[Vo]:Re:Some fusion reaction tables of possible interest
B, Ag, and C now added to the equation collection: http://www.mtaonline.net/~hheffner/B_LENR.pdf http://www.mtaonline.net/~hheffner/AgLENR.pdf http://www.mtaonline.net/~hheffner/C_LENR.pdf Best regards, Horace Heffner http://www.mtaonline.net/~hheffner/
[Vo]:Re:Some fusion reaction tables of possible interest
Nb, Ag, Ta, W, Mo, V, Ba, and U now added to the equation collection: http://www.mtaonline.net/~hheffner/NbLENR.pdf http://www.mtaonline.net/~hheffner/AgLENR.pdf http://www.mtaonline.net/~hheffner/TaLENR.pdf http://www.mtaonline.net/~hheffner/W_LENR.pdf http://www.mtaonline.net/~hheffner/MoLENR.pdf http://www.mtaonline.net/~hheffner/V_LENR.pdf http://www.mtaonline.net/~hheffner/BaLENR.pdf http://www.mtaonline.net/~hheffner/U_LENR.pdf The U allows for limited radioactive products. Still amazing how few products are feasible. Best regards, Horace Heffner http://www.mtaonline.net/~hheffner/
[Vo]:Re:Some fusion reaction tables of possible interest
The full picture has not yet emerged. The reactions in which the deflated electron binding energy exceeds the fusion energy are high probability candidates for weak reactions, due to the longevity of the initial fused nucleus, and the prolonged presence of the electrons. The electrons decrease the stability of the neutrons, thus enhancing the probability of neutron beta decay. In some cases the probability of electron capture is also increased. Most important to confirmation of the deflation fusion theory, reactions with very negative net energy (in brackets), but positive fusion energy, are the best candidates for strange exchange reactions and K0 production. These heavy LENR reactions are fostered by use of extreme magnetic field gradients, which can be imposed by ambient fields, or better by powerful coherent EM radiation. Some examples of such reactions are: 90Zr40 + D -- 71Ga31 + 21Ne10 + 00.236 MeV [-11.772 MeV] ( 1 ) 90Zr40 + D -- 91Zr40 + 1H1 + 4.970 MeV [-7.038 MeV] ( 2 ) 90Zr40 + 2 D -- 68Zn30 + 26Mg12 + 23.722 MeV [-0.720 MeV] ( 9 ) 90Zr40 + 2 D -- 70Zn30 + 24Mg12 + 20.996 MeV [-3.446 MeV] ( 10 ) 90Zr40 + 2 D -- 71Ga31 + 23Na11 + 17.170 MeV [-7.272 MeV] ( 11 ) 90Zr40 + 2 D -- 72Ge32 + 22Ne10 + 18.113 MeV [-6.329 MeV] ( 12 ) 90Zr40 + 2 D -- 73Ge32 + 21Ne10 + 14.533 MeV [-9.909 MeV] ( 13 ) 90Zr40 + 2 D -- 74Ge32 + 20Ne10 + 17.968 MeV [-6.474 MeV] ( 14 ) 90Zr40 + 2 D -- 75As33 + 19F9 + 12.024 MeV [-12.418 MeV] ( 15 ) 90Zr40 + 2 D -- 76Se34 + 18O8 + 13.538 MeV [-10.904 MeV] ( 16 ) 90Zr40 + 2 D -- 77Se34 + 17O8 + 12.911 MeV [-11.531 MeV] ( 17 ) 90Zr40 + 2 D -- 78Se34 + 16O8 + 19.266 MeV [-5.176 MeV] ( 18 ) 90Zr40 + 2 D -- 79Br35 + 15N7 + 13.470 MeV [-10.972 MeV] ( 19 ) 90Zr40 + 2 D -- 82Kr36 + 12C6 + 18.092 MeV [-6.350 MeV] ( 20 ) 90Zr40 + 2 D -- 90Zr40 + 4He2 + 23.847 MeV [-0.595 MeV] ( 21 ) 90Zr40 + 2 D -- 91Zr40 + 3He2 + 10.464 MeV [-13.978 MeV] ( 22 ) 90Zr40 + 2 D -- 93Nb41 + 1H1 + 17.423 MeV [-7.019 MeV] ( 23 ) 90Zr40 + 2 D -- 94Mo42 + 25.914 MeV [1.472 MeV] ( 24 ) 42Ca20 + D -- 40K19 + 4He2 + 5.699 MeV [-1.979 MeV] ( 26 ) 42Ca20 + D -- 43Ca20 + 1H1 + 5.708 MeV [-1.970 MeV] ( 27 ) 46Ti22 + D -- 47Ti22 + 1H1 + 6.653 MeV [-1.552 MeV] ( 1 ) 46Ti22 + 2 D -- 26Mg12 + 24Mg12 + 12.293 MeV [-4.629 MeV] ( 3 ) 46Ti22 + 2 D -- 27Al13 + 23Na11 + 8.872 MeV [-8.051 MeV] ( 4 ) 46Ti22 + 2 D -- 28Si14 + 22Ne10 + 11.662 MeV [-5.261 MeV] ( 5 ) 46Ti22 + 2 D -- 29Si14 + 21Ne10 + 9.772 MeV [-7.151 MeV] ( 6 ) 46Ti22 + 2 D -- 30Si14 + 20Ne10 + 13.621 MeV [-3.302 MeV] ( 7 ) 46Ti22 + 2 D -- 31P15 + 19F9 + 8.074 MeV [-8.849 MeV] ( 8 ) 46Ti22 + 2 D -- 32S16 + 18O8 + 8.944 MeV [-7.979 MeV] ( 9 ) 46Ti22 + 2 D -- 33S16 + 17O8 + 9.541 MeV [-7.382 MeV] ( 10 ) 46Ti22 + 2 D -- 34S16 + 16O8 + 16.814 MeV [-0.109 MeV] ( 11 ) 46Ti22 + 2 D -- 35Cl17 + 15N7 + 11.057 MeV [-5.865 MeV] ( 12 ) 46Ti22 + 2 D -- 38Ar18 + 12C6 + 16.861 MeV [-0.062 MeV] ( 13 ) 46Ti22 + 2 D -- 39K19 + 11B5 + 7.285 MeV [-9.638 MeV] ( 14 ) 46Ti22 + 2 D -- 40K19 + 10B5 + 3.630 MeV [-13.293 MeV] ( 15 ) 46Ti22 + 2 D -- 46Ti22 + 4He2 + 23.847 MeV [6.924 MeV] ( 16 ) 46Ti22 + 2 D -- 47Ti22 + 3He2 + 12.146 MeV [-4.776 MeV] ( 17 ) Zr is most interesting because both Zr + D reactions are weak reaction candidates. All the above kinds of candidate reactions must be re-worked to include weak reaction prospects. Best regards, Horace Heffner http://www.mtaonline.net/~hheffner/
[Vo]:Re:Some fusion reaction tables of possible interest
Oxygen should not be overlooked as a powerful weak reaction candidate: 16O8 + D -- 14N7 + 4He2 + 3.111 MeV [-1.026 MeV] ( 1 ) 16O8 + D -- 17O8 + 1H1 + 1.919 MeV [-2.218 MeV]( 2 ) 16O8 + 2 D -- 14N7 + 6Li3 + 4.585 MeV [-4.402 MeV] ( 3 ) 16O8 + 2 D -- 17O8 + 3He2 + 7.412 MeV [-1.575 MeV] ( 5 ) Best regards, Horace Heffner http://www.mtaonline.net/~hheffner/
[Vo]:Re:Some fusion reaction tables of possible interest
The recent examination of deflation fusion scenarios indicate high voltage Zr electrolysis in the blue-green glow range may be useful to look for weak reactions and strange matter creation. I have run Zr electrode pairs in AC electrospark experiments at over 400 V. The breakdown voltage for conditioned electrodes was observed to be in the 280-320 V range. It is important to never exceed breakdown voltage to run in the glow range. It is important to slowly condition Zr so as to avoid going into the electrospark range and thus destroying the Zr electrodes. See: http://www.mtaonline.net/~hheffner/GlowExper.pdf For an example of what not to do, i.e. push power before conditioning so as to go into an electrospark range, instead of a glow range, and destroy the ZrO surface by perforating it, see: http://www.mtaonline.net/~hheffner/OrangeGlow.pdf A useful electrolyte might be obtained using either saturated pickling lime, i.e. CaO, or boric acid. Alternating between acidic and basic electrolytes may be useful for long term running. Current can be controlled using a two cells in series system, one with low conductivity to act only as a resister, that resistance varied by adding salts, the other being the live cell. Glow activity, as well as LENR, may produce UV or EUV. Dyes, such as fluorescein or rhodamine 6G, may be useful for observing or photographing active areas, and developing a conditioning protocol. After long running in a glow regime, the Zr electrodes can be heated in a vacuum as a HV anode, in order to emit atoms for accelerating to a target at voltages of 10 keV or more. If high energy reactions are observed in the target are then this wold be a possible indication of strange matter creation. Best regards, Horace Heffner http://www.mtaonline.net/~hheffner/
[Vo]:Re:Some fusion reaction tables of possible interest
The following tables now include more reaction equations, an extra energy entry for fusion energy minus deflated electron binding energy, and some typo corrections: http://www.mtaonline.net/~hheffner/ZrLENR.pdf http://www.mtaonline.net/~hheffner/PdLENR.pdf http://www.mtaonline.net/~hheffner/AlLENR.pdf http://www.mtaonline.net/~hheffner/NiLENR.pdf http://www.mtaonline.net/~hheffner/TiLENR.pdf http://www.mtaonline.net/~hheffner/CaLENR.pdf Something I find very interesting is the way lattice elements can act in a purely catalytic fashion. Some examples follow. 27Al13 + 2 D -- 29Si14 + 2H1 + 17.833 MeV [5.753 MeV] ( 11 ) 27Al13 + 2 D -- 30Si14 + 1H1 + 26.218 MeV [14.138 MeV] ( 12 ) 27Al13 + 5 D -- 27Al13 + 10B5 + 53.628 MeV [19.056 MeV]( 42 ) 27Al13 + 6 D -- 27Al13 + 12C6 + 78.814 MeV [35.652 MeV]( 52 ) 40Ca20 + 2 D -- 40Ca20 + 4He2 + 23.847 MeV [7.723 MeV] ( 4 ) 40Ca20 + 6 D -- 40Ca20 + 12C6 + 78.814 MeV [24.349 MeV]( 17 ) 40Ca20 + 8 D -- 40Ca20 + 16O8 + 109.822 MeV [33.305 MeV] ( 22 ) 58Ni28 + 2 D -- 58Ni28 + 4He2 + 23.847 MeV [3.986 MeV] ( 13 ) 58Ni28 + 3 D -- 58Ni28 + 6Li3 + 25.321 MeV [-5.173 MeV]( 20 ) 58Ni28 + 5 D -- 58Ni28 + 10B5 + 53.628 MeV [00.501 MeV]( 36 ) 46Ti22 + D -- 47Ti22 + 1H1 + 6.653 MeV [-1.552 MeV]( 1 ) 46Ti22 + 2 D -- 46Ti22 + 4He2 + 23.847 MeV [6.924 MeV] ( 16 ) 46Ti22 + 2 D -- 47Ti22 + 3He2 + 12.146 MeV [-4.776 MeV]( 17 ) 46Ti22 + 3 D -- 46Ti22 + 6Li3 + 25.321 MeV [-0.822 MeV]( 28 ) 102Pd46 + 2 D -- 102Pd46 + 4He2 + 23.847 MeV [-3.072 MeV] ( 44 ) 102Pd46 + 3 D -- 102Pd46 + 6Li3 + 25.321 MeV [-15.660 MeV] ( 59 ) 90Zr40 + D -- 91Zr40 + 1H1 + 4.970 MeV [-7.038 MeV]( 2 ) 90Zr40 + 2 D -- 90Zr40 + 4He2 + 23.847 MeV [-0.595 MeV]( 21 ) 90Zr40 + 2 D -- 91Zr40 + 3He2 + 10.464 MeV [-13.978 MeV] ( 22 ) 90Zr40 + 3 D -- 90Zr40 + 6Li3 + 25.321 MeV [-11.974 MeV] ( 33 ) What is interesting about this is the lattice elements are much closer to the hydrogen than other hydrogen atoms. If the hydrogen is in the deflated state, it is much more probable it will tunnel to a lattice nucleus. The lattice nucleus can thus act as a catalyst for multiple simultaneous deuteron reactions which would otherwise not be feasible under less than extreme loading conditions. Best regards, Horace Heffner http://www.mtaonline.net/~hheffner/
[Vo]:Re:Some fusion reaction tables of possible interest
Here is a corrected sample list of some heavy LENR catalytic reactions: 27Al13 + 2 D -- 27Al13 + 4He2 + 23.847 MeV [11.767 MeV]( 10 ) 27Al13 + 5 D -- 27Al13 + 10B5 + 53.628 MeV [19.056 MeV]( 42 ) 27Al13 + 6 D -- 27Al13 + 12C6 + 78.814 MeV [35.652 MeV]( 52 ) 40Ca20 + 2 D -- 40Ca20 + 4He2 + 23.847 MeV [7.723 MeV] ( 4 ) 40Ca20 + 6 D -- 40Ca20 + 12C6 + 78.814 MeV [24.349 MeV]( 17 ) 40Ca20 + 8 D -- 40Ca20 + 16O8 + 109.822 MeV [33.305 MeV] ( 22 ) 58Ni28 + 2 D -- 58Ni28 + 4He2 + 23.847 MeV [3.986 MeV] ( 13 ) 58Ni28 + 3 D -- 58Ni28 + 6Li3 + 25.321 MeV [-5.173 MeV]( 20 ) 58Ni28 + 5 D -- 58Ni28 + 10B5 + 53.628 MeV [00.501 MeV]( 36 ) 46Ti22 + D -- 47Ti22 + 1H1 + 6.653 MeV [-1.552 MeV]( 1 ) 46Ti22 + 2 D -- 46Ti22 + 4He2 + 23.847 MeV [6.924 MeV] ( 16 ) 46Ti22 + 2 D -- 47Ti22 + 3He2 + 12.146 MeV [-4.776 MeV]( 17 ) 46Ti22 + 3 D -- 46Ti22 + 6Li3 + 25.321 MeV [-0.822 MeV]( 28 ) 102Pd46 + 2 D -- 102Pd46 + 4He2 + 23.847 MeV [-3.072 MeV] ( 44 ) 102Pd46 + 3 D -- 102Pd46 + 6Li3 + 25.321 MeV [-15.660 MeV] ( 59 ) 90Zr40 + D -- 91Zr40 + 1H1 + 4.970 MeV [-7.038 MeV]( 2 ) 90Zr40 + 2 D -- 90Zr40 + 4He2 + 23.847 MeV [-0.595 MeV]( 21 ) 90Zr40 + 2 D -- 91Zr40 + 3He2 + 10.464 MeV [-13.978 MeV] ( 22 ) 90Zr40 + 3 D -- 90Zr40 + 6Li3 + 25.321 MeV [-11.974 MeV] ( 33 ) What is interesting about this is the lattice elements are much closer to the hydrogen than other hydrogen atoms. If the hydrogen is in the deflated state, it is much more probable it will tunnel to a lattice nucleus. The lattice nucleus can thus act as a catalyst for multiple simultaneous deuteron reactions which would otherwise not be feasible under less than extreme loading conditions. Best regards, Horace Heffner http://www.mtaonline.net/~hheffner/
[Vo]:Re:Some fusion reaction tables of possible interest
The following style graphic is now available for Zr, Pd, Al, Ni, Ti, and Ca: Energetically Feasible Ca LENR Reactions Creating Only Stable Products Combined Fusion Product Data for Ca + n D reactions Relative Percent Abs. 0 10 20 30 40 50 60 70 80 90 100 Z Percent El.||||||||||| 1 8.389 H |** 2 12.027 He |* 3 2.347 Li |** 4 1.035 Be |* 5 1.729 B | 6 3.716 C | 7 2.033 N |* 8 4.156 O |* 9 00.644 F | 10 2.862 Ne | 11 1.246 Na |** 12 4.638 Mg |*** 13 00.631 Al | 14 3.767 Si | 15 00.842 P | 16 4.983 S |* 17 1.662 Cl | 18 1.784 Ar | 19 4.451 K |*** 20 11.866 Ca | 21 9.751 Sc | 22 12.624 Ti | *** 23 1.554 V |*** 24 1.263 Cr |** ||||||||||| 0 10 20 30 40 50 60 70 80 90 100 Note: the above data excludes fusion with more than 4 D. It is weighted by source isotope abundance, the square of the ratio of fusion energy to deflated hydrogen binding energy, and inversely as the square of the number of deuterons fused. This graph type is located on the last pages of: http://www.mtaonline.net/~hheffner/ZrLENR.pdf http://www.mtaonline.net/~hheffner/PdLENR.pdf http://www.mtaonline.net/~hheffner/AlLENR.pdf http://www.mtaonline.net/~hheffner/NiLENR.pdf http://www.mtaonline.net/~hheffner/TiLENR.pdf http://www.mtaonline.net/~hheffner/CaLENR.pdf Best regards, Horace Heffner http://www.mtaonline.net/~hheffner/
