Element | Mass defect in number of Δm = δ | δ’s | N˚ shell given by Table A4 | Probable role of this remaining Δm | Neutrons in add. to hélions | Comments | |
168O | 95.41 | 5 95.41 − 68.81 − 21.07 = 5.53 | 2 | 2 double bonds for the last hellion (2 × 2.76d) |
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| |
2010Ne | 120.12 | 4 120.12 − 95.41 − 21.07 = 3.64 | 2 | Idem (2 × 1.82d) |
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| |
2412Mg | 148.38 | 7 148.4 − 120.12 − 21.07 = 7.19 | 2 | idem |
| Calculation/C (shell 1) gives: 148 − 69 − 63 = 16 or 16/6 = 2.66Δm per bond thus shell 2 | |
2814Si | 177 | 8 | 3 | 2 triple bonds |
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| |
3216S | 204 | 6 | 3 | 2 triple bonds |
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| |
3618Ar | 229.77 | 230 − 204 − 21 = 5 | 3 | 2 triple bonds |
| 230 − 148 − 63 = 19 or 19/6 = 3.17 (shell 3) | |
4020Ca | 256.28 | 256 − 230 − 21 = 5 | 4 |
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|
| |
4622Ti | 298.85 | 299 − 256 − 21 = 22 | 4 |
| 2 | .δs increases strongly when 2 add. n are needed. | |
5024Cr | 326.53 | 327 − 299 − 21 = 7 | 4 |
| 2 |
| |
5426Fe | 354.09 | 354 − 327 − 21 = 6 | 4 |
| 2 |
| |
5828Ni | 380.10 | 380 − 354 − 21 = 5 | 4 |
| 2 |
| |
6430Zn | 419.96 | 420 − 380 − 21 = 19 | 4 |
| 4 |
| |
7032Ge | 458.88 | 459 − 420 − 21 = 18 | 5 |
| 6 |
| |
7434Se | 483 | 483 − 459 − 21 = 3 | 5 |
| 6 |
| |
8036Kr | 522.89 | 523 − 483 − 21 = 19 | 5 |
| 8 |
| |
8438Sr | 548 | 548 − 523 − 21 = 4 | 2 |
| 8 |
| |
9040Zr | 589.63 | 590 − 548 − 21 = 21 | 2 |
| 10 |
| |
9242Mo | 598.58 | 599 − 548 − 42 = 9** | 2 |
| 8 |
| |
9644Ru | 620.95 | 621 − 599 − 21 = 1 | 3 |
| 8 |
| |
10246Pd | 657.79 | 658 − 621 − 21 = 16 | 3 |
| 10 |
| |
10648Cd | 680.11 | 680 − 599 − 63 = 18 | 3 |
| 10 |
| |
11250Sn | 716.70 | 717 − 680 − 21 = 16 | 5 |
| 12 |
| |
12052Te | 765.14 | 765 − 717 − 21 = 27 | 5 |
| 16 |
| |
12454Xe | 786.73 | 787 − 680 − 63 = 44 | 5 |
| 16 |
| |
13056Ba* | 821.83 | 822 − 787 − 21 = 14 | 5 | The new He go to shell 5 with 2n | 18 |
| |
13658Ce | 856.62 | 857 − 822 − 21 = 14 | 5 | The new He go to shell 5 with 2n | 20 |
| |
14260Nd | 891.63 | 892 − 857 − 21 = 14 | 5 | The new He go to shell 5 with 2n | 22 |
| |
14462Sm | 899.02 | 899 − 892 − 21 = −14 |
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| 20 | From Sm to Er, we see 2 decreases of −14 followed by 2 strong increases of 21 and 24 | |
15264Gd | 941.29 | 941 − 899 − 21 = 21 |
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| 24 | It is interpreted as saying that the last helion of the Sm is placed at a nivel 4 and drives at least one other helion previously arrived in 5 at a level 4 | |
15466Dy* | 948.43 | 948 − 941 − 21 = −14 |
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| 22 | 2 n are no longer necessary The helion brought by Gd is then placed at level 5 and requires 4n. The same goes for Dy and Er | |
16268Er | 993.17 | 993 − 948 − 21 = 24 |
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| 26 |
| |
16870Yb | 1024.89 | 1025 − 993 − 21 = 11 |
| The new He go to shell 5 with 2n | 28 | Yb, Hf, W. The 3 He occupy first 3 places in level 5 (filling sequence idem Kr Cd) | |
17472Hf* | 1055.87 | 1056 − 1025 − 21 = 10 |
| The new He go to shell 5 with 2n | 30 |
| |
18074W | 1086.48 | 1087 − 1056 − 21 = 10 |
| The new He go to shell 5 with 2n | 32 | Os sees the end of the filling of level 4 with another He going | |
18476Os | 1105.26 | 1105 − 1087 − 21 = −3 |
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| 32 | in 4. No new n. n decrease in level | |
19078Pt | 1135.31 | 1135 − 1105 − 21 = 5 |
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| 34 |
| |
19680Hg | 1166.47 | 1167 − 1135 − 21 = 11 |
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| 36 | Pt to Pb end of filling shell 5 | |
20482Pb | 1209.15 | 1209 − 1167 − 21 = 21 |
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| 40 |
| |
20984Po* | 1231.57 | 1232 − 1209 − 21 = 1 |
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| 41 |
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22286Rn* | 1285.32 | 1285 − 1232 − 21 = 32 |
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| 50 |
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22688Ra* | 1302.62 | 1303 − 1285 − 21 = −3 |
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| 50 |
| |
23290Th* | 1328.93 | 1329 − 1303 − 21 = 5 |
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| 52 |
| |
23492U* | 1337.32 | 1337 − 1329 − 21 = −13 |
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| 50 |
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