/4/2016 9:35 AM, Hodge John wrote:<br>
</div>
<blockquote
cite="mid:1902794968.6309975.1462379705690.JavaMail.yahoo@mail.yahoo.com"
type="cite">
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font-family:HelveticaNeue, Helvetica Neue, Helvetica, Arial,
Lucida Grande, sans-serif;font-size:16px">
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<div id="yui_3_16_0_ym19_1_1462379656731_2617">Wolf</div>
<div id="yui_3_16_0_ym19_1_1462379656731_2618">Thanks for your
paper. </div>
<div id="yui_3_16_0_ym19_1_1462379656731_2619">Your Eq.2 appears
as a fluid flow. Please expand on your
treatment of the time derivative term. What effect would
differentiate your
model with other models? How could the time derivative be
effective in an
experiment? How would this term be different from merely
proportional to the
gradient term? Is the time derivative term like an
acceleration or velocity?</div>
<div id="yui_3_16_0_ym19_1_1462379656731_2620"> </div>
<div id="yui_3_16_0_ym19_1_1462379656731_2621">You suggest it
would be effective at larger distances.</div>
<div id="yui_3_16_0_ym19_1_1462379656731_2622">I ask because the
existence of the time derivative term is
the most problematical part of my STOE. I consider the “space”
(plenum) has a
substantive existence rather than being merely a backdrop for
matter to play
its role. Therefore, it should have some fluid flow
characteristics. However,
gravity potential seems to be only 1/r. In the analysis of
galaxy rotation
curves, I used the gradient without the time derivative term
despite the
outflow of matter (hydrogen and other stuff) on the rational
that the time
derivative term was proportional to the gradient (not an
acceleration). The
derivation of the photon trajectory in Young’s Experiment
simulation included a
similar assumption where the term was a velocity (not velocity
squared which
would render a turbulence in the flow) that rendered a
description of inertia
of space (plenum).<span
id="yui_3_16_0_ym19_1_1462379656731_2623"
style="mso-spacerun: yes"> </span></div>
<div id="yui_3_16_0_ym19_1_1462379656731_2624"> </div>
<div id="yui_3_16_0_ym19_1_1462379656731_2625">Hodge</div>
<div dir="ltr">
</div>
</div>
<br>
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