|
My aim
is to show that data found by particle experiments can be interpreted in
way that unites the basic quantities (Energy, Force, Mass, Charge,
Radius and wavelength) of elementary particles in a single equation and
that all elementary charged particles are compaction states of a single
elementary particle.
Since
1918 various cosmologists1 have suggested that there is a
relationship between mass and radius such that Ru and
Mu equals 1. In an expanding universe we would expect
particles to change in unison with universal expansion leading to the
question, is there a relationship between mass and radii of particles?
If the answer is yes then there should be an arbitrary constant or a
constant value, to which all the other values relate. It is proposed
that linear force is constant for all elementary particles giving the
formula:
Fl = 2rm..
. (1)
As Relativity and CLF are both classical theories there
should be a link between them. Mass is common to both Einsteins formula and the Constant
Linear Force (CLF) formula, giving:
Ec2
= m = Fl/2r
.. (2)
E
= energy
c = speed of light
m =
mass
Fl = linear
force
r =
radius
The choice of 2r (where
r would also produce a constant) is to allow for the inclusion of
wavelength. We intend to show that 2r = λ allowing the substitution:
Ec2
= m = Fl/λ
.. (3)
Linear force is found
using the classical electron radius, electron mass and equation (1).
Given that linear force is a constant, it can be used together with mass
numbers2 and equation (1); to find the radii of other
particles as shown in table 1.
Table 2 shows that
providing all particles have a charge value of 1, the formula for the
classical radius produces the same radii values as that shown in table 1
indicating that the arbitrary allocation of fractional charge to quarks
is incorrect.
It is proposed that
although particles can change their form, the number of particles in
infinity, remains constant. The two remaining particles with radii that
can be found by experiment justify this claim.
Table 3 uses the sum of
the linear force of the particles to calculate the radii of proton and
neutron and compare the result with the radii found by experiment3;
columns A and D give the best match. Indicating that, in particle
interactions, it is the number of particles that is conserved.
Fractional waves are
found in Fractional Quantum Hall Experiments4. It is proposed
that particles are compacted by the fractional wave pattern; it follows
that particle diameters should be determined by the fractional wave
sequence 1, 1/2, 1/3, 1/4, 1/5 etc. Table 4 compares the mass
calculated using wavelength, linear force constant and equation 1, with
the mass values found by experiment as listed in the Particle Data Group
lists for 2004. Fig. 1 shows table 4 in graph form and includes those
wave fractions for which no experimental particle is listed in the 2004
PDG list.
|
|
Linear
force |
|
|
|
radius |
force |
force |
|
|
1 |
1 |
4.5 |
|
|
2 |
2 |
9 |
|
|
3 |
3 |
13.5 |
|
|
4 |
4 |
18 |
|
|
5 |
5 |
11.52 |
|
|
6 |
6 |
8 |
|
|
7 |
7 |
5.877551 |
|
|
8 |
8 |
4.5 |
|
|
9 |
9 |
3.555556 |
|
|
10 |
7.29 |
2.88 |
|
|
11 |
6.024793 |
2.380165 |
|
|
12 |
5.0625 |
2 |
|
|
13 |
4.313609 |
1.704142 |
|
|
14 |
3.719388 |
1.469388 |
|
|
15 |
3.24 |
1.113198 |
|
|
16 |
2.847656 |
|
|
|
17 |
2.522491 |
|
|
|
18 |
2.25 |
|
|
|
19 |
2.019391 |
|
|
|
20 |
1.8225 |
|
|
|
21 |
1.653061 |
|
|
|
22 |
1.506198 |
|
|
|
23 |
0.728412 |
|
|
TOTALS |
|
|
|
field (linear force) |
90 |
90 |
|
nucleus or shell |
45 |
45 |
|

Fig.1
The table and graph shows how the same total linear
force is distributed in two different vacuum fields.
Force is distributed in equal quantities either side
of the point of maximum force. |
|
Table 1
(PDG data in
bold type) |
|
|
|
|
|
CLF model |
|
|
Force (F) |
Mass2(m) |
|
radius |
|
particle |
constant |
MeV |
|
x 10-15 m |
|
|
(F=rm) |
(m=F/r) |
(r = Fl/m) |
r |
|
(a) |
(b) |
('c) |
(d) |
(e) |
|
e |
2.8799296 |
0.51099892 |
5.6358822 |
2.82E+00 |
|
΅ |
2.8799296 |
105.658369 |
0.02725699 |
1.36E-02 |
|
τ |
2.8799296 |
1776.99 |
0.00162068 |
8.10E-04 |
|
|
|
|
|
|
|
u |
2.8799296 |
2.75 |
1.04724713 |
5.24E-01 |
|
d |
2.8799296 |
6 |
0.47998827 |
2.40E-01 |
|
s |
2.8799296 |
105 |
0.0274279 |
1.37E-02 |
|
c |
2.8799296 |
1250 |
0.00230394 |
1.15E-03 |
|
b |
2.8799296 |
4250 |
0.00067763 |
3.39E-04 |
|
t |
2.8799296 |
174300 |
0.000016523 |
8.26E-06 |
| |
|
Table 2
(current data
in bold type) |
|
|
|
|
|
|
|
|
|
classical |
|
|
|
|
|
|
|
|
|
r |
|
particle |
e |
(e2) |
4π |
εo |
me |
c2 |
(cdef) |
b/g=ro
(cm) |
|
|
a |
b |
c |
d |
e |
f |
g |
h |
|
e |
|
|
|
|
0.51099892 |
|
5.11E+06 |
2.817900E-13 |
|
΅ |
|
|
|
|
105.658369 |
|
1.06E+09 |
1.362830E-15 |
|
τ |
|
|
|
|
1776.99 |
|
1.78E+10 |
8.103275E-17 |
|
|
0.0012 |
1.44E-06 |
12.56637061 |
8.85E-12 |
|
8.99E+16 |
|
|
|
u |
|
|
|
|
2.75 |
|
2.75E+07 |
5.236159E-14 |
|
d |
|
|
|
|
6 |
|
6.00E+07 |
2.399906E-14 |
|
s |
|
|
|
|
105 |
|
1.05E+09 |
1.371375E-15 |
|
c |
|
|
|
|
1250 |
|
1.25E+10 |
1.151955E-16 |
|
b |
|
|
|
|
4250 |
|
4.25E+10 |
3.388103E-17 |
|
t |
|
|
|
|
174300 |
|
1.74E+12 |
8.261296E-19 |
|
Given that all
particles have the same charge as the electron, then the formula
for finding the Classical electronic radius |
|
produces the
same value for radii (col h) as that given in col d of table 1. |
|
|
|
|
|
|
|
Table 3
(data from
experiments in bold type) |
|
|
Proton |
Possible Neutron
structures |
|
|
(SM and CLF) |
(SM) |
|
(CLF) |
|
|
A |
B |
C |
D |
|
sub-particles
(a) |
uud |
ddu |
dduep |
uudep |
|
mass (b) |
11.5 |
14.75 |
15.772 |
12.522 |
|
r = Fl/m (c) |
0.375643 |
0.292874 |
0.456494 |
0.574974 |
|
2r (d) |
0.751286 |
0.585748 |
0.912988 |
1.149948 |
|
r (fermi)
(e) |
0.805 |
1.1 |
1.1 |
1.1 |
|
|
|
|
|
|
|
(e) - (d)
(f) |
+0.053714 |
+0.514252 |
+0.187012 |
-0.049948 |
|
Table 4 |
|
Fl =
2.87992961524744 |
|
|
|
|
theoretical |
mass |
|
|
|
|
|
|
|
fraction of |
λ |
mass |
found by |
|
|
|
|
|
|
|
remainder |
B1-(A2*B1) |
(m=Fl/λ) |
experiment |
|
c-d |
PDG reference |
|
|
|
|
a |
b |
c |
d |
|
e |
|
|
|
|
1/1 |
1 |
28.17941 |
0.1021998 |
|
|
|
Graviton? |
|
|
|
1/2 |
0.5 |
14.089705 |
0.2043996 |
0.26 |
±48 |
-0.06 |
56 CHETYRKIN 98
THEO MS scheme |
|
1/3 |
0.3333333 |
9.3931367 |
0.3065994 |
0.3 |
±10 |
0.01 |
57 CUCCHIERI 98
LATT MS scheme |
|
1/4 |
0.25 |
7.0448525 |
0.4087991 |
0.43 |
± 8 |
-0.02 |
52 MALTMAN 99
THEO MS scheme |
|
1/5 |
0.2 |
5.635882 |
0.5109989 |
0.510998918 |
electron |
|
|
|
|
|
1/6 |
0.1666667 |
4.6965684 |
0.6131987 |
0.553 |
±12 |
0.06 |
55 BECIREVIC 98
LATT MS scheme |
|
1/7 |
0.1428571 |
4.02563 |
0.7153985 |
0.66 |
±19 |
0.06 |
58 DOMINGUEZ 98
THEO MS scheme |
|
1/13 |
0.0769231 |
2.1676469 |
1.3285972 |
1.3 |
±0.3 |
0.03 |
ASTIER 00D NOMD |
|
|
1/17 |
0.0588235 |
1.6576124 |
1.7373963 |
1.7 |
±0.3 |
0.04 |
1 AUBIN 04A LATT
MS scheme |
|
|
1/18 |
0.0555556 |
1.5655228 |
1.8395961 |
1.79 |
±0.38 |
0.05 |
VILAIN 99 THEO
MS scheme |
|
1/23 |
0.0434783 |
1.2251917 |
2.350595 |
2.3 |
±0.4 |
0.05 |
3 NARISON 99
THEO MS scheme |
|
1/27 |
0.037037 |
1.0436819 |
2.7593942 |
2.7 |
±0.06 4.72 |
0.06 |
3 AUBERT 04X
THEO |
|
|
1/28 |
0.0357143 |
1.0064075 |
2.8615939 |
2.9 |
±0.6 |
-0.04 |
2 JAMIN 02 THEO
MS scheme |
|
|
1/30 |
0.0333333 |
0.9393137 |
3.0659935 |
3 |
±0.7 |
0.07 |
5 NARISON 95C
THEO MS scheme |
|
1/33 |
0.030303 |
0.8539215 |
3.3725929 |
3.4 |
±0.11 |
-0.03 |
5 HOANG 04 THEO |
|
|
1/35 |
0.0285714 |
0.805126 |
3.5769924 |
3.6 |
±0.03 4.68 |
-0.02 |
4 BAUER 04 THEO |
|
|
1/37 |
0.027027 |
0.7616057 |
3.781392 |
3.8 |
±0.2 |
-0.02 |
27 EICKER 97
LATT MS scheme |
|
1/38 |
0.0263158 |
0.7415634 |
3.8835918 |
3.9 |
±0.5 |
-0.02 |
6 AUBIN 04A LATT
MS scheme |
|
|
1/39 |
0.025641 |
0.722549 |
3.9857916 |
3.95 |
±0.3 |
0.04 |
17 CHIU 02 LATT
MS scheme |
|
40 |
0.025 |
0.7044853 |
4.0879913 |
4.05 |
±0.6 |
0.04 |
19 MALTMAN 01
THEO MS scheme |
|
1/41 |
0.0243902 |
0.6873027 |
4.1901911 |
4.19 |
±0.9 |
0.00 |
7 JAMIN 02 THEO
MS scheme |
|
1/42 |
0.0238095 |
0.6709383 |
4.2923909 |
4.25 |
±0.7 |
0.04 |
5 NARISON 95C
THEO MS scheme |
|
1/43 |
0.0232558 |
0.6553351 |
4.3945907 |
4.4 |
±0.1 ±0.4 |
-0.01 |
14 BECIREVIC 03
LATT MS scheme |
|
1/44 |
0.0227273 |
0.6404411 |
4.4967905 |
4.5 |
±0.11 |
0.00 |
6 MCNEILE 04
LATT |
|
|
1/45 |
0.0222222 |
0.6262091 |
4.5989903 |
4.57 |
|
0.03 |
20 AOKI 00 LATT
MS scheme |
|
46 |
0.0217391 |
0.6125959 |
4.70119 |
4.7 |
±2 |
0.00 |
21 GOECKELER 00
LATT MS scheme |
|
1/51 |
0.0196078 |
0.5525375 |
5.212189 |
5.2 |
±0.9 |
0.01 |
7 JAMIN 02 THEO
MS scheme |
|
|
1/63 |
0.015873 |
0.4472922 |
6.4385864 |
6.4 |
±1.1 8 |
0.04 |
NARISON 99 THEO
MS scheme |
|
|
1/69 |
0.0144928 |
0.4083972 |
7.0517851 |
7 |
±1.1 |
0.05 |
9 JAMIN 95 THEO
MS scheme |
|
|
1/72 |
0.0138889 |
0.3913807 |
7.3583844 |
7.4 |
±0.7 |
-0.04 |
10 NARISON 95C
THEO MS scheme |
|
223 |
0.0044843 |
0.1263651 |
22.790552 |
22.7 |
±20 |
0.09 |
61 EICKER 97
LATT MS scheme |
|
1/224 |
0.0044643 |
0.1258009 |
22.892752 |
22.8 |
±14.1 |
0.09 |
59 CHETYRKIN 97
THEO MS scheme |
|
1/744 |
0.0013441 |
0.0378756 |
76.036639 |
76 |
±0.09 |
0.04 |
9 CORCELLA 03
THEO |
|
|
1/793 |
0.001261 |
0.0355352 |
81.044428 |
81 |
±0.09 |
0.04 |
7 BAUER 03 THEO |
|
|
1/827 |
0.0012092 |
0.0340743 |
84.519221 |
84.5 |
±0.10 |
0.02 |
11 EIDEMULLER 03
THEO |
|
|
1/861 |
0.0011614 |
0.0327287 |
87.994014 |
88 |
±0.05 |
-0.01 |
16 KUHN 01 THEO |
|
|
1/900 |
0.0011111 |
0.0313105 |
91.979805 |
92 |
±0.06 |
-0.02 |
13 MAHMOOD 03
THEO |
|
|
1/910 |
0.0010989 |
0.0309664 |
93.001803 |
93 |
±0.05 |
0.00 |
8 BORDES 03
THEO |
|
|
1/930 |
0.0010753 |
0.0303004 |
95.045799 |
95 |
± 4 |
0.05 |
49 GOECKELER 00
LATT MS scheme |
|
1/969 |
0.001032 |
0.0290809 |
99.03159 |
99 |
±0.090 ±0.025 |
0.03 |
18 PINEDA 01
THEO |
|
|
1/978 |
0.0010225 |
0.0288133 |
99.951388 |
100 |
±0.82 |
-0.05 |
19 BARATE 00V
ALEP |
|
|
1/979 |
0.0010215 |
0.0287839 |
100.05359 |
100 |
±14 |
0.05 |
50 AOKI 99 LATT
MS scheme |
|
1/1008 |
0.0009921 |
0.0279558 |
103.01738 |
103 |
±0.57 |
0.02 |
15 ABBIENDI 01S
OPAL |
|
|
1/1027 |
0.0009737 |
0.0274386 |
104.95918 |
105 |
±17 |
-0.04 |
40 GAMIZ 03 THEO
MS scheme |
|
1/1037 |
0.0009643 |
0.027174 |
105.98118 |
106 |
±0.031 |
-0.02 |
12 ERLER 03 THEO |
|
|
1/1086 |
0.0009208 |
0.0259479 |
110.98896 |
111 |
±12 |
-0.01 |
55 BECIREVIC 98
LATT MS scheme |
|
1/1115 |
0.0008969 |
0.025273 |
113.95276 |
114 |
±12 |
-0.05 |
45 MALTMAN 02
THEO MS scheme |
|
1/1125 |
0.0008889 |
0.0250484 |
114.97476 |
115 |
±0.06 |
-0.03 |
17 NARISON 01B
THEO |
|
|
1/1135 |
0.0008811 |
0.0248277 |
115.99675 |
116 |
±0.10 |
0.00 |
10 DEDIVITIIS 03
LATT |
|
|
1/1145 |
0.0008734 |
0.0246108 |
117.01875 |
117 |
±0.070 |
0.02 |
14 PENIN 02 THEO |
|
|
1/1155 |
0.0008658 |
0.0243978 |
118.04075 |
118 |
±17 |
0.04 |
41 GAMIZ 03 THEO
MS scheme |
|
1/1223 |
0.0008177 |
0.0230412 |
124.99034 |
125 |
± 2 ± 8 38 |
-0.01 |
BECIREVIC 03
LATT MS scheme |
|
1/1262 |
0.0007924 |
0.0223292 |
128.97613 |
129 |
±16 |
-0.02 |
44 JAMIN 02 THEO
MS scheme |
|
1/1272 |
0.0007862 |
0.0221536 |
129.99812 |
130 |
± 9 ±16 |
0.00 |
39 CHIU 03 LATT
MS scheme |
|
1/1370 |
0.0007299 |
0.0205689 |
140.0137 |
140 |
±15 |
0.01 |
48 AOKI 00 LATT
MS scheme |
|
1/1448 |
0.0006906 |
0.0194609 |
147.98529 |
148 |
±48 |
-0.01 |
56 CHETYRKIN 98
THEO MS scheme |
|
1/1487 |
0.0006725 |
0.0189505 |
151.97108 |
152 |
±27 |
-0.03 |
47 KOERNER 01
THEO MS scheme |
|
1/1663 |
0.0006013 |
0.0169449 |
169.95824 |
170 |
-3 |
-0.04 |
42 ALIKHAN 02
LATT MS scheme |

Fig.2
Graph of table 4.
-------------------------------------------------
Ec2
= m = Fl/λ
Einstein's equation uses the energy
generated by movement and given that movement cannot be instantaneous,
allows Einstein to include time in his work on relativity; but the
maximum energy is only present on one radial. By ignoring movement and
time the Constant linear force (CLF) equation gives the structure of static
particles and allows an explanation of compaction to show that all
particles are compactions of a single elementary particle. Both Einstein
and CLF give the
same mass value for the same radius, even when movement causes the same
radius value to apply to different particles. The potential energy
and rest mass of Einstein's equation are equal to the linear
force and mass of the CLF equation.

Fig 3
References
1
arXiv:astro-ph/0606448 v1 19 June 2006
2
S. Eidelman et al.,
Phys. Lett. B 592, 1 (2004) (bibtex)
3
http://www.terra.es/personal/gsardin/news13.htm
4
http://nobelprize.org/nobel_prizes/physics/laureates/1998/press.html
|