Magnetic Domain

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Dale Basgall explores magnetic field strengths and speculates that understanding them may be important to LENR.

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Magnetic Domain 2:

Magnetic Domain 2 Field line strength Author Dale G. Basgall November 5, 2012

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Within the center of the graph there is a circle denoted in four sections as A and it is for reference in original scaling. The four square divisions within the center are 28-29-36-37 and are 1” X 1”. In this graph we will map the gauss in Y+ = 0 R+ and X+16. This is the side view of the 1” diameter 1/8 th thick magnet N52 . Y0+16 = 26.5 (N +)gauss (G):XO+16 = 16G @180.5 15 = 31.7 + 0degrees all 19.7 - + 180.8 14 = 38.5 + 24.5 - + 179.1 13 = 47.2 + 30.9 - + 180 12 = 58.7 + 40.2 - + 180.4 11 = 74.1 + 53.3 - + 180.2 10 = 95.2 + 72.7 - + 178.8 09 = 124.6 + 105.8 - + 179.7 08 = 166.4 + 160.1 - + 180.1 07 = 227.4 + 266.7 - + 179.9 06 = 317.9 + 514 - + 179.9 05 = 454.3 + 1336 - + 180 04 = 658.6 + 6003.9 - + 180.1 03 = 951.9 + = all .125” apart up. 02 = 1325 + = .125” from (01) 01 = 1682.1 + .0625” from surface N+ 0 = surface N from X0-Y0 = 1796.6 G The gauss measurements in this text can be found at KJ magnetics calculator. Measurements in the lab proved in fact that when using an expensive gauss meter and polarity tester the measurements are consistent with these factors. Regarding the rotation angle of measurement relative to vertical or Y axis both + and -. The gauss meter probe had cross hairs and a bronze machined surface which could be precisely positioned and held firm. Side view disk magnet 1” diameter X 1/8” thick. Use quadrant 57. start reference. 11/11/2012 2

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In this set of figures we are working on gathering 288 individual points of exact gauss per quadrant. Each Quadrant is identical in symmetry and mirrored in function. These measurements extend from 1 to 16 from center @.250” divisions. X extends horizontally and measures 0 G extended out and a fine line at 0 gauss. Total measureable gauss to 0 from the surface of the magnet gave results showing clearly that the equatorial axis is the longitudinal base for the domain field. The X axis extends angulated to 9” @.4G from surface, X axis @0 is 0G @ 9.1” and that Y axis extends without rotation 5” to 1.5G and @ 5.1” results 0G. When precisely positioned and focused the gauss meter indicates that a 0G line exists and extends along the X axis. This indicated a 0 gauss potential in the hemispherical center of a dipole or permanent block magnet. Keep in mind the sphere is where we need to end up at. 1. Y1-X1 = 1742.9G + @ 5.1 degrees : Y2-X1 = 1343.9 + @8.8 : Y3-X1 = 930.1G + @ 10.5 : Y4-X1 = 645.6 @ 10.9 X2 = 1956.7 + 12.6 1379.8 + 19.9 895.7 + 22.4 607.5 + 22.7 3. 2403.1 + 27.8 1365.8 + 37.2 815.5 + 37.4 538 + 35.7 4. 2584.6 + 72.7 1133.1 + 63 663.4 + 55.8 444.7 + 50.1 5. 1077.5 - 120 706.1 - 90.1 470.5 + 74.6 337.8 + 64.6 6. 479.3 - 139 401.2 - 101.8 309.3 - 90.6 242.8 + 78 7. 257.7 - 148.7 238.3 - 122.3 201.2 - 103.5 170.6 + 89.4 8. 157.4 - 154 149.7 - 131.5 134.8 - 113.5 120.5 - 99.3 9. 104.2 - 158.6 100.6 - 137.2 93.9 - 121.2 86.6 - 107.3 10. 73.5 - 159.7 71.5 - 143 66.9 - 127.8 63.8 - 114.1 11. 53.4 - 163.5 52.1 - 147.5 49.5 - 132.2 47.9 - 120.2 12. 40 - 165.3 39.2 - 150 37.7 - 136.6 37 - 124.8 13. 30.7 - 166 30.7 - 152.9 29.4 - 140.2 28 - 128.9 14. 24.4 - 166.5 24 - 155 23.6 - 142.7 23.5 - 132.5 15. 19.7 - 167.8 19.6 - 156.6 19.1 - 145.7 18.8 - 135.1 16. 16 - 168.9 16 - 158.7 15.7 - 148.9 15.7 - 138.2 11/11/2012 3

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Y5 – X1 = 446.8G + @ 10.8 : Y6 – X1 = 309 + @ 9.8 : Y7 – X1 = 222.7 + @ 9.4 : Y8 – X1 = 160.6 + @ 9.1 421.4 + 21.6 292 + 20.2 212.7 + 18.4 152.4 + 17.2 3. 374.7 + 32.2 261.6 + 30.2 190.9 + 27.8 140.2 + 26.1 314.7 + 45.1 228.4 + 41.4 166.8 + 37.6 126.4 + 34.6 251.1 + 57.1 185.4 + 52 142.2 + 47 108.8 + 43.1 187.6 + 68.7 146.1 + 61.2 118.4 + 55.7 92 + 51.5 141.4 + 79 116.1 + 70.4 94.4 + 64.2 76.8 + 59.2 106.3 + 88.3 88.7 + 79.6 77 + 77.2 63.2 + 66 79.1 - 95.9 69.1 + 86.8 61.2 + 79.1 51.4 + 72.8 59.8 - 103 53.2 - 93.9 48.2 + 85.7 42 + 79.2 45.5 - 109.3 41.6 - 99.8 38.5 - 91.8 34.2 + 84.7 35.8 - 114.8 33.1 - 105.1 31 - 96.8 28 - 90.9 28.6 - 118.9 26.6 - 109.6 25.1 - 102 23.1 - 95.4 22.8 - 123.1 22 - 113.8 20.9 - 106.3 19.2 - 99.6 18.8 - 126.3 17.9 - 118.1 17.6 - 109.9 16.1 - 103.3 15.4 - 129.6 14.7 - 122.3 14.4 - 115.1 13.6 - 107.6 After applying these figures to the Graph in slide 2 a pattern emerges, and this pattern extends above the North (+) face and to the right of center X axis 0 to 2” +X. These figures represent divisions of .125” one thru sixteen. Note that +X = right of center & –X is to the left of center 0. +Y = up from X0 and –Y is down from X0. +Z = from screen towards you from X0 & Y0. –Z = from screen away from you which is the depth and Z becomes the variable in the 2D view of the vector graph. Important to understand is that the specific field lines imaged are in a quadrant and on this graph include the division squares 37-38-39-40-41-42-43-44-53-54-55-56-57-58-59-60. Z axis is not present at this time, it will be added after the entire field line has been indicated in the 2d graph. These lines are imaged from the mechanical viewpoint contended by all claims in magnetic domain theory whereas the flux lines cross but do not inner mix together. For this reason specific gauss readings indicate flux line vector points. 11/11/2012 4

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Quadrant 57 has been cut from the graph in slide number 2. The magnetic product strength is measured in gauss which is a result of induced electrical current when the magnet was created. The X axis is measured at the surface and Y axis extends upward in divisions of .125” ending up at the 2” mark. The O gauss always remains throughout the fields meshing together. While using the expensive digital gauss meter the cross hairs on the probe could be angulated at any specific point to measure differentials in effective gauss usage. Important in these graphs is the exhibiting of a non-symmetrical domain field in relation to a sphere. This makes it possible to position objects that can be affected by different magnetic field strengths. The shape of the block that the magnetic product is forced into and created to be held or stored outlines what the domain field will look like after gauss is measured in all directions at all possible vertices within this vector graph. I feel that understanding better the magnetic domain and positions to access and bias that pinpoint a location where another element can be locked into suspension at a specific position, and thus making it possible to implement into LENR. 11/11/2012 5

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After removing the graph and using the 0 lines as reference divisions for gauss strength, the points of measurement resulted these field line images. At minimum this should raise questions regarding several issues of interest after experimenting hands on with these stored magnetic domain fields. I believe zero point energy liberation will end up in a magnetic understanding of how to actually use the zero points of magnetic gauss making it like a vice in a workshop for holding firmly magnetic particles. This zero potential is critical in friction reducing applications and also becomes evident after the proof of concept for the magnetic rail experiment. A question of mine was and also is still hounding me to understand better what the actual working possibilities of an isolated field point could be. One should question in fact as to how the magnet surface around the edges becomes so strong, and after documenting the gauss strengths on the graph what became of interest was the illusion of none of the lines come out to how we were taught and is imaged in a later slide. 11/11/2012 6

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Here is one of the biggest dipoles there is, the earth and it’s magnetosphere. The equator is there for a reason and this resembles a conventional view understanding of our earths magnetosphere. Above is a pick from what a conventional assumed magnetic field should look like. In reality on the magnet these flux lines do not cross the equator they enter at quadrants and above the equator for North and below the equator for South and depending on strength. An image above of the sun, a huge magnet and the earth the smaller magnet. If a solar storm or sunspot had a large enough magnetic pulse in amplitude (strength gauss) and hit our magnetosphere head on it could potentially re arrange the polarity of the earth and depending at what position the polarity was in when the pulse was emitted by the sun. One small comment on the North and South on the compass. In lab experiments when a polarity tester and gauss meter were used in conjunction with one another it clearly proved that when gauss on a magnet indicates north that a compass needle points to the south on the compass and when the meter indicates a south magnetic field on the magnet the compass indicates north. The inside geometry of this compass resembles what the fields actually appear to be. 11/11/2012 7

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This experimenting with the permanent block magnet has raised so many interesting observations I feel I know nothing now regarding the fields and their obvious symmetry to one another in quadrants but not in relation to a sphere or circular wheel of which mechanical issues usually always end up with circles of symmetry. Has anyone did this proof of concept above? Well I had to and I extended it 4feet with several hundred radio shack magnets. Used bar magnets, rectangle magnets, disk magnets but never the sphere. I had hold them but I ended up experimenting with them also in another proof of concept. I will follow up I didn’t get to take any pictures but I can draw them out. This operation worked well @ 1 foot, then at 2 with a little plastic and then 2 and a half feet with olive oil the plastic channel floor. Unique and interesting was the 0 gauss concept at the edges when opposed. 11/11/2012 8

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The follow up power point to this one will detail several experiments and questions that someone attempting to demonstrate to themselves the actual magnetic field gauss lines and how it becomes apparent that the fields have not been accurately pictured. At least there was not enough detail for serious advancement for the public trying to get permanent block magnets operating to liberate mechanically motionless electrical energy from the atmosphere. Just for a little fun and cheap proof of concept buy three 1” diameter X .125” thick magnets. hang a nail from the ceiling or a higher object about 3 feet tall. Put the magnet on the floor and raise it slowly until the nail is straight and solid and just touching the surface of the magnet North of S outh face. Why does the nail always want to go to the center of the face when that’s the weakest gauss on the surface. How do the edges accumulate more gauss than the center if the theory states the dipoles are aligned in a lattice formation? Take two of the magnets and get them to repel surfaces and make a black dot on each like face. Take your gauss meter and set your magnet to produce a specific gauss reading and place the nail close, it will be attracted but when you slide the other magnet closer with the same polarity the gauss biases and the net is zero friction on the nail, very interesting also. I will follow up on several more proof of concepts however I want to get into the migration of magnetic product. 11/11/2012 9

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With these power points I hope to convey a possibility I feel strongly about, that these dipoles are divided into quadrants and not a hemisphere as currently depicted by mainstream science. Also a torque factor can be used by holding a position in specific of the flowing elements within as the stored electrical energy or the magnetic product of induction on the primary level of creation for the magnet. Interesting also is that I have had different shapes cut out of regular magnets to see what the change is to the magnetic product and strength and what I had found is that a magnet is made out of material that can only be magnetized in a certain direction. After the block metal is saturated fully the gauss should equal the input current used to create the entire domain field of the magnet (dipole). The following slide is a picture of a rare magnet, it is rare because of how it is cut and the cost just to cut the magnet was $182.00 not counting the machine to make it that had to be special made and that also was pricey to get. In the next power point I will include pictures of an experiment using the face and side fields of a permanent disk magnet that acts like a ball bearing mechanical assembly. 11/11/2012 10

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Here is how deep the magnet cutting got, shapes that when assembled made solid magnetic wheels of different sizes rotating within one another. Each cut piece was $182.00 and with 16 per wheel that’s $2912.00 per wheel and we broke a few cause they were ground to .001” clearances. Nonetheless I have observed a magnet and it’s magnetic domain shift like something alive and healing. No matter how you cut what shape it always ends up with perfectly symmetrical field gauss lines, just proportionally weaker in pressure or magnetic gauss. Cut ½ the mass in any way and ½ the gauss is left. 11/11/2012 11

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