Version 5.0, Sep 28, 2019
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Lists all energetically favourable reactions that cascade from a starting list of the nuclides in the active core fuel.
Simplified version of Cascades5 without the Feedback table. In this, you must directly enter the active core fuel list, as explained below.
It gives quick, but still detailed results for the many cases where the full flexibilty of Cascades5 is not needed.
Maximmum number of nuclei allowed in all pairings as inputs to both the Fusion and the TwoToTwo (2-2) reaction tables = 100
Maximum number of loops allowed for the recursion process = 2
Maximum Reactor Temperature (Kelvin) = 200
Elements that will NOT have MELTED at Maximum Reactor Temperature: Feedback Core Fuel Only
Elements that WILL have BOILED before Maximum Reactor Temperature: Feedback All
Minimum energy (MeV) for any Fusion reaction that was counted = 2
Minimum energy (MeV) for any 2-2 reaction that was counted = 2
Radioactive Isotopes: Feedback All
LHL threshold below which nuclides were counted as Radioactive Isotopes = 18
Nuclear Fermions: Feedback Core Fuel Only
Atomic Fermions: Feedback Core Fuel Only
Elements H, D, N, O, F, Cl, Br, I, Li, Na, Rb and Cr, being able to form Dimers (always Bosonic): Feedback None
SQL compatible string for the order by which the Nuclei Table is presented = order by Z, A
Reactions Not Found in the Parkhomov Tables were Excluded in the Reactions Table
SQL compatible string for the order by which the Reactions Table is presented = order by MeV desc
List of Nuclides in the Fuel = H1 O16
The Reactions Table Has 13, gross but 5 net rows; Nuclei Table Has 4 rows. 'Tid' is the row number of the reaction in either the Fusion or the TwoToTwo Table.
The number 'id' reflects the original order in which the reactions were added to the table on this particular run.
Original order in which the Nuclei below were added = 6, , ,
| id | A | Z | nBorF | aBorF | E | AMU | BE | BEN | SUS | LHL | RDM | DEMeV | pcaNCrust | ppmNCrust | ppmNSolar | SP | MD | EQ | RCPT | Inova_MHz |
| 3 | 1 | 1 | f | b | H | 1.00782503223 | 0.00000000000 | 0.00000000000 | SPN | 50.0000 | null | 0.0000 | 99.9850 | 1399.79 | 705700 | 1/2+ | 2.7928473510 | null | 5700.0000 | 400.000 |
| 7 | 4 | 2 | b | b | He | 4.00260325413 | 28.29476455561 | 7.07369113890 | SPN | 50.0000 | null | 0.0000 | 99.9999 | null | 275200 | null | null | null | null | null |
| 18 | 16 | 8 | b | b | O | 15.99491461957 | 127.61572716061 | 7.97598294754 | SPN | 50.0000 | null | 0.0000 | 99.7590 | 459888.99 | 9592 | null | null | null | null | null |
| 22 | 20 | 10 | b | b | Ne | 19.99244017620 | 160.64033816500 | 8.03201690825 | SPN | 50.0000 | null | 0.0000 | 90.9200 | null | 1548 | null | null | null | null | null |
| id | Type | Tid | neutrino | E1 | A1 | nBorF1 | Z1 | aBorF1 | E2 | A2 | nBorF2 | Z2 | aBorF2 | E3 | A3 | nBorF3 | Z3 | aBorF3 | E4 | A4 | nBorF4 | Z4 | aBorF4 | MeV | found |
| 5 | Fusion | 2900 | none | O | 16 | b | 8 | b | O | 16 | b | 8 | b | S*mp | 32 | b | 16 | b | null | null | null | null | null | 16.539600 | 1 |
| 6 | TwoToTwo | 81737 | none | O | 16 | b | 8 | b | O | 16 | b | 8 | b | He | 4 | b | 2 | b | Si*mp | 28 | b | 14 | b | 9.594400 | 1 |
| 7 | TwoToTwo | 81735 | none | O | 16 | b | 8 | b | O | 16 | b | 8 | b | H | 1 | f | 1 | b | P*mp*f | 31 | f | 15 | b | 7.677400 | 1 |
| 10 | Fusion | 910 | none | He | 4 | b | 2 | b | O | 16 | b | 8 | b | Ne | 20 | b | 10 | b | null | null | null | null | null | 4.728300 | 1 |
| 3 | Fusion | 16 | left | H | 1 | f | 1 | b | O | 16 | b | 8 | b | O*f*f | 17 | f | 8 | f | null | null | null | null | null | 3.358970 | 1 |