The table is subdivided into two parts:
Simulation 1 is almost the same as simulation 1, only the starting date is different. The starting date for simulation 2 is:
Simulation 1 and 2 are identical for the values in column 1.
Simulation 1 and 2 are not identical for the values in column 2 and 3.
The reason is because:
The first value in column 1 of simulation 1 is 3363.86. This value is not included in simulation 2.
The last value in column 1 of simulation 2 is -587.89. This value is not included in simulation 1.
The averaged difference is:
The last value of simulation 3 column 3 is 618.81.
This value represents the final averaged value after 420 revolutions when the Sun moves away from Aphelion. This is 93.40 more than the final value 525.41 of simulation 1 column 3.
That is the maximum case.
In the opposite case the Sun would move towards Aphelion. The result of a simulation under those conditions gives a final average value of 430.41 arc seconds. This is 95.00 less than the final value 525.41 of simulation 1 column 3.
That is the minimum case.
This means many other values are possible including 574 arc sec per century.
The final value in the third column of simulation 1 (525.61) and 2 (518.14) should both have been equal to 531 arc seconds per century.
In order to improve the simulation one method is to increase the number of planets. One can divide each planet in two parts, which each half the mass of the original planet. The second planet of each is placed 180 degrees forward.
The forward angle after 420 revolutions in simulation 1 is than 529.04 arc seconds.
The forward angle after 420 revolutions in simulation 2 is than 524.78 arc seconds.
The most important aspect of simulation 3 is to demonstrate that it is possible to simulate the movement of the planet Mercury without the Relativity Theory.
The most important assumption for this simulation is that the speed of gravity propagation is much larger than c.
For a more technical description see:The Reality, Now and Understanding
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The simulation more or less starts the first time when Mercury reaches aphelion. (furtest distance). This defines angle 0.
The second time when Mercury reaches aphelion defines angle 1. The differences between angle 1 and angle 0 defines the first red dot (left bottom corner)
The third time when Mercury reaches aphelion defines angle 2. The differences between angle 2 and angle 0 defines the second red dot.
The fourth time when Mercury reaches aphelion defines angle 3. The differences between angle 3 and angle 0 defines the third red dot
This angle slowly increases, which explains the 45 angle.
The yellow line is more or less the same as the red line (dots), but now a more or less running averege is shown. (running squared distance).
The red dots define an angle as a function of a running time. The blue line defines also an angle but the time period is fixed i.e. 100 years. That is why the line of 45 degrees and the horizontal line cross each other at a distance 100 years after the origin. In this case this angle is 276.8 arc secs.
The pink line defines again the running average.
What is important to see that the forward movement angle is rather irregular. This is caused because the distance between Venus and Mercury is rather irregular. Specific the average distance during one revolution of Mercury depents very much on the average position of Venus. The influence is very different when Venus is on average closer to aphelion as to perihelion.
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simulation 1 simulation 2 Rev delta a a av(a) delta a a av(a) 0 0.0 1 3363.86 3363.86 3363.90 0.0 2 335.95 1849.91 1849.92 313.81 313.81 313.81 3 -399.63 1100.07 1140.94 -353.13 -19.66 -19.66 4 246.71 886.73 875.03 325.99 95.56 57.83 5 3302.44 1369.87 1103.13 3127.86 853.64 609.54 6 921.91 1295.21 1170.31 783.60 839.63 775.86 7 -670.02 1014.47 1077.78 -652.37 590.97 706.50 8 -352.88 843.55 961.24 -251.47 470.62 612.89 9 1408.51 906.32 921.29 1557.30 606.45 617.66 10 -174.39 798.25 862.28 -290.78 506.76 581.62 11 -995.27 635.21 774.75 -1040.94 351.99 505.47 12 -1540.39 453.91 664.78 -1532.59 180.67 401.92 13 689.70 472.04 595.69 833.82 235.10 349.09 14 1678.91 558.25 570.49 1854.24 359.65 347.32 15 -952.28 457.55 529.31 -981.19 263.87 321.90 16 -1925.82 308.59 466.01 -1956.12 115.87 268.04 17 -1323.82 212.56 398.53 -1342.39 24.73 207.66 18 2108.92 317.92 369.25 2288.32 157.89 191.16 19 4057.99 514.77 385.70 4020.93 372.50 222.85 20 -1110.38 433.51 384.45 -1130.95 293.37 232.55 -1316.09 212.90 225.56 400 -455.71 529.08 525.22 401 4298.61 538.48 525.35 4189.17 531.65 518.51 402 1635.48 541.21 525.51 1509.01 534.09 518.69 403 -936.71 537.54 525.62 -919.47 530.47 518.82 404 -1116.90 533.45 525.70 -1074.88 526.49 518.91 405 280.97 532.82 525.77 361.21 526.08 519.00 406 802.11 533.49 525.85 676.16 526.45 519.09 407 -716.81 530.42 525.89 -792.41 523.20 519.14 408 -1223.36 526.12 525.89 -1233.10 518.89 519.16 409 -108.37 524.57 525.88 -19.80 517.57 519.16 410 534.19 524.59 525.87 665.62 517.93 519.16 411 -747.67 521.49 525.82 -823.88 514.65 519.14 412 -678.07 518.58 525.75 -734.71 511.61 519.08 413 -924.61 515.09 525.65 -922.09 508.14 518.99 414 1133.07 516.58 525.56 1259.47 509.95 518.92 415 3121.89 522.86 525.54 3221.45 516.50 518.91 416 192.21 522.06 525.50 159.27 515.64 518.89 417 -994.19 518.43 525.43 -1006.54 511.98 518.84 418 -477.60 516.04 525.34 -483.63 509.60 518.77 419 3797.18 523.88 525.33 3896.40 517.70 518.77 420 4737.21 533.91 525.41 4652.45 527.57 518.87 421 -587.89 524.91 518.95
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simulation 3 Rev delta a a av(a) 0 0.0 1 3457.32 3457.32 3457.37 2 429.40 1943.37 1943.39 3 -306.16 1193.53 1234.40 4 339.90 980.12 968.45 5 3396.18 1463.34 1196.57 6 1015.40 1388.68 1263.76 7 -576.55 1107.94 1171.24 8 -259.68 936.98 1054.69 9 1501.04 999.66 1014.70 10 -80.86 891.61 955.67 11 -901.26 728.62 868.14 12 -1447.17 547.31 758.18 13 782.03 565.36 689.06 14 1771.24 651.50 663.83 15 -858.26 550.84 622.63 16 -1831.73 401.94 559.34 17 -1231.14 305.87 491.85 18 2201.43 411.18 462.56 19 4151.59 608.05 479.00 20 -1016.87 526.80 477.75 400 -332.07 622.59 618.62 401 4353.64 631.89 618.75 402 1666.33 634.46 618.91 403 -847.61 630.79 619.02 404 -982.80 626.79 619.10 405 405.54 626.24 619.17 406 828.59 626.74 619.24 407 -657.66 623.59 619.28 408 -1093.57 619.38 619.28 409 -4.46 617.85 619.27 410 691.65 618.03 619.26 411 -686.27 614.86 619.22 412 -587.09 611.94 619.14 413 -862.82 608.37 619.04 414 1298.98 610.04 618.95 415 3263.51 616.43 618.93 416 271.05 615.60 618.90 417 -937.53 611.88 618.83 418 -369.65 609.53 618.74 419 3947.11 617.50 618.73 420 4764.98 627.37 618.81
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