VC-X
Vibration Cell
While my initial intrest in this type of system came from "Joe Cell"
research and experiment with Joe Cells, the
information contained in this document, is not based on the same
Orgone principles as the
traditional "Joe Cell". It is based on a tube
vibration system which can excite water. I have no
experience in using the water as a medium of intelligent manifesting,
and have considered "Y factor" a problem for most practical powering
systems, rather then a desirable interaction. The main goal has been
simply to assist running an engine using vibration science to reduce
inertia, increase power, and raise gas mileage.
Comprehensive Document - Vibration Tube Design

1 - The best V Cell, would have a perfect wavelength to fit each
tube, such that there is a perfect 2 x or 4 x down shift relationship
towards the next inner and outer tube
2 - The tube accuracy should not be greater then .001" as common
machinist tools do not exist to lathe any more accurately, so final
charts must be only to .001 digit placement for the machinist.
3 - The smallest wavelength should remain about the thickness of the tube or about .064" or greater if possible
4 - The polygon pattern on the tubes ends should be divisible by 2
5 - Tubes can be pushed to resonate off the center of their meat slightly, to make use of factory stock tubes
VC-Basic
Wavelength Coupling Spread Sheet
This kind of spread sheet can be used to spot natural 2x or 4x down shift functions between the different tube diameters.
The top line is the polygon structure. The first entry block is for a 12 sided polygon placed on a 4" tube.
Below this is another block for a 3" tube, below that for a 2" tube, and the bottom line is a 1" tube.
The 1" tube will not be up shifting so there is only one line of data for it, just it's FS length.
Block Layout:
Block Organization:
1 FS [Fractal Segment Length]
Tube 4"
1/4 FS
Tube 3"
1/2 FS
Tube 2"
Tube 1"
12x |
16x |
18x |
20x |
22x |
24x |
26x |
28x |
30x |
32x |
34x |
36x |
38x |
40x |
42x |
44x |
46x |
1.018453 |
0.767680 |
0.683306 |
0.615570 |
0.560009 |
0.513621 |
0.474312 |
0.440580 |
0.411320 |
0.385697 |
0.363076 |
0.342958 |
0.324950 |
0.308737 |
0.294063 |
0.280720 |
0.268534 |
0.254613 |
0.191920 |
0.170826 |
0.153892 |
0.140002 |
0.128405 |
0.118578 |
0.110145 |
0.102830 |
0.096424 |
0.090769 |
0.085739 |
0.081237 |
0.077184 |
0.073516 |
0.070180 |
0.067133 |
0.509226 |
0.383840 |
0.341653 |
0.307785 |
0.280004 |
0.256810 |
0.237156 |
0.220290 |
0.205660 |
0.192849 |
0.181538 |
0.171479 |
0.162475 |
0.154368 |
0.147031 |
0.140360 |
0.134267 |
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0.759634 |
0.572590 |
0.509657 |
0.459135 |
0.417694 |
0.383094 |
0.353775 |
0.328616 |
0.306791 |
0.287680 |
0.270808 |
0.255802 |
0.242370 |
0.230277 |
0.219333 |
0.209381 |
0.200291 |
0.189908 |
0.143148 |
0.127414 |
0.114784 |
0.104424 |
0.095774 |
0.088444 |
0.082154 |
0.076698 |
0.071920 |
0.067702 |
0.063951 |
0.060593 |
0.057569 |
0.054833 |
0.052345 |
0.050073 |
0.379817 |
0.286295 |
0.254829 |
0.229568 |
0.208847 |
0.191547 |
0.176888 |
0.164308 |
0.153396 |
0.143840 |
0.135404 |
0.127901 |
0.121185 |
0.115139 |
0.109666 |
0.104690 |
0.100146 |
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0.500815 |
0.377500 |
0.336009 |
0.302701 |
0.275379 |
0.252568 |
0.233238 |
0.216651 |
0.202263 |
0.189663 |
0.178539 |
0.168646 |
0.159791 |
0.151818 |
0.144603 |
0.138041 |
0.132049 |
0.125204 |
0.094375 |
0.084002 |
0.075675 |
0.068845 |
0.063142 |
0.058310 |
0.054163 |
0.050566 |
0.047416 |
0.044635 |
0.042162 |
0.039948 |
0.037955 |
0.036151 |
0.034510 |
0.033012 |
0.250407 |
0.188750 |
0.168005 |
0.151350 |
0.137690 |
0.126284 |
0.116619 |
0.108326 |
0.101131 |
0.094832 |
0.089270 |
0.084323 |
0.079896 |
0.075909 |
0.072301 |
0.069021 |
0.066025 |
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0.241996 |
0.182409 |
0.162361 |
0.146266 |
0.133064 |
0.122042 |
0.112702 |
0.104687 |
0.097734 |
0.091646 |
0.086271 |
0.081491 |
0.077212 |
0.073359 |
0.069873 |
0.066702 |
0.063807 |
Progression
Starting at the 12x polygon 4" tube, upper left block of numbers, we
slide down and notice the 1/2x length in red, also matches the 18x 3"
tube 1x FS to 3 digits accuracy.
Next we drop down to the 1/2x position and notice, on the 24x there is another wavelength match.
Two more jumps are found off this one now, to the one inch tube, one for a 4x down shift
at 46x polygon, and another on the 24x polygon, both likely
close enough to work.
Because the 46x polygon has a wavelength of .063807 and this rounds off
to .064" for the machinist, this is probably about as far down in wavelength we care
to go.
This is the the most basic, perfect down shift practical, I see in the numbers. It is an
overall down shift of 2 x 2 x 4 = 16 x [across to tops of the
tubes].
The frequencies perfectly fit the tubes! I did not find any matches on
smaller polygons worth mentioning, as most would be pushing the
vibration off the tubes edges to fit.
Tube Length Spreadsheet
The next spreadsheet, is to calculate some possible tube lengths for these polygons, and
also see how far off center we need to push the tubes vibration from
the center of the mass.
As I rounded off the smallest wavelength to .063" I noticed the
deviation from center all went negative a further distance, then if I
round off to .064" they all go positive by a lot less.
.064" is the best vibrational fit across all the tubes. The
deviation line shows how far off of center we are pushing the tube to
vibrate up.
Min and Max represent the inner and outer edges of the tubes meat, where the vibration will then totally miss the tube.
Our deviation appears to be acceptable, with this choice of wavelengths and tubes.
Min |
0.000000 |
0.000000 |
0.000000 |
0.000000 |
Center |
0.065000 |
0.065000 |
0.065000 |
0.065000 |
Max |
0.130000 |
0.130000 |
0.130000 |
0.130000 |
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Deviation |
0.002833 |
0.026292 |
0.013490 |
0.021432 |
New Center |
0.062167 |
0.038708 |
0.051510 |
0.043568 |
New Diam |
0.937833 |
1.961292 |
2.948490 |
3.956432 |
Wave Chg |
0.000193 |
0.003432 |
0.002343 |
0.005547 |
Center Seg |
0.063807 |
0.252568 |
0.509657 |
1.018453 |
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Polygon 46x |
Polygon 24x |
Polygon 18x |
Polygon 12x |
Cell 8 |
1” |
2” |
3” |
4” |
1x |
0.064 |
0.256 |
0.512 |
1.024 |
2x |
0.128 |
0.512 |
1.024 |
2.048 |
3xP |
0.192 |
0.768 |
1.536 |
3.072 |
4x |
0.256 |
1.024 |
2.048 |
4.096 |
5xP |
0.320 |
1.280 |
2.560 |
5.120 |
6x |
0.384 |
1.536 |
3.072 |
6.144 |
7xP |
0.448 |
1.792 |
3.584 |
7.168 |
8x |
0.512 |
2.048 |
4.096 |
8.192 |
9x |
0.576 |
2.304 |
4.608 |
9.216 |
10x |
0.640 |
2.560 |
5.120 |
10.240 |
11xP |
0.704 |
2.816 |
5.632 |
11.264 |
12x |
0.768 |
3.072 |
6.144 |
12.288 |
13xP |
0.832 |
3.328 |
6.656 |
13.312 |
14x |
0.896 |
3.584 |
7.168 |
14.336 |
15x |
0.960 |
3.840 |
7.680 |
15.360 |
16x |
1.024 |
4.096 |
8.192 |
16.384 |
17xP |
1.088 |
4.352 |
8.704 |
17.408 |
18x |
1.152 |
4.608 |
9.216 |
18.432 |
19xP |
1.216 |
4.864 |
9.728 |
19.456 |
20x |
1.280 |
5.120 |
10.240 |
20.480 |
21x |
1.344 |
5.376 |
10.752 |
21.504 |
22x |
1.408 |
5.632 |
11.264 |
22.528 |
23xP |
1.472 |
5.888 |
11.776 |
23.552 |
29xP |
1.856 |
7.424 |
14.848 |
29.696 |
31xP |
1.984 |
7.936 |
15.872 |
31.744 |
37xP |
2.368 |
9.472 |
18.944 |
37.888 |
41xP |
2.624 |
10.496 |
20.992 |
41.984 |
43xP |
2.752 |
11.008 |
22.016 |
44.032 |
47xP |
3.008 |
12.032 |
24.064 |
48.128 |
53xP |
3.392 |
13.568 |
27.136 |
54.272 |
59xP |
3.776 |
15.104 |
30.208 |
60.416 |
61xP |
3.904 |
15.616 |
31.232 |
62.464 |
67xP |
4.288 |
17.152 |
34.304 |
68.608 |
71xP |
4.544 |
18.176 |
36.352 |
72.704 |
73xP |
4.672 |
18.688 |
37.376 |
74.752 |
79xP |
5.056 |
20.224 |
40.448 |
80.896 |
83xP |
5.312 |
21.248 |
42.496 |
84.992 |
89xP |
5.696 |
22.784 |
45.568 |
91.136 |
97xP |
6.208 |
24.832 |
49.664 |
99.328 |
101xP |
6.464 |
25.856 |
51.712 |
103.424 |
103xP |
6.592 |
26.368 |
52.736 |
105.472 |
107xP |
6.848 |
27.392 |
54.784 |
109.568 |
109xP |
6.976 |
27.904 |
55.808 |
111.616 |
113xP |
7.232 |
28.928 |
57.856 |
115.712 |
127xP |
8.128 |
32.512 |
65.024 |
130.048 |
131xP |
8.384 |
33.536 |
67.072 |
134.144 |
137xP |
8.768 |
35.072 |
70.144 |
140.288 |
139xP |
8.896 |
35.584 |
71.168 |
142.336 |
149xP |
9.536 |
38.144 |
76.288 |
152.576 |
151xP |
9.664 |
38.656 |
77.312 |
154.624 |
157xP |
10.048 |
40.192 |
80.384 |
160.768 |
163xP |
10.432 |
41.728 |
83.456 |
166.912 |
167xP |
10.688 |
42.752 |
85.504 |
171.008 |
173xP |
11.072 |
44.288 |
88.576 |
177.152 |
179xP |
11.456 |
45.824 |
91.648 |
183.296 |
181xP |
11.584 |
46.336 |
92.672 |
185.344 |
191xP |
12.224 |
48.896 |
97.792 |
195.584 |
193xP |
12.352 |
49.408 |
98.816 |
197.632 |
197xP |
12.608 |
50.432 |
100.864 |
201.728 |
199xP |
12.736 |
50.944 |
101.888 |
203.776 |
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Now from the table above, choose a set of lengths having the qualities you desire.
Consider both even down shift length drop the frequency again, and prime counts hold the higher fractal consistently.
I have omitted many
possible numbers in favor of the primes on the first two tubes.
However do not feel limited. It is possible to now make a cell with all
4 tubes the exact same length if the chart above is completed.
Look at the number 1.024" On each tube. 4" 16x - 3" 4x - 2" 2x - 1" 1x
A cell built like this is going to work, but the center tube will
down shift 16x before the energy hits the 2nd tube, where it will now
up shift back to 2x???
This is likely not a desirable pattern for creating Aetheric pressure,
however the tubes will have perfect alignment of the waves down them
top to bottom.
VC-16
|
Polygon 46x |
Polygon 24x |
Polygon 18x |
Polygon 12x |
Cell 8 |
1” |
2” |
3” |
4” |
89xP |
5.696 |
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23xP |
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5.888 |
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13xP |
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6.656 |
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7xP |
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7.168 |
Notes:
All prime stacks used, for square pattern frequency alignment.
After assembly, the tubes should couple well all the way to the bottom end!
VC-128
|
Polygon 46x |
Polygon 24x |
Polygon 18x |
Polygon 12x |
Cell 9 |
1” |
2” |
3” |
4” |
89xP |
5.696 |
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23xP |
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5.888 |
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14x |
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7.168 |
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8x |
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8.192 |
Notes:
Now stretching the 2 outer tubes a bit to increase the final down shift wavelength.
An 8x will down shift 8x! Shooting the cell up to a pure 128x harmonic.
Dave L
12 / 27 / 2011
www.ResonantFractals.org