LYMAN wavelengths determined from the electron mass
Standard procedure calculates these Lyman wavelengths using the
Rydberg constant.
My proposed scheme assumes that the electron mass times Rydeberg equals 1.000000 x 10.
Whereas according to NIST this would only be close at 9.10938188 x 1.09737157 or 9.99637665
This suggested procedure then allows the electron mass to be able to be mutlipled by N
2 over N
2-1
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electron mass |
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N x N |
-1 |
|
911.89065278104 |
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NIST |
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% |
|
NCR |
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% |
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1 |
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4 |
3 |
|
1215.85420370806 |
|
1215.673 |
|
1.0001491 |
|
1215.6737 |
|
1.0001485 |
|
|
9 |
8 |
|
1025.87698437867 |
|
1025.722 |
|
1.0001511 |
|
1025.7223 |
|
1.0001508 |
|
|
16 |
15 |
|
972.68336296645 |
|
972.537 |
|
1.0001505 |
|
972.5371 |
|
1.0001504 |
|
|
25 |
24 |
|
949.88609664692 |
|
949.743 |
|
1.0001507 |
|
949.7431 |
|
1.0001506 |
|
|
36 |
35 |
|
937.94467143193 |
|
937.803 |
|
1.0001511 |
|
937.8035 |
|
1.0001505 |
|
|
49 |
48 |
|
930.88837471398 |
|
930.748 |
|
1.0001508 |
|
930.7483 |
|
1.0001505 |
|
|
64 |
63 |
|
926.36510758709 |
|
926.226 |
|
1.0001502 |
|
926.2257 |
|
1.0001505 |
|
|
81 |
80 |
|
923.28928594081 |
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|
|
|
|
923.1504 |
|
1.0001504 |
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|
100 |
99 |
|
921.10166947580 |
|
|
|
|
|
920.9631 |
|
1.0001505 |
|
|
121 |
120 |
|
919.48974155422 |
|
|
|
|
|
919.3515 |
|
1.0001504 |
|
|
144 |
143 |
|
918.26751049280 |
|
|
|
|
|
918.1294 |
|
1.0001504 |
|
|
169 |
168 |
|
917.31857333331 |
|
|
|
|
|
917.1806 |
|
1.0001504 |
|
|
196 |
195 |
|
916.56701510300 |
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|
|
|
|
916.4292 |
|
|
|
|
225 |
224 |
|
915.96159319524 |
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|
|
|
|
915.8239 |
|
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256 |
255 |
|
915.46669455665 |
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|
|
915.3290 |
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289 |
288 |
|
915.05693976987 |
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|
|
914.9193 |
|
|
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|
324 |
323 |
|
914.71384365653 |
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|
914.5763 |
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361 |
360 |
|
914.42368237210 |
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|
|
|
|
914.2862 |
|
|
|
|
400 |
399 |
|
914.17609301358 |
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|
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|
|
914.0386 |
|
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|
441 |
440 |
|
913.96313153736 |
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|
|
913.8257 |
|
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484 |
483 |
|
913.77862514705 |
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913.6412 |
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529 |
528 |
|
913.61771841131 |
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|
913.4803 |
|
|
|
|
576 |
575 |
|
913.47654956849 |
|
|
|
|
|
913.3392 |
|
|
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|
625 |
624 |
|
913.35201600665 |
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|
|
913.2147 |
|
|
|
|
676 |
675 |
|
913.24160189627 |
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|
|
|
|
913.1043 |
|
|
|
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729 |
728 |
|
913.14324983157 |
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|
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|
|
913.0059 |
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|
784 |
783 |
|
913.05526408728 |
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|
912.9180 |
|
|
|
|
841 |
840 |
|
912.97623689150 |
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|
|
|
912.8389 |
|
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|
900 |
899 |
|
912.90499166067 |
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|
|
|
|
912.7677 |
|
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|
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961 |
960 |
|
912.84053887769 |
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|
|
912.7033 |
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961 |
960 |
|
912.84053887769 |
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912.7033 |
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Interestingly, the electron mass at infinity would therefore ALSO have a wavelength of
911.89065278104181 that is the same as the electron mass of 911.89065278104181. Thus suggesting a direct
relationship between mass and wavelengths.