Wiki
Version 95 (Sean Logan, 06/19/2014 11:22 pm)
1 | 74 | Sean Logan | !https://opendesignengine.net/attachments/download/499/fountains-23.jpg! |
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3 | 41 | Sean Logan | |
4 | 83 | Sean Logan | *We are seeking:* |
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6 | 90 | Sean Logan | 1. Someone with a HackRF One or Jawbreaker, and a strong attenuator, to preform Spectral Analysis on the RF generated by this device. |
7 | 84 | Sean Logan | 2. Someone with HFSS or other Method of Moments simulation program, to model the E and B fields during a 10 kV, 10 pico- second discharge. We are particularly interested in how the B fields orientate within the resonant cavities, so we can best position the magnetic loop antennas. |
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9 | 85 | Sean Logan | If you would like to contribute in one of the capacities, please contact wam2358 aaatttt gmail dddddoooottttt com |
10 | 82 | Sean Logan | Thank you! |
11 | 83 | Sean Logan | |
12 | 94 | Sean Logan | *We encourage you to manufacture your own devices and experiment with the parameters.* |
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14 | 82 | Sean Logan | |
15 | 2 | Sean Logan | h1. Wave Articulation Matrix |
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17 | 70 | Sean Logan | The Wave Articulation Matrix is composed of concentric steel cylinders. The simplest design uses four cylinders. More sophisticated devices may have 6, 8, or any even number of cylinders. |
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19 | 71 | Sean Logan | Fig. 1.1: "Wave Articulation Matrix, 8-Element":https://opendesignengine.net/attachments/download/446/6frw2.jpg |
20 | 71 | Sean Logan | |
21 | 71 | Sean Logan | All the cylinders have the same mass, and the same surface area. |
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23 | 1 | Sean Logan | |
24 | 92 | Sean Logan | *23 April 2014:* |
25 | 92 | Sean Logan | Iron-Nickel alloys exist which have much higher Magnetic Permeability than steel. |
26 | 92 | Sean Logan | Co-Netic, |
27 | 92 | Sean Logan | supermalloy, |
28 | 92 | Sean Logan | supermumetal, |
29 | 92 | Sean Logan | nilomag, |
30 | 92 | Sean Logan | sanbold, |
31 | 92 | Sean Logan | Molybdenum permalloy, |
32 | 92 | Sean Logan | Sendust, |
33 | 92 | Sean Logan | M-1040, |
34 | 92 | Sean Logan | Hipernom, |
35 | 92 | Sean Logan | HyMu-80 and |
36 | 92 | Sean Logan | Amumetal. |
37 | 1 | Sean Logan | Plastic or ceramic cylinders can be Metalized with Iron-Nickel alloy. |
38 | 93 | Sean Logan | *End Note* |
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44 | 4 | Sean Logan | The length of the innermost cylinder is equal to the circumference of the outermost cylinder. The length of the outermost cylinder is equal to the circumference of the innermost. |
45 | 5 | Sean Logan | |
46 | 16 | Sean Logan | Fig. 1.2: "Physical Dimensions -- Side View -- 8-Element WAM":https://opendesignengine.net/attachments/download/439/side_dimensions.jpg |
47 | 16 | Sean Logan | Fig. 1.3: "Physical Dimensions -- Top View -- 8-Element WAM":https://opendesignengine.net/attachments/download/455/top-view.gif |
48 | 17 | Sean Logan | Fig. 1.4: "Perspective Views -- 8-Element WAM":https://opendesignengine.net/attachments/download/451/primary-axis2.jpg |
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50 | 46 | Sean Logan | The WAM can be described as a Log Periodic Nested Waveguide. It is Log Periodic, in that, the radius of each element (counting from the innermost element, outwards) is equal to that of the previous element, multiplied by a constant. Likewise, the length of each element (counting from the outermost element, inwards) is equal to that of the previous, multiplied by that constant. The constant we use (our base of logarithms) is the Golden Ratio. |
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52 | 58 | Sean Logan | In this document, this particular configuration will be referred to as The Fountain. |
53 | 49 | Sean Logan | |
54 | 58 | Sean Logan | A Log Periodic Dipole Array is Log Periodic in one dimension, so a curve traced through the tips of its elements is a logarithmic curve. The Fountain is Log Periodic in two dimensions simultaneously (radius, and length), so a curve traced through the bottom edges of its cylinders is a Hyperbola. |
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56 | 58 | Sean Logan | Fig. 1.5: "The Fountain is a Log Periodic Nested Waveguide":https://opendesignengine.net/attachments/download/477/log-periodic2.jpg |
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58 | 58 | Sean Logan | If we want to build a 4-element Fountain around a 0.75 inch diameter acetel rod, using 0.002 inch thick steel shim stock, then Lambda = 10.008 inch. |
59 | 58 | Sean Logan | |
60 | 58 | Sean Logan | Fig. 1.6: "Example Dimensions -- 4-Element Fountain":https://opendesignengine.net/attachments/download/453/4wam.jpg |
61 | 1 | Sean Logan | Fig. 1.7: "Photo of a 4 Element Fountain":https://opendesignengine.net/attachments/download/498/4-wam-proto.jpg |
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63 | 92 | Sean Logan | |
64 | 92 | Sean Logan | *Firing* |
65 | 92 | Sean Logan | Let's call the innermost cylinder the Anode. |
66 | 92 | Sean Logan | |
67 | 92 | Sean Logan | The steel cylinders surrounding the Anode are perceived as inductor cores by the magnetic flux, which circles the Anode when the Thyratron fires. The volumes of space between the cylinders are resonant cavities. RF is obtained from these cavities by magnetic loop antennas. |
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71 | 58 | Sean Logan | h1. Two Waves, Whose Frequencies are Consecutive Integer Powers of the Golden Ratio, Heterodyne in a Unique Way |
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73 | 55 | Sean Logan | Fig. 9.1: "Powers of the Golden Ratio":https://opendesignengine.net/attachments/download/450/golden-ratio-powers.gif |
74 | 55 | Sean Logan | Fig. 9.2: "...Heterodyne to Produce More Terms of the Series":https://opendesignengine.net/attachments/download/441/heterodyne.gif |
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79 | 75 | Sean Logan | h1. Casting Resonant Cavities in Epoxy |
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81 | 75 | Sean Logan | In a 4 Element Fountain, there are three resonant cavities. |
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83 | 75 | Sean Logan | Fig. 10.0: "There are three Resonant Cavities in a 4 Element Fountain":https://opendesignengine.net/attachments/download/500/cavities-resonant.jpg |
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85 | 75 | Sean Logan | Let's cast these volumes of space out of epoxy resin. |
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87 | 79 | Sean Logan | We will make urethane molds to cast in. The positives, from which the molds are made, are turned on a lathe from Acetel (Delrin). Here are the dimensions for the positives for the 4 element fountain with Lambda = 10.008 inches. |
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89 | 80 | Sean Logan | Fig. 10.1: "Positive for Mold, Cavity A":https://opendesignengine.net/attachments/download/504/positive_a.jpg |
90 | 80 | Sean Logan | Fig. 10.2: "Positive for Mold, Cavity B":https://opendesignengine.net/attachments/download/505/positive_b.jpg |
91 | 80 | Sean Logan | Fig. 10.3: "Positive for Mold, Cavity C":https://opendesignengine.net/attachments/download/506/positive_c.jpg |
92 | 80 | Sean Logan | Fig. 10.4: "Acetel Rod for Central Element":https://opendesignengine.net/attachments/download/507/positive_d.jpg |
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94 | 80 | Sean Logan | Fig. 10.5: "Epoxy sections and their dimensions":https://opendesignengine.net/attachments/download/508/mold.jpg |
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96 | 78 | Sean Logan | -Fig. 10.1: "Positives for Molds pt. 1":https://opendesignengine.net/attachments/download/502/positives-1.jpg |
97 | 78 | Sean Logan | Fig. 10.2: "Positives for Molds pt. 2":https://opendesignengine.net/attachments/download/503/positives-2.jpg- |
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99 | 81 | Sean Logan | The disc is to hold the central shaft centered within the mold while the epoxy cures. The positives are each about one inch taller than the actual epoxy pieces, so we have some room to work with and the molds don't overflow. |
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106 | 75 | Sean Logan | h1. Wiring Diagrams |
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110 | 1 | Sean Logan | Fig. 3.23: "New Wiring Diagram, 7-April-2014":https://opendesignengine.net/attachments/download/501/wiring-174.jpg |
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112 | 86 | Sean Logan | Notes: |
113 | 1 | Sean Logan | |
114 | 86 | Sean Logan | 1. The Anode may swing negative if the load resistor (the one at the top which the Anode discharges into) is not matched to the impedance of the Anode. The Anode, surrounded by the other steel cylinders, can be thought of as a transmission line, and it has a particular impedance. We want the resistor to match this impedance so there is no ringing when we discharge. For the resistor, it may be appropriate to use a bar of some resistive material, with a moveable contact that can slide along its length to choose a particular resistance. This may or may not be important. |
115 | 86 | Sean Logan | |
116 | 86 | Sean Logan | 2. The positive voltage on the Control Ring (the outermost cylinder is called the Control Ring) is what we're pushing against. It is the weight of your friend in the swing. You push her on the swing at regular intervals, hopefully as she's swinging *away* from you, and each time she goes higher and higher. If there's no one in the swing, and you try to push it, you'll just fall on your face. That's what would happen if the control ring was grounded. Then there'd be nothing to push against. The Anode and the Control Ring have to both be positive. But the Anode is like 10kV, while the Control Ring is only 12V. |
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118 | 76 | Sean Logan | |
119 | 75 | Sean Logan | The circuit used to excite the WAM is very similar to a RADAR Modulator. |
120 | 75 | Sean Logan | |
121 | 75 | Sean Logan | Fig. 3.0: "RADAR Modulator is very Similar to WAM Exciter":https://opendesignengine.net/attachments/download/479/RADAR23.jpg |
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125 | 75 | Sean Logan | Fig. 3.1: "Simple Wiring Diagram":https://opendesignengine.net/attachments/download/475/wiring-simple.jpg |
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127 | 1 | Sean Logan | Fig. 3.2: "Complete Wiring Diagram":https://opendesignengine.net/attachments/download/495/wiring-complete2.jpg |
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129 | 77 | Sean Logan | The Control Ring is tied to the low side of the switch. It is held at a positive low voltage, 12v. |
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131 | 75 | Sean Logan | |
132 | 75 | Sean Logan | Let's use a Hydrogen Thyratron, or Spark Gap as the switching mechanism. These devices switch from "OFF" to "ON" very quickly -- on the order of tens of pico seconds. Some fast IGBTs can switch in 20 - 50 nano seconds, but this is still 1000 times slower than a Thyratron. And a spark gap is even faster. |
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134 | 77 | Sean Logan | Why do we need such a fast switch? Theoretical: The switching time is directly proportional to the diameter of the first cylinder surrounding the Primary Axis. The Modes which this cylindrical waveguide can support are around 11 GHz for the 4-element WAM shown above. Larger structures would tolerate slower switching times. |
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143 | 51 | Sean Logan | h1. Assembly Instructions |
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145 | 70 | Sean Logan | *The method of construction documented here is obsolete. A superior method is to cast the volumes of space between the cylinders in epoxy. This new method will be documented here shortly.* |
146 | 70 | Sean Logan | |
147 | 69 | Sean Logan | _Note: We recommend using a 100 watt soldering iron to solder the steel cylinders._ |
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149 | 51 | Sean Logan | A 4-element prototype can be constructed, using 0.002 inch thick steel shim stock to form the cylinders. |
150 | 51 | Sean Logan | |
151 | 58 | Sean Logan | Fig. 8.0: "Physical Dimensions of a 4-element Fountain":https://opendesignengine.net/attachments/download/453/4wam.jpg |
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153 | 64 | Sean Logan | Begin by choosing a value for Lambda (how big you want your Fountain to be). All physical dimensions are derived from this value. You may wish to consider what diameters are available for the rod material which you will build your structure around. Then choose a lambda based on that. For example, we decided to use a 0.75 inch dia. Acetel rod, so our Lambda came out to be 10.008 inches. |
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155 | 52 | Sean Logan | Steel shim stock, 0.002 inch thick, is reasonable to work with. |
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157 | 51 | Sean Logan | Fig. 8.1: "0.002 inch thich Steel Shim Stock":https://opendesignengine.net/attachments/download/490/as_steel-shim.jpg |
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159 | 51 | Sean Logan | The shim stock can be measured, then cut with a utility knife. |
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161 | 51 | Sean Logan | Fig. 8.2: "Cut Steel Shim Stock with a Utility Knife":https://opendesignengine.net/attachments/download/485/as_cut-shim.jpg |
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163 | 53 | Sean Logan | You will cut out 4 rectangles of steel to roll up into cylinders. The "Circumference" of the cylinder, in Fig. 8.0, is the width of the rectangle. The "Length" is the length. |
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165 | 53 | Sean Logan | Remember that the steel has a grain to it. Cut your rectangles such that the grain runs in the direction which they roll up to form cylinders. |
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167 | 53 | Sean Logan | The meeting edges of the cylinder should be sanded with fine emery cloth to remove oxide layer. Then soldered together using high-acid flux and lead free silver solder. |
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169 | 51 | Sean Logan | Fig. 8.3: "Steel can be Soldered with a High Acid Flux":https://opendesignengine.net/attachments/download/488/as_silver-solder.jpg |
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171 | 64 | Sean Logan | You will need wooden spacer rings to hold the metal cylinders apart. We had ours laser-cut from good quality plywood. The "OD" and "ID" dimensions in Fig. 8.0 refer to the dimensions of these wooden rings. |
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173 | 51 | Sean Logan | Fig. 8.4: "Wooden Spacer Rings, Laser-Cut":https://opendesignengine.net/attachments/download/489/as_spacer-rings.jpg |
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175 | 51 | Sean Logan | Wrap the first steel rectangle around a dowel or rod and solder. This is cylinder number zero. We used a 12 inch length, 0.75 inch diameter Acetel (Delrin) rod for our prototype. |
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177 | 64 | Sean Logan | Next, wrap a thin layer of dielectric material (4 mil plastic sheeting) around the metal cylinder. The dielectric layer should be as long as the next metal cylinder, and flush with the top of the cylinders. (see Fig. 8.4.1, and Fig. 8.6). |
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179 | 64 | Sean Logan | Fig. 8.4.1: "Dielectric Layers":https://opendesignengine.net/attachments/download/497/dielectric-layers.jpg |
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181 | 64 | Sean Logan | Now, assemble the wooden spacer rings around the first cylinder, on top of the dielectric. You may wish to use cyanoacrylate glue (superglue) to keep everything in place and flush at the top. Water-based glues may not be ideal, due to their material characteristics at microwave frequencies. |
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183 | 67 | Sean Logan | Wrap the next steel rectangle around the wooden rings and solder. This is cylinder number one. This cylinder, and the next one, each get a wire soldered to them, which provides the output of the device. When cylinder one is all soldered, it will look like Fig. 8.5. Wrap a layer of dielectric around it, and it will look like Fig. 8.6. |
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185 | 51 | Sean Logan | Fig. 8.5: "The First Two Elements":https://opendesignengine.net/attachments/download/483/as_2-rings.jpg |
186 | 51 | Sean Logan | Fig. 8.6: "The First Two Elements, with Dielectric":https://opendesignengine.net/attachments/download/486/as_dielectric.jpg |
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188 | 51 | Sean Logan | Now assemble the next set of wooden spacer rings on top of the structure you have created thus far. It will look like this: |
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190 | 51 | Sean Logan | Fig. 8.7: "Two Completed Cylinders, with Spacer Rings Ready for Third":https://opendesignengine.net/attachments/download/491/as_wooden-rings.jpg |
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192 | 68 | Sean Logan | Wrap the next steel layer around the wooden rings and solder. Also solder to this cylinder a wire for output. Wrap dielectric around it. Put the next set of wooden rings around that. It will now look like this: |
193 | 51 | Sean Logan | |
194 | 51 | Sean Logan | Fig. 8.8: "Three completed Cylinders, with Spacer Rings Ready for Fourth":https://opendesignengine.net/attachments/download/492/as_wooden-rings2.jpg |
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196 | 51 | Sean Logan | Wrap the last steel layer on and solder. Now you are done. The last cylinder does not get a layer of dielectric. Here is your completed Fountain: |
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198 | 51 | Sean Logan | Fig. 8.9: "Four Completed Cylinders. You're Done!":https://opendesignengine.net/attachments/download/484/as_complete2.jpg |
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200 | 51 | Sean Logan | |
201 | 51 | Sean Logan | Notice that during the assembly, cylinders 1 and 2 had wires soldered on before the dielectric was wrapped around. These provide the output of the device. |
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213 | 9 | Sean Logan | h1. From a Golden Spiral to Gabriel's Horn |
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215 | 1 | Sean Logan | I would like to show you how the geometry of the Fountain can be derived from a Golden Spiral. |
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217 | 15 | Sean Logan | Let's take a look at a Golden Spiral. |
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219 | 10 | Sean Logan | Fig. 2.1: "A Golden Spiral":https://opendesignengine.net/attachments/download/447/golden-spiral3.gif |
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221 | 10 | Sean Logan | A Golden Spiral is a Logarithmic Spiral. Its radius multiplies by the Golden Ratio every quarter cycle. In Fig. 2.1, the Golden Ratio is written as the Greek letter Phi. |
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223 | 10 | Sean Logan | Just to make things simpler, let's have our Golden Spiral grow by a factor of Phi every complete cycle, instead of every quarter cycle. Let's also look at our spiral sideways, and allow it to exist in the dimension of time. Now what does it look like? |
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225 | 10 | Sean Logan | Fig. 2.2: "A Golden Spiral in Time":https://opendesignengine.net/attachments/download/448/golden-spiral-2.gif |
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227 | 21 | Sean Logan | The envelope of the wave on the right is an exponential curve; the amplitude of the wave is growing exponentially. |
228 | 21 | Sean Logan | |
229 | 21 | Sean Logan | Can our wave grow in any other way? Yes. Its frequency can grow as well as its amplitude. Let's make a wave where each time it completes one cycle, its amplitude has multiplied by the Golden Ratio, and its period has been divided by the Golden Ratio. Now what does our wave look like? |
230 | 22 | Sean Logan | |
231 | 1 | Sean Logan | Fig. 2.3: "A Golden Spiral with a Hyperbolic Envelope":https://opendesignengine.net/attachments/download/444/hyperbolic-wave.gif |
232 | 38 | Sean Logan | Fig. 2.3.1: "Explanation of the Logarithm Used in the Equation":https://opendesignengine.net/attachments/download/449/logarithm.gif |
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234 | 38 | Sean Logan | This wave has a hyperbolic envelope, not an exponential one, as before. |
235 | 38 | Sean Logan | |
236 | 38 | Sean Logan | We can also flip our wave around. This is perhaps the more general form of the equation. |
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238 | 38 | Sean Logan | Fig. 2.4: "A Golden Spiral with a Hyperbolic Envelope -- a Chirp":https://opendesignengine.net/attachments/download/458/wave.gif |
239 | 38 | Sean Logan | Fig. 2.4.1: "The Constant K Determines How Quickly the Wave Collapses":https://opendesignengine.net/attachments/download/457/enter-time1.jpg |
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241 | 22 | Sean Logan | If we rotate the envelope of this wave around the Z-axis, we create a Hyperboloid. |
242 | 37 | Sean Logan | |
243 | 63 | Sean Logan | Fig. 2.5: "Gabriel's Horn":https://opendesignengine.net/attachments/download/460/below.jpg |
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245 | 70 | Sean Logan | This Hyperboloid is known as Gabriel's Horn, because it looks like the trumpet blown by Archangel Gabriel on the Last Day. It has finite volume, yet infinite surface area. This is the correct shape of a vortex in water. |
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247 | 89 | Sean Logan | !http://fountain11235.files.wordpress.com/2014/04/water-vortex1.jpg! !http://fountain11235.files.wordpress.com/2014/04/trombaditorricelli1.gif! |
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249 | 1 | Sean Logan | The cylinders of the Fountain are formed by taking slices of Gabriel's Horn. |
250 | 70 | Sean Logan | |
251 | 70 | Sean Logan | Fig. 2.6: "Wave Articulation Matrix and Gabriel's Horn":https://opendesignengine.net/attachments/download/443/hyperboloid.gif |
252 | 70 | Sean Logan | Fig. 2.7: "Wave Articulation Matrix -- Perspective View":https://opendesignengine.net/attachments/download/438/beautiful.jpg |
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256 | 70 | Sean Logan | Gabriel's Horn is pertinent to Hyperbolic Geometry, and the work of N. I. Lobachevsky (Lobachevskii). |
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264 | 8 | Sean Logan | h1. Not a Steady State Device |
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266 | 6 | Sean Logan | The Fountain is not a steady state device. It is not excited by RF alternating currents. Rather, it is excited by Transients. |
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268 | 30 | Sean Logan | Fig. 4.1: "Transients vs. Steady State AC":https://opendesignengine.net/attachments/download/478/fig8.jpg |
269 | 30 | Sean Logan | |
270 | 30 | Sean Logan | For an excellent introduction on Transients, please see: |
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272 | 31 | Sean Logan | "Steinmetz, Charles Proteus, Elementary lectures on electric discharges, waves and impulses, and other transients":https://archive.org/details/elementarylectur00stei |
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276 | 38 | Sean Logan | h1. Pulsed DC, not AC |
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278 | 38 | Sean Logan | The Fountain is excited with pulsed DC, not AC. In a pulsed DC circuit, the magnetic field always spins the same direction. This is in contradistinction to the magnetic field in an AC circuit, which reverses direction repeatedly. |
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280 | 39 | Sean Logan | Fig 5.1: "The Magnetic Field in a Pulsed DC circuit Always Spins the Same Direction":https://opendesignengine.net/attachments/download/480/ac-dc.gif |
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283 | 91 | Sean Logan | The magnetic field has to spin in the same direction each time so we can get a vortex going. Imagine you're pushing on a flywheel. You want to push it the same way each time to get it going. If your flywheel was liquid instead of solid, then it would be a vortex. |
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286 | 87 | Sean Logan | *Maxwell's Equations are Fluid Dynamics* |
287 | 87 | Sean Logan | |
288 | 87 | Sean Logan | The people who gave us the mathematics to describe electrical phenomena were thinking in |
289 | 87 | Sean Logan | terms of Fluid Mechanics. Divergence and Curl are concepts from Fluid Mechanics. |
290 | 87 | Sean Logan | Tesla said, "Whatever Electricity may be, it behaves like an incompressible fluid." |
291 | 95 | Sean Logan | Water is an incompressible fluid. |
292 | 1 | Sean Logan | |
293 | 95 | Sean Logan | We're not talking about electrons in a wire. We're talking about the fields in space. The Electric and Magnetic fields. |
294 | 95 | Sean Logan | |
295 | 95 | Sean Logan | Divergence is the flow of a liquid into, or out of, a region of space. Electric Flux means electric flow. |
296 | 95 | Sean Logan | Curl is a description of the rotation or swirling of a fluid. The term rotation is used broadly; water flowing through a |
297 | 95 | Sean Logan | river, moving more quickly in the center of the river, is said to have vorticity. |
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301 | 87 | Sean Logan | One kind of phenomenon that can occur in a fluid is a wave. |
302 | 87 | Sean Logan | |
303 | 87 | Sean Logan | Another is a Vortex. |
304 | 87 | Sean Logan | |
305 | 87 | Sean Logan | A vortex in a fluid is shaped like a Hyperboloid called Gabriel's Horn. |
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307 | 1 | Sean Logan | |
308 | 88 | Sean Logan | Vorticity |
309 | 87 | Sean Logan | |
310 | 88 | Sean Logan | http://www.youtube.com/watch?v=loCLkcYEWD4 |
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312 | 87 | Sean Logan | |
313 | 87 | Sean Logan | *Test Question:* |
314 | 87 | Sean Logan | |
315 | 87 | Sean Logan | We have a copper rod with a small steel ring around it. |
316 | 87 | Sean Logan | The steel ring does not touch the rod. It rides on a plastic bearing |
317 | 87 | Sean Logan | and can spin freely. |
318 | 87 | Sean Logan | |
319 | 87 | Sean Logan | Use the copper rod to short the terminals of a very large capacitor that is fully charged. |
320 | 87 | Sean Logan | |
321 | 87 | Sean Logan | Does the steel ring spin? Why? |
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323 | 87 | Sean Logan | |
324 | 87 | Sean Logan | What if you had many capacitors, and you discharged one after another this way. |
325 | 1 | Sean Logan | What would happen then? |
326 | 87 | Sean Logan | |
327 | 88 | Sean Logan | Does the steel ring get magnetized? |
328 | 87 | Sean Logan | |
329 | 87 | Sean Logan | What if the rod was steel, would that change anything? |
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331 | 87 | Sean Logan | |
332 | 1 | Sean Logan | What if there were two rings instead of one, stacked inside each other. |
333 | 87 | Sean Logan | What would happen then? |
334 | 87 | Sean Logan | |
335 | 88 | Sean Logan | 23 pts. |
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349 | 38 | Sean Logan | h1. Discharge to Low Voltage, Not to Ground |
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351 | 38 | Sean Logan | In order to create the phenomenon, the following must be done: |
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353 | 38 | Sean Logan | 1. One plate of a capacitor is connected to Earth Ground. |
354 | 38 | Sean Logan | 2. The other plate is charged to a high positive voltage (300-600V). |
355 | 38 | Sean Logan | 3. The capacitor is rapidly discharged (through a spark gap, or thyratron) to a low positive voltage (12V). |
356 | 38 | Sean Logan | 4. The capacitor is charged up again, and the process repeats. |
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358 | 40 | Sean Logan | Fig. 6.1: "The Low Side of the Switch is Biased at +12v":https://opendesignengine.net/attachments/download/481/bias.gif |
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360 | 38 | Sean Logan | One terminal of the spark gap is connected to a conductor, which is connected to the high voltage plate of the capacitor. The other terminal of the spark gap is connected to the positive terminal of a 12v battery. The negative terminal of the battery is connected to Earth Ground. |
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366 | 38 | Sean Logan | h1. Transformation Between Extensive Space, and Gegenraum |
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368 | 38 | Sean Logan | Consider the concept of "Duality" in Projective Geometry, applied not to a particular solid, but to space itself. |
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370 | 38 | Sean Logan | Consider the transformation between the Infinite Plane (Euclidean Space), and the Point at Infinite Distance (Gegenraum). This transformation is represented by Gabriel's Horn. |
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372 | 1 | Sean Logan | See the Projective Geometry developed by George Adams and Rudolph Steiner. |
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374 | 40 | Sean Logan | Fig. 7.1: "Growth Measure from Gegenraum to Extensive Space":https://opendesignengine.net/attachments/download/454/gegenraum.jpg |
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378 | 33 | Sean Logan | h1. Recursive Process |
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380 | 56 | Sean Logan | We believe that a recursive process iterates once, each time the Fountain is charged and discharged. |
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384 | 5 | Sean Logan | !http://opendesignengine.net/dmsf_files/262?download=!:http://www.oshwa.org/definition/ |