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Table 1 |
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force per |
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CLF model |
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unit of |
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Force (Fl) |
mass (m) |
radius |
surface |
surface |
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particle |
constant |
MeV |
x 10-15 m |
area |
area |
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(Fl=2rm) |
(m=Fl/2r) |
(2r = Fl/m) |
(4πr2) |
(Fl/2)/area |
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(a) |
(b) |
('c) |
(d) |
(e) |
(f) |
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e |
2.879929534 |
0.51099892 |
2.817941 |
99.7869287 |
0.014430395 |
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u |
2.879929534 |
2.75 |
0.523624 |
3.445473801 |
0.417929391 |
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d |
2.879929534 |
6 |
0.239994 |
0.723786757 |
1.989487586 |
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0.417929391 |
divided by |
0.0144304= |
28.96174357 |
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1.989487586 |
divided by |
1.0144304= |
137.8678565 |
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137.8678565 |
minus 2 x |
0.417929391 |
= |
137.0319977 |
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Fine structure constant = |
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137.036000 |
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difference |
0.004002 |
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Table 1 shows the cause of the Fine Structure Constant (which, at
present, is considered to be dimensionless); but the CLF model shows
that it is the ratio of the surface forces. The difference between
experimental value and CLF predicted value is probably due to a
difference between the mass values of the experimental and predicted
particles.
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