A.M.Molchanov, Russian mathematician. He devoted himself to mathematical modeling in biology, ecology, genetics, etc. He assumed resonance structure of the solar system. The development of the planet's leads to resonances and orbital periods in the ratio of small integers. He suggested some relationships for both the sun and the sun system, as well as for the systems of Jupiter and Saturn. |
Three Jupiter and three Uranus moons respect the so-called Laplace resonance, which limits the possibility of multiple conjunctions. It is a certain principle of minimal interaction - which ensures balance.
Therefore, resonance does not generally only represent a disturbing element (which can break objects, destroy bridges, etc.), but it can also be a thing to ensure synchronization and stability.
There is a simple argument regarding the moon of Jupiter / Uranus: they are synchronized thanks to the tidal forces. According to A.M.Molchanov (1965, 1968), however, the bodies can be synchronized even when operating by very weak forces. Molchanov considers "small dissipative forces", in some newer theories also other hypotheses were proposed (M. B. Gubaidullin, 2015, see also N. Scafetta, 2013).
According to the behavior of Jupiter / Uranus moons, generalization offers: multiple conjunctions of bodies are not desirable in the Solar System - there is a tendency for them to appear only minimally, not to appear exactly or to be somehow balanced.
Small (tidal) effects can enhance the natural oscillation of the solar atmosphere and cause great changes.
J.J.Condon and R.R.Schmidt at work (1975) derive a resonance relationship in the form Lt = 3 * Lv -5 * Le + 2 * Lj where Lv, Le and Lj are the longitude of Venus, Earth and Jupiter.
From the comparison of the synodic periods of the planets,
((E, J) / 5, (V, J) / 3) = 2 · W. Then 1 / (2W) = 3 / V-5 / E + 2 / J, and 2W = 22.13505 years,
ie, W = 11.06753 years span>.
Maximum solar activity occurs approximately when (for the longitude of Venus,
Earth and Jupiter):
But that does not always apply ...
Here we derive:
For 2W = 22.3855 years, Jupiter will go back by 40.6 dg, ie, if we observe the system with a 2W period, we will sense that Jupiter is orbiting the period with the period about 198.4 years. If he really moved, he would meet Saturn every 25.65 years, ie 4 * I or 3 * Y, where I is the period of the inner planets = 6.4 years and Y is 8.54 years. The difference between 25.65 and 22.39 years is 3.26 years. (52 Tun / 72 Almanac Cycle 18720 d, Calendar Round 52 Haab / 73 Almanac Cycle 18980 d).
Molchanov's Resonance: [M, -V, -E / 2, -R] [V, -R / 3, -S] [E, -R, 2, J, / 2] [U, -U / 7], [U, -N / 2], [U, -P / 3] (plus their linear combination ...)
In the repetition of the climatic periods, there is a so-called Hallstatt cycle (H = 2300 years) which correlates with the resonance of orbital periods of outer planets.
The difference of 2403.05 years and 2224.10 years (with the sum of 4627 years) is 178.95 years, but the common divisor is the period 185.1 years (+ -0.2 years) which can be modeled by resonance 1 / J-3 / S + 2 / N (or ((U, N), H)).
Line of conjunctions V-E-J move (backward) with period: P=
(W,J) = (11.06753, 11.861983) = 165.25 years, i.e. approximately
with orbital period of Neptune.
Axial period Jupiter-Neptun [J,N] = 22.13075 y = 2*11.06538 years
coincides with period of Solar activity.
Some authors (Ray Tomes,…) connect solar period with these two bodies ( Jupiter, Neptune).
(In combination with resonance of inner planet it leads to
6/V-10/E+3/J-1/N = 0, i.e. unstable resonance).
Importance of Jupiter (with a view to the weight) is clear.
Neptune might acquire its influence by the distance from the
sun, see, for example value (M * R2 (moment of inertia):
M [1024 kg] | a [109 m] | M*a2 [1039kg*m²] | |
Jupiter | 1899,0 | 778,6 | 1151,2 |
Saturn | 568,0 | 1433,5 | 1167,2 |
Uran | 86,8 | 2872,5 | 716,2 |
Neptun | 102,0 | 4495,1 | 2061,0. |
Also period of resonance 1/W = 1/J + 1/U – 1/N correlates by value W = 11.094 years with the mean period of the Solar cycle. Let us write it to form of stable resonance: 1/W - 1/J + 1/N - 1/U = 0.
Resonance maxima occur, when it holds (for longitudes of Jupiter,
Jupiter perihelion, Uranus and Neptune):
Resonance minima occur, when it holds (for longitudes of
Jupiter, Jupiter perihelion, Uranus and Neptune):
This resonance binds the period of solar activity W with orbital periods of planets Jupiter, Neptune, Uranus. Saturn's here seemingly outside game - however it is bound by resonance of outer planets to Jupiter perihelion (viz Influence of Jupiter)!?
The resonance arise as a sum of the two delta angles ∆J + ∆UN where:
n | Mo | ∆J | ∆UN | n | Mo | ∆J | ∆UN | n | Mo | ∆J | ∆UN | n | Mo | ∆J | ∆UN | |||
-30 | 1416,7 | 316 | 224 | -14 | 1594,4 | 306 | 234 | 2 | 1772,0 | 296 | 244 | 18 | 1949,5 | 283 | 257 | |||
-29 | 1428,0 | 296 | 244 | -13 | 1605,6 | 286 | 254 | 3 | 1783,1 | 273 | 267 | 19 | 1960,5 | 257 | 283 | |||
-28 | 1439,2 | 275 | 265 | -12 | 1616,6 | 262 | 278 | 4 | 1794,1 | 246 | 294 | 20 | 1971,4 | 229 | 311 | |||
-27 | 1450,2 | 251 | 289 | -11 | 1627,6 | 235 | 305 | 5 | 1805,0 | 218 | 322 | 21 | 1982,4 | 203 | 337 | |||
-26 | 1461,2 | 224 | 316 | -10 | 1638,5 | 207 | 333 | 6 | 1815,9 | 192 | 348 | 22 | 1993,4 | 180 | 0 | |||
-25 | 1472,0 | 197 | 343 | -9 | 1649,4 | 182 | 358 | 7 | 1826,9 | 168 | 312 | 23 | 2004,5 | 159 | 21 | |||
-24 | 1483,0 | 172 | 8 | -8 | 1660,5 | 160 | 20 | 8 | 1838,1 | 149 | 31 | 24 | 2015,7 | 140 | 40 | |||
-23 | 1494,1 | 150 | 30 | -7 | 1671,6 | 140 | 40 | 9 | 1849,3 | 130 | 50 | 25 | 2026,8 | 120 | 60 | |||
-22 | 1505,3 | 130 | 50 | -6 | 1682,8 | 120 | 60 | 10 | 1860,4 | 109 | 71 | 26 | 2037,9 | 96 | 84 | |||
-21 | 1516,4 | 110 | 70 | -5 | 1694,0 | 99 | 81 | 11 | 1871,5 | 85 | 95 | 27 | 2049,0 | 70 | 110 | |||
-20 | 1527,5 | 88 | 92 | -4 | 1705,0 | 74 | 106 | 12 | 1882,5 | 58 | 122 | 28 | 2060,0 | 42 | 137 | |||
-19 | 1538,6 | 63 | 117 | -3 | 1716,0 | 47 | 133 | 13 | 1893,5 | 31 | 149 | 29 | 2071,1 | 18 | 162 | |||
-18 | 1549,6 | 36 | 144 | -2 | 1727,1 | 21 | 159 | 14 | 1904,6 | 7 | 173 | 30 | 2082,3 | 356 | 184 | |||
-17 | 1560,7 | 10 | 170 | -1 | 1738,2 | 357 | 183 | 15 | 1915,9 | 346 | 194 | 31 | 2093,6 | 336 | 204 | |||
-16 | 1571,9 | 346 | 194 | 0 | 1749,5 | 336 | 204 | 16 | 1927,2 | 326 | 213 | 32 | 2104,8 | 316 | 224 | |||
-15 | 1583,7 | 326 | 214 | 1 | 1760,8 | 316 | 224 | 17 | 1938,4 | 306 | 234 | 33 | 2116 | 294 | 246 |
N | WS | WI | WO | WA | WI-WS | Wo-WS | Wo-WI | |
-23 | 1492 | 1494,6 | 1494,1 | 1490,4 | 2,6 | 2,1 | -0,5 | |
-22 | 1505 | 1505,8 | 1505,2 | 1501,6 | 0,8 | 0,2 | -0,6 | |
-21 | 1519,0 | 1517,3 | 1516,4 | 1513,1 | -1,7 | -2,6 | -0,9 | |
-20 | 1528,0 | 1527,5 | 1527,5 | 1523,7 | -0,5 | -0,5 | 0,0 | |
-19 | 1539,0 | 1539,1 | 1538,6 | 1535,6 | 0,1 | -0,4 | -0,5 | |
-18 | 1548,0 | 1549,6 | 1549,6 | 1546,9 | 1,6 | 1,6 | 0,0 | P-maximum |
-17 | 1558,0 | 1560,8 | 1560,7 | 1558,1 | 2,8 | 2,7 | -0,1 | |
-16 | 1572,0 | 1572,5 | 1571,9 | 1570,1 | 0,5 | -0,1 | -0,6 | |
-15 | 1581,0 | 1583,6 | 1583,7 | 1580,4 | 2,6 | 2,7 | 0,1 | |
-14 | 1591,0 | 1594,6 | 1594,4 | 1591,7 | 3,6 | 3,4 | -0,2 | |
-13 | 1604,0 | 1606,2 | 1605,6 | 1602,8 | 2,2 | 1,6 | -0,6 | 1607 - Kepler's spot |
-12 | 1615,5 | 1616,8 | 1613,1 | 1613,0 | 1,3 | 1,1 | -0,2 |
1618 - Simon Mair's (Marius) spots |
-11 | 1626,0 | 1627,8 | 1627,6 | 1625,3 | 1,8 | 1,6 | -0,2 | |
-10 | 1639,5 | 1638,8 | 1638,5 | 1636,3 | -0,7 | -1,0 | -0,3 |
n | WS | WI | WO | WA | WI-WS | WO-WS | WO-WI | |
-9 | 1649,0 | 1649,9 | 1649,4 | 1647,5 | 0,9 | 0,4 | -0,5 | |
-8 | 1660,0 | 1660,8 | 1660,5 | 1659,2 | 0,8 | 0,5 | -0,3 | 1660 - Hevelius spots, 1661 - Boyle and Picard sunspot group |
-7 | 1675,0 | 1672,2 | 1671,6 | 1669,5 | -2,8 | -3,4 | -0,6 | 1671 (August) - Pickard spot, Hevelius spot, 1676 - Pickard extreme, Maunder |
-6 | 1685,0 | 1682,5 | 1682,8 | 1681,0 | -2,5 | -2,2 | 0,3 | 1684 - Pickard extreme, Cassini, Kirch |
-5 | 1693,0 | 1693,5 | 1694,0 | 1692,2 | 0,5 | 1,0 | 0,5 | |
-4 | 1705,5 | 1705,2 | 1705,0 | 1703,1 | -0,3 | -0,5 | -0,2 | |
-3 | 1718,2 | 1716,0 | 1716,0 | 1715,2 | -2,2 | -2,2 | 0,0 | 1716 - visible aurora, 1714-15 - P-maximum, end of Maunder period |
-2 | 1727,5 | 1727,4 | 1727,1 | 1726,3 | -0,1 | -0,4 | -0,3 | |
-1 | 1738,7 | 1738,5 | 1738,2 | 1737,8 | -0,2 | -0,5 | -0,3 | |
0 | 1750,3 | 1750,1 | 1749,5 | 1749,2 | -0,2 | -0,8 | -0,6 | 1752 - second maximum |
1 | 1761,5 | 1761,3 | 1760,8 | 1759,7 | -0,2 | -0,7 | -0,5 | |
2 | 1769,7 | 1771,8 | 1772,0 | 1771,4 | 2,1 | 2,3 | 0,2 | 1774 - second maximum |
3 | 1778,4 | 1782,8 | 1783,1 | 1782,3 | 4,4 | 4,7 | 0,3 | |
4 | 1788,1 | 1794,5 | 1794,1 | 1793,4 | 6,4 | 6,0 | -0,4 |
n | WS | WI | WO | WA | WI-WS | WO-WS | Wo-WI | |
5 | 1805,2 | 1805,5 | 1805,0 | 1805,7 | 0,3 | -0,2 | -0,5 | |
6 | 1816,4 | 1815,6 | 1815,9 | 1816,3 | -0,8 | -0,5 | 0,3 | |
7 | 1829,9 | 1827,2 | 1826,9 | 1827,7 | -2,7 | -3,0 | -0,3 | |
8 | 1837,2 | 1838,3 | 1838,1 | 1838,7 | 1,1 | 0,9 | -0,2 | |
9 | 1848,1 | 1849,2 | 1849,3 | 1848,9 | 1,1 | 1,2 | 0,1 | 1847-48 - Giant sunspots |
10 | 1860,1 | 1860,2 | 1860,4 | 1860,7 | 0,1 | 0,3 | 0,2 | 1859 - proton event (Carrington), 1864 - second maximum, 1859-60 - Giant sunspots |
11 | 1870,6 | 1871,3 | 1871,5 | 1871,6 | 0,7 | 0,9 | 0,2 | 1870-71 - Giant sunspots, 1870 - proton event (Young) |
12 | 1883,9 | 1881,7 | 1882,5 | 1882,9 | -2,2 | -1,6 | -0,8 | 1882 - P-maximum, 1882 - Giant sunspot, 1882 - proton events (Maunder) |
13 | 1894,1 | 1893,5 | 1893,5 | 1894,9 | -0,6 | -0,6 | 0,0 | 1892-93 - Giant sunspots, 1892 - proton events (Rudeaux) |
14 | 1907,0 | 1904,5 | 1904,7 | 1905,7 | -2,5 | -2,3 | -0,2 | 1905,07,08 - Giant sunspots, 1908 - proton event |
15 | 1917,6 | 1916,1 | 1915,9 | 1917,3 | -1,5 | -1,7 | -0,2 | 1917 - Giant sunspot, 1917 - proton event |
16 | 1928,4 | 1926,7 | 1927,2 | 1928,4 | -1,7 | -1,2 | -0,5 | 1926,29 - Giant sunspots, 1926 - proton event |
17 | 1937,4 | 1937,9 | 1938,4 | 1939,1 | 0,5 | 1,0 | 0,5 | 1935,37-42 - Giant sunspots, 1938 - proton event |
18 | 1947,5 | 1949,5 | 1949,6 | 1951,1 | 2,0 | 2,1 | 0,1 | 1946 - proton event, 1949 - proton event |
n | WS | WI | WO | WA | WI-WS | WO-WS | WO-WI | |
19 | 1957,9 | 1960,5 | 1960,5 | 1962,1 | 2,6 | 2,6 | 0,0 | 1958 - the highest level since Galileo's observations (1610), 1956,59-61 - proton events |
20 | 1968,9 | 1972,2 | 1971,4 | 1973,8 | 3,3 | 2,5 | -0,8 | 1969 - proton event, 1972 - extreme flare, 1972 - second maximum |
21 | 1979,9 | 1983,2 | 1982,4 | 1985,5 | 3,3 | 2,5 | -0,8 | 1981 - extreme flare |
22 | 1989,6 | 1993,2 | 1993,4 | 1996,1 | 3,6 | 3,8 | 0,2 | 1990 - the second highest level since Galileo's observations (1610) |
23 | 2000,5 | 2004,3 | 2004,6 | 2007,8 | 3,8 | 4,1 | 0,3 | |
24 | ? | 2015,3 | 2015,7 | 2018,3 | ? | ? | 0,4 | |
25 | ? | 2026,1 | 2026,8 | 2028,9 | ? | ? | 0,7 | |
26 | ? | 2036,6 | 2037,9 | 2040,9 | ? | ? | 1,3 | |
27 | ? | 2048,1 | 2049,0 | 2051,5 | ? | ? | 0,9 | 2050-51 - P-maximum |
28 | ? | 2059,5 | 2060,0 | 2063,4 | ? | ? | 0,5 | |
29 | ? | 2070,6 | 2071,1 | 2074,7 | ? | ? | 0,5 |
Theoretical extremes (maxima as well as minima) of solar activity take place about with the same period as the actual extremes. The biggest differences in maximum are observed in years 1583-1606, 1675-1685, 1778- 1788, 1829, 1958-2000. The biggest differences in minimum are observed in years 1553,1619, 1784, 1902-1924,1996.
Justin Flynn has noticed certain regularities of these deviations (personal communication).
Consider the following chart:
Let us divide the Uranus-Neptune conjuction cycle to following time-periods, and to write departures taken from the column Mo-MS of the tables above:
Time- Departures period sign maxima minima ------------------------------------ 1543-1586 - 1586-1628 + 1628-1671 - 1671-1714 + 1714-1757 - 1718-1761 1745-1765 1757-1800 + 1769-1788 1777-1799 1800-1842 - 1805-1830 1810-1832 1842-1885 + 1838-1871 1844 1885-1928 - 1884-1928 1856-1943 1928-1971 + 1938-2004 1954-2008 1971-2014 - ????????? 2014-2057 +
For the period 1714 -1971 all seems to work quite well. But this rule (like the rule from the paragraph Coincidence of geometrical axes) fails - and again roughly after year 1960!?)
Let dUN = Neptune.Longitude - Uranus.Longitude, dJJa = Jupiter.Longitude - Jupiter.LongPerihelion - 180 and we look for extremes where dUN + correction = dJJa (with a given precission, e.g. 5 dg).
The following function was derived from the previous paragraph: f = Cos(2*dUN) * abs(Cos(2*dUN)) = sign(Cos(2*dUN)) * Cos2(2*dUN) with a correction angle equal to k * f. For value of the constant k = 120 we get the following table:
Table of corrected extremesDiff Theory Jp J S U N f(dUN) Corrected Observation ------------------------------------------------------------------------------ 11,28 1749,39 - 15 346 231 322 118 +0.38 1750,73 1750.3 * 1757 11,25 1760,65 - 14 326 358 6 143 0.00 1760,72 1761.5 * 11,20 1771,84 + 14 305 146 51 167 -0.30 1770,79 1769.7 * 11,09 1782,93 + 13 281 276 98 191 -0.87 1779,56 1778.4 * 11,01 1793,94 + 14 256 46 148 215 -0.70 1791,19 1788.1 ? 1800 10,92 1804,86 - 15 229 191 200 238 +0.06 1805,13 1805.2 * 10,92 1815,79 - 15 203 314 249 262 +0.98 1819,56 1816.4 ? 11,01 1826,79 - 14 179 92 296 286 +0.73 1829.80 1829.9 * 11,14 1837,94 + 14 159 233 340 310 +0.21 1838,80 1837.2 . 1842 11,17 1849,11 + 14 140 359 24 334 -0.02 1849,04 1848.1 * 11,17 1860,28 + 14 119 147 69 359 -0.48 1858,55 1860,1 * 11,12 1871,39 + 15 97 277 118 24 -0.99 1868,05 1870,6 ? 10,98 1882,37 - 15 69 48 169 48 -0.29 1881,41 1883,9 ? 1885 11,01 1893,38 - 14 41 193 220 72 +0.25 1894,28 1894,1 * 11,14 1904,52 - 14 17 318 270 97 +1.00 1908,13 1907,0 * 11,23 1915,75 - 14 356 101 315 122 +0.66 1918,04 1917,6 * 11,34 1927,08 - 16 338 242 360 147 +0.14 1927,54 1928,4 * 1928 11,23 1938,31 + 16 317 10 44 171 -0.08 1938,11 1937,4 * 11,12 1949,42 + 14 294 157 91 195 -0.63 1947,03 1947,5 * 10,98 1960,40 + 14 267 284 141 218 -0.99 1956,54 1957,9 * 10,90 1971,30 + 14 239 55 192 242 -0.03 1971,21 1968,9 ? 1971 10,95 1982,25 + 15 214 199 242 265 +0.68 1984,90 1979,9 ?? 11,03 1993,29 + 16 191 323 289 289 +0.94 1997,03 1989,6 ?? 11,12 2004,40 + 15 170 105 334 313 +0.47 2006,28 2000,5 ?? 11,14 2015,55 14 150 243 17 338 +0.78 2015,70 ? 2014
Rows with "acceptable" results are marked by asterisks.
Resonances observed above are not only resonances producing cycles with period close to the period of solar activity. For example (J/1,-S/2,+U/4,-N/3) = 21.8 years while (J/1,-S/3,+U/4,-N/2) = 55.8 years. Also (S/1,+U/3,-N/4) = 22.0 years, therefore e.g. cos(Ls+3*Lu-4*Ln) oscillates with 11-years period etc.
J S U N k*W M ------------------------------------ 0 3 1 -4 11,2 -971,5 1 0 2 -3 11,1 -1671,2 2 -3 3 -2 11,1 -5971,4 0 1 3 -4 22,0 7807,8 1 -1 -1 1 22,5 -1376,5 0 1 -1 0 45,4 -1724,2 1 -2 0 1 44,5 -6717,5 0 0 2 -2 85,7 2829,8 0 1 -3 2 96,3 -1072,9 1 -3 3 -1 82,7 1275,0
Now let us consider resonance with period 44.5 years according to row:
J S U N k*W M ------------------------------------ 1 -2 0 1 44,5 -6717,5
After rewriting to the form:
we get new values WN (we will compare them to extremes WO):
Spacing WN WO 0,00 1605,503 1605,6 9,09 1614,593 1613,1 14,84 1629,433 1627,6 8,27 1637,701 1638,5 10,82 1648,516 1649,4 13,03 1661,548 1660,5 8,10 1669,652 1671,6 14,26 1683,917 1682,8 9,67 1693,582 1694,0 9,75 1703,329 1705,0 13,61 1716,936 1716,0 9,42 1726,355 1727,1 11,80 1738,155 1738,2 12,21 1750,366 1749,5 9,34 1759,702 1760,8 13,53 1773,228 1772,0 9,91 1783,139 1783,1
Spacing WN WO 9,75 1792,886 1794,1 14,35 1807,232 1805,0 8,19 1815,419 1815,9 12,70 1828,123 1826,9 11,14 1839,266 1838,1 8,27 1847,534 1849,3 14,59 1862,127 1860,4 9,25 1871,382 1871,5 10,16 1881,539 1882,5 13,28 1894,818 1893,5 9,34 1904,154 1904,7 12,54 1916,694 1915,9 11,47 1928,166 1927,2 9,75 1937,913 1938,4 13,61 1951,520 1949,6 9,58 1961,103 1960,5
Spacing WN WO 10,98 1972,082 1971,4 13,11 1985,196 1982,4 8,27 1993,465 1993,4 14,10 2007,565 2004,6 9,58 2017,148 2015,7 8,52 2025,663 2026,8 14,76 2040,420 2037,9 8,76 2049,181 2049,0
Interval of years 1761 - 1805 (with a centre around y. 1783) may be important. There would be solar-activity extremes expected on years marked by # (odd rows), but real activity was observed rather on years marked by asterisks:
Theory Jp J S U N Observation ------------------------------------------------------- # 1760,65 *** 14 326 358 6 143 1761.5 1765,96 14 136 66 27 154 # 1771,85 *** 14 305 146 51 167 1769.7 1777,08 *** 13 115 211 73 179 1778.4 # 1782,94 13 281 276 98 191 1788,14 *** 13 90 334 122 202 1788.1 # 1793,94 14 256 46 148 215 1799,14 14 63 117 173 226 # 1804,87 *** 15 229 191 200 238 1805.2
There is certain symmetry or perpendicularity, alignment of outer planets on the year. 1783 (see image of planetary position - Jupiter perihelion is on the right side of the image...!?)