Volume 2 - LENR-CANR

More documents

Recommendations

Info

Electrical Breakeven from LANR Phusor Device Systems: Relative Limitations of Thermal Loss in Feedback Loop Mitchell Swartz JET Energy, Inc. Wellesley, MA 02481 (USA) Dr. Mitchell Swartz does not wish to have his papers uploaded to <strong>LENR</strong>-<strong>CANR</strong>.org. A copy of this paper can be found here: http://www.iscmns.org/iccf14/ProcICCF14b.pdf 689
Self-Polarisation of Fusion Diodes: From Excess Energy to Energy Fabrice David and John Giles Deuo Dynamics Moss Side House, East Blairdaff, Aberdeenshire, AB51 5LT. (UK) http://www.deuodynamics.com Abstract Conventionally, the cold fusion reaction produces heat. (1),(2) The authors have sought a different approach, wherein the device has no input energy, relying on the energy produced by cold fusion in the device. The device consists of diodes fabricated as powder, with a large surface junction made up of a semiconductor in contact with palladium charged with deuterium. The apparent fusion reactions take place in the junction between the semiconductor and the Palladium powder, which produces an excitation which is transmitted to the electrons. This excitation increases their energy and allows them to cross the bandgap of the semiconductor and pass into the conduction band, as in a photovoltaic cell. This energy very quickly appears as a spontaneous potential difference which can reach over 0.5 volt per junction. The potential drop concentrates on the junction region, and at a nano scale the electric field reaches considerable values, higher than the megavolt per meter, which constrains the deuterium nuclei and increases the probability of deuterium fusion. (3),(4) Experimental Device Diodes comprising of a stack of junctions were made, making it possible to obtain over 1 volt at the poles of a very compact device of a few centimetres long. The power generated by the device remains very low for the moment, but it should be noted that it is in the form of directly usable electrical energy, and not thermal energy. The authors compare the density of energy obtained in their device, with the density of energy released by the first atomic pile produced by Fermi in Chicago. The levels of energy are very comparable to the fusion diode. The authors describe the various devices experimented with and used during this work over the last two years. As part of this work, an extremely sensitive calorimetry device was built. The authors present the principle of this device, as well as a project for detecting of neutrons from very weak sources. This neutron counter records the particles emitted in all the directions of space, and can be scaled to the size of the neutron source. Our concept considers that before transforming itself into heat, the energy released by fusions of the deuterium initially will produce an excitation of the atoms. It is the same thing when a 696
Page 1 and 2:
Proceedings of the 14th Internation
Page 3 and 4:
Table of Contents VOLUME 1 Preface
Page 5 and 6:
Photon Measurements 326 Excess Heat
Page 7 and 8:
Investigation of Deuteron-Deuteron
Page 9 and 10:
Introduction to Cavitation Experime
Page 11 and 12:
Bubble Driven Fusion Roger Stringha
Page 13 and 14:
to the density of muon fusion syste
Page 15 and 16:
4.184 Joules/calorie to give Qo. No
Page 17 and 18:
References 1. M. P. Brenner, S. Hil
Page 19 and 20:
Experiments on stimulation of cavit
Page 21 and 22:
foil (thickness 0.1 mm) was situate
Page 23 and 24:
the external surface of thick wall
Page 25 and 26:
Introduction to Materials The outco
Page 27 and 28:
the foils, and the effects of subse
Page 29 and 30:
Material Science on Pd-D System to
Page 31 and 32:
level required higher current compa
Page 33 and 34:
morphology, and surface morphology
Page 35 and 36:
Figure 11. Evolution of the input a
Page 37 and 38:
Electrode Surface Morphology Charac
Page 39 and 40:
fundamental peak; on the other hand
Page 41 and 42:
RPSD@ max (x10 -32 m 4 ) 0.20 0.10
Page 43 and 44:
2. V. Violante, F. Sarto, E.Castagn
Page 45 and 46:
Experimental Starting with the meta
Page 47 and 48:
Figure 3.1. A typical database reco
Page 49 and 50:
palladium lot as received. Differen
Page 51 and 52:
Condensed Matter “Cluster” Reac
Page 53 and 54:
Loading Measurements A high-vacuum
Page 55 and 56:
Reaction Rate Estimates An estimate
Page 57 and 58:
References 1. Andrei Lipson, Brent
Page 59 and 60:
Introduction to the Theory Papers P
Page 61 and 62:
Foundations: Experimental Evidence,
Page 63 and 64:
Such results are applicable to a wi
Page 65 and 66:
electrostatic fields, that could ge
Page 67 and 68:
Theory Papers 1. V. Adamenko & V.I.
Page 69 and 70:
Figure 1. The general view and deta
Page 71 and 72:
So with a high probability the unkn
Page 73 and 74:
Potential energy of pair (without m
Page 75 and 76:
the corresponding electron wave fun
Page 77 and 78:
applicable in case of interaction o
Page 79 and 80:
The expression in the exponent of (
Page 81 and 82:
Empirical System Identification (ES
Page 83 and 84:
esults of the previous sections to
Page 85 and 86:
The higher the mass of a particle (
Page 87 and 88:
The Hubbard model [18, 19], along w
Page 89 and 90:
A B Figure 2. Atomic Arrangements o
Page 91 and 92:
deuterons, their interaction is aff
Page 93 and 94:
expected in D-D reactions is that w
Page 95 and 96:
It is being argued that, while heav
Page 97 and 98:
with odd permutations weighted by -
Page 99 and 100:
20. C. Elsasser, K.M. Ho, C.T. Chan
Page 101 and 102:
must have positive Bose Exchange sy
Page 103 and 104:
these different statements that ref
Page 105 and 106:
Fig.2 shows a pictorial representat
Page 107 and 108:
(a) A Pictorial Representation of V
Page 109 and 110:
esonance” can take place, in whic
Page 111 and 112:
interior boundaries of the ordered
Page 113 and 114:
Interface Model of Cold Fusion Talb
Page 115 and 116:
D + Bloch "atom" sublayer, 3) epita
Page 117 and 118:
sometimes stimulating an irreversib
Page 119 and 120:
Toward an Explanation of Transmutat
Page 121 and 122:
Given the well-established validity
Page 123 and 124:
The next question is, therefore, if
Page 125 and 126:
An Experimental Device to Test the
Page 127 and 128:
Figure 1. Palladium/deuterium total
Page 129 and 130:
Experimental Reaction enthalpies of
Page 131 and 132:
10. J. Dufour, X. Dufour, D. Murat
Page 133 and 134:
Together with the Coulomb-repulsion
Page 135 and 136:
“The Coulomb Barrier not Static i
Page 137 and 138:
2 16 2 gc 27 3 So, a solution for
Page 139 and 140:
Moreover, we study the “nuclear e
Page 141 and 142:
Then, according to the loading quan
Page 143 and 144:
Having mapped that the -phase depen
Page 145 and 146:
Considering the attractive force, d
Page 147 and 148:
The expression (45) was partially e
Page 149 and 150:
Table 1. Using the phase potential
Page 151 and 152:
10. A.De Ninno et al. Europhysics L
Page 153 and 154:
Fusion system still outperformed th
Page 155 and 156:
Van der Waals attraction occurs at
Page 157 and 158:
Quantum Fusion (QF) Quantum Fusion
Page 159 and 160:
Energy exchange There is some exper
Page 161 and 162:
of the weak coupling matrix element
Page 163 and 164:
Figure 3. Energy levels that contri
Page 165 and 166:
Input to Theory from Experiment in
Page 167 and 168:
substrate, and excess heat is obser
Page 169 and 170:
4. Laser stimulation Letts and Crav
Page 171 and 172:
energetic particles are produced, o
Page 173 and 174:
15. K. Kunimatsu, N. Hasegawa, A. K
Page 175 and 176:
A Theoretical Formulation for Probl
Page 177 and 178:
at some point we will require tools
Page 179 and 180:
3. Matrix element example The appro
Page 181 and 182:
Now the wavefunction on the RHS has
Page 183 and 184:
Theory of Low-Energy Deuterium Fusi
Page 185 and 186:
If mobile deuterons in a metal are
Page 187 and 188:
allowed since [Z1/m1] = [Z2/m2], an
Page 189 and 190:
traps (in 3g of Pd particles with a
Page 191 and 192:
9. S.N. Bose, Z. Phys. 26, 178 (192
Page 193 and 194:
system composed of host nuclei and
Page 195 and 196: A simple specific form of beff (p)
Page 197 and 198: Nuclear Transmutations in Polyethyl
Page 199 and 200: Furthermore, there are interesting
Page 201 and 202: The NT’s in phenanthrene [7] may
Page 203 and 204: explains why there is no neutron em
Page 205 and 206: T+T Fusion CrossSection (Barn) T+T
Page 207 and 208: science, the incident energy is so
Page 209 and 210: When the incident energy approaches
Page 211 and 212: 9. Chadwick, M. B., Oblozinsky, P.,
Page 213 and 214: He = Em C + m Cm + tmn (C + m Cm
Page 215 and 216: where k 2 = (2 Md Ea / ħ ) = Md 2
Page 217 and 218: y altering the shape of the Coulomb
Page 219 and 220: Analysis and Confirmation of the
Page 221 and 222: This is the basic Langevin equation
Page 223 and 224: The fusion rate is calculated by th
Page 225 and 226: EQPET molecule must go back and con
Page 227 and 228: Introduction to Challenges and Summ
Page 229 and 230: notes that the common usage of the
Page 231 and 232: insufficient to allow us to reprodu
Page 233 and 234: in the early days of semiconductors
Page 235 and 236: Water In Acrylic Toppiece Gas Tube
Page 237 and 238: Much of this uncertainty would be r
Page 239 and 240: Figure 5. The effect of input power
Page 241 and 242: maximum values. From these values w
Page 243 and 244: considerably that they were enginee
Page 245: Technogies”, in 11th Internationa
Page 249 and 250: We propose that in this field of on
Page 251 and 252: Results A. Self-sustained voltage O
Page 253 and 254: Figure 6. Differential calorimeter
Page 255 and 256: Weight of Evidence for the Fleischm
Page 257 and 258: Figure 1. Multiple support for a hy
Page 259 and 260: P(D | T) = P(T | D) P(D) / P(T) = 0
Page 261 and 262: For more information about Bayesian
Page 263 and 264: positive is in the range 0.980 ± 0
Page 265 and 266: With the notation Emn = “m heads
Page 267 and 268: 3.1. Selected papers Cravens and Le
Page 269 and 270: Table 3. P(Eif | Pf) Table 4. P(Ein
Page 271 and 272: Condensed Matter Nuclear Science”
Page 273 and 274: 4. J. Breese and D. Koller, “Tuto
Page 275 and 276: Taking the nuclear origin of copiou
Page 277 and 278: The evolution of protoscience into
Page 279 and 280: References 1. Mosier-Boss, P.A., et
Page 281 and 282: Cold fusion (CF) is a potentially r
Page 283 and 284: ISCMNS has initiated a CF-dedicated
Page 285 and 286: Table 2. Current Methods and Propos
Page 287 and 288: For the CF/OSSc project, the ISCMNS
Page 289 and 290: ole of skeptical mainstream physici
Page 291 and 292: sized Pd and Pd alloy particles. Ap
Page 293 and 294: Honoring Pioneers For most fields o
Page 295 and 296: A&Z introduced new terms to describ
Page 297 and 298:
The top portion of Fig. 3 shows plo
Page 299 and 300:
Figure 7. New catalyst shows nano-P
Page 301 and 302:
catalyst to outer vessel wall is 7
Page 303 and 304:
Establishment of the “Solid Fusio
Page 305 and 306:
Figure 1. Experimental Device Figur
Page 307 and 308:
[The protocol for producing the ZrO
Page 309 and 310:
Figure 5A. Comparison of generation
Page 311 and 312:
Figure 6. Gas pressure characterist
Page 313 and 314:
Note on Sources The Abstract is a r
Page 315 and 316:
37. Arata Y, Zhang Y-C; Proc. Japan
Page 317 and 318:
LENR Research using Co-Deposition S
Page 319 and 320:
that the tritium production was spo
Page 321 and 322:
(a) (b) (c) Figure 4. Images obtain
Page 323 and 324:
SPAWAR Systems Center-Pacific Pd:D
Page 325 and 326:
7. S. Szpak, P.A. Mosier-Boss, S.R.
Page 327 and 328:
17. S. Szpak, P.A. Mosier-Boss, and
Page 329 and 330:
Preparata Prize Acceptance Speech I
Page 331 and 332:
Cold Fusion Country History Project
Page 333 and 334:
2. “Condensed Matter Nuclear Scie
Page 335 and 336:
need for a coordinated effort in ma
Page 337 and 338:
Colloid J. USSR 48, 8(1986)). In 19
Page 339 and 340:
scientists on the problem of Cold F
Page 341 and 342:
Financial support for the conferenc
Page 343 and 344:
Author Index Pages are in Volume 1
Page 345:
Wang, J., 299 Watanabe, A., 338 Wei
show all

Volume 2 - LENR-CANR

You also want an ePaper? Increase the reach of your titles

Delete template?

Save as template?