| j | J, м/с2 | P1, Н | P2, Н | N, Н |
| 0 | 4935.32 | 8328.00 | -3272.12 | -60.67 |
| 10 | 4829.03 | 26445.00 | -3201.65 | 366.91 |
| 20 | 4496.79 | 17881.00 | -2981.37 | 637.14 |
| 30 | 3960.94 | 13472.00 | -2626.10 | 739.23 |
| 40 | 3257.46 | 10288.00 | -2159.69 | 741.49 |
| 50 | 2433.93 | 8083.00 | -1613.70 | 719.71 |
| 60 | 1546.14 | 6614.00 | -1025.09 | 713.09 |
| 70 | 652.92 | 5389.00 | -432.88 | 692.34 |
| 80 | -190.34 | 4654.00 | 126.20 | 703.34 |
| 90 | -938.37 | 3919.00 | 622.14 | 679.57 |
| 100 | -1561.41 | 3307.00 | 1035.22 | 638.90 |
| 110 | -2047.57 | 2694.00 | 1357.54 | 565.98 |
| 120 | -2401.70 | 2205.00 | 1592.33 | 484.50 |
| 130 | -2641.32 | 1837.00 | 1751.19 | 399.18 |
| 140 | -2790.99 | 1592.00 | 1850.42 | 314.03 |
| 150 | -2876.92 | 1225.00 | 1907.40 | 213.50 |
| 160 | -2922.73 | 1102.00 | 1937.77 | 129.99 |
| 170 | -2946.70 | 857.00 | 1953.66 | 44.37 |
| 180 | -2960.36 | 735.00 | 1962.72 | -32.38 |
| 190 | -2967.79 | -490.00 | 1967.64 | -58.83 |
| 200 | -2965.39 | -441.00 | 1966.05 | -101.98 |
| 210 | -2941.89 | -367.00 | 1950.47 | -146.30 |
| 220 | -2878.79 | -294.00 | 1908.64 | -186.67 |
| 230 | -2751.63 | -245.00 | 1824.33 | -214.48 |
| 240 | -2532.73 | 0.00 | 1679.20 | -255.74 |
| 250 | -2195.56 | 122.00 | 1455.66 | -259.58 |
| 260 | -1720.62 | 245.00 | 1140.77 | -238.44 |
| 270 | -1101.51 | 490.00 | 730.30 | -213.07 |
| 280 | -349.55 | 857.00 | 231.75 | -187.33 |
| 290 | 504.92 | 1225.00 | -334.76 | -146.47 |
| 300 | 1415.11 | 1715.00 | -938.22 | -118.30 |
| 310 | 2323.61 | 2205.00 | -1540.56 | -90.23 |
| 320 | 3169.66 | 2939.00 | -2101.48 | -96.83 |
| 330 | 3895.97 | 3429.00 | -2583.03 | -78.16 |
| 340 | 4454.13 | 4287.00 | -2953.09 | -89.20 |
| 350 | 4807.94 | 5389.00 | -3187.67 | -87.65 |
| 360 | 4935.32 | 8328.00 | -3272.12 | -60.67 |
Дезаксіальний КШМ (e=0.004 м)
| j | J, м/с2 | P1, Н | P2, Н | N, Н |
| 0 | 4935.73 | 8328.00 | -3272.39 | -80.90 |
| 10 | 4832.93 | 26445.00 | -3204.23 | 273.88 |
| 20 | 4504.23 | 17881.00 | -2986.30 | 577.20 |
| 30 | 3972.01 | 13472.00 | -2633.44 | 695.09 |
| 40 | 3272.21 | 10288.00 | -2169.47 | 707.74 |
| 50 | 2452.28 | 8083.00 | -1625.86 | 692.06 |
| 60 | 1567.79 | 6614.00 | -1039.45 | 688.43 |
| 70 | 677.26 | 5389.00 | -449.02 | 669.76 |
| 80 | -164.23 | 4654.00 | 108.88 | 681.14 |
| 90 | -911.64 | 3919.00 | 604.42 | 658.23 |
| 100 | -1535.30 | 3307.00 | 1017.90 | 618.50 |
| 110 | -2023.23 | 2694.00 | 1341.40 | 547.12 |
| 120 | -2380.05 | 2205.00 | 1577.97 | 467.18 |
| 130 | -2622.96 | 1837.00 | 1739.03 | 383.27 |
| 140 | -2776.24 | 1592.00 | 1840.65 | 299.24 |
| 150 | -2865.85 | 1225.00 | 1900.06 | 200.41 |
| 160 | -2915.29 | 1102.00 | 1932.84 | 117.61 |
| 170 | -2942.80 | 857.00 | 1951.08 | 33.09 |
| 180 | -2959.96 | 735.00 | 1962.45 | -43.16 |
| 190 | -2970.92 | -490.00 | 1969.72 | -64.85 |
| 200 | -2972.17 | -441.00 | 1970.55 | -108.45 |
| 210 | -2952.48 | -367.00 | 1957.50 | -153.40 |
| 220 | -2893.32 | -294.00 | 1918.27 | -194.42 |
| 230 | -2770.07 | -245.00 | 1836.56 | -222.69 |
| 240 | -2554.79 | 0.00 | 1693.82 | -264.99 |
| 250 | -2220.59 | 122.00 | 1472.25 | -268.95 |
| 260 | -1747.61 | 245.00 | 1158.67 | -247.39 |
| 270 | -1129.19 | 490.00 | 748.66 | -221.46 |
| 280 | -376.54 | 857.00 | 249.65 | 195.04 |
| 290 | 479.89 | 1225.00 | -318.17 | -152.98 |
| 300 | 1393.06 | 1715.00 | -923.60 | -123.81 |
| 310 | 2305.18 | 2205.00 | -1528.33 | -94.68 |
| 320 | 3155.13 | 2939.00 | -2091.85 | -101.40 |
| 330 | 3885.38 | 3429.00 | -2576.01 | -82.27 |
| 340 | 4447.35 | 4287.00 | -2948.59 | -94.89 |
| 350 | 4804.81 | 5389.00 | -3185.59 | -96.57 |
| 360 | 4935.73 | 8328.00 | -3272.39 | -80.90 |
Дезаксіальний КШМ (e=-0.001 м)
| j | J, м/с2 | P1, Н | P2, Н | N, Н |
| 0 | 4934.86 | 8328.00 | -3271.81 | 20.22 |
| 10 | 4814.53 | 26445.00 | -3192.03 | 739.44 |
| 20 | 4467.97 | 17881.00 | -2962.27 | 877.59 |
| 30 | 3917.36 | 13472.00 | -2597.21 | 916.72 |
| 40 | 3198.80 | 10288.00 | -2120.81 | 877.66 |
| 50 | 2360.44 | 8083.00 | -1564.97 | 831.66 |
| 60 | 1459.02 | 6614.00 | -967.33 | 813.32 |
| 70 | 554.65 | 5389.00 | -367.73 | 784.44 |
| 80 | -295.97 | 4654.00 | 196.23 | 794.08 |
| 90 | -1046.58 | 3919.00 | 693.88 | 766.90 |
| 100 | -1667.04 | 3307.00 | 1105.25 | 722.37 |
| 110 | -2145.84 | 2694.00 | 1422.69 | 643.12 |
| 120 | -2488.82 | 2205.00 | 1650.09 | 555.27 |
| 130 | -2714.81 | 1837.00 | 1799.92 | 464.05 |
| 140 | -2849.64 | 1592.00 | 1889.31 | 374.11 |
| 150 | -2920.50 | 1225.00 | 1936.29 | 266.49 |
| 160 | -2951.54 | 1102.00 | 1956.87 | 179.94 |
| 170 | -2961.20 | 857.00 | 1963.28 | 89.68 |
| 180 | -2960.82 | 735.00 | 1963.03 | 10.79 |
| 190 | -2954.17 | -490.00 | 1958.62 | -34.94 |
| 200 | -2937.32 | -441.00 | 1947.45 | -76.51 |
| 210 | -2898.85 | -367.00 | 1921.94 | -118.52 |
| 220 | -2820.38 | -294.00 | 1869.91 | -156.54 |
| 230 | -2678.04 | -245.00 | 1775.54 | -182.76 |
| 240 | -2445.15 | 0.00 | 1621.14 | -220.15 |
| 250 | -2096.51 | 122.00 | 1389.99 | -223.69 |
| 260 | -1613.98 | 245.00 | 1070.07 | -204.38 |
| 270 | -992.21 | 490.00 | 657.84 | -181.28 |
| 280 | -242.91 | 857.00 | 161.05 | -158.22 |
| 290 | 603.97 | 1225.00 | -400.43 | -121.99 |
| 300 | 1502.69 | 1715.00 | -996.28 | -97.60 |
| 310 | 2397.20 | 2205.00 | -1589.35 | -73.51 |
| 320 | 3228.06 | 2939.00 | -2140.21 | -79.35 |
| 330 | 3939.02 | 3429.00 | -2611.57 | -62.31 |
| 340 | 4482.19 | 4287.00 | -2971.69 | -66.80 |
| 350 | 4821.56 | 5389.00 | -3196.69 | -52.16 |
| 360 | 4934.86 | 8328.00 | -3271.81 | 20.23 |
Дезаксіальний КШМ (e=-0.002 м)
| j | J, м/с2 | P1, Н | P2, Н | N, Н |
| 0 | 4935.03 | 8328.00 | -3271.93 | 40.45 |
| 10 | 4811.18 | 26445.00 | -3189.81 | 832.69 |
| 20 | 4461.00 | 17881.00 | -2957.65 | 937.89 |
| 30 | 3906.63 | 13472.00 | -2590.10 | 961.34 |
| 40 | 3184.21 | 10288.00 | -2111.13 | 911.99 |
| 50 | 2342.03 | 8083.00 | -1552.77 | 860.00 |
| 60 | 1437.09 | 6614.00 | -952.79 | 838.79 |
| 70 | 529.83 | 5389.00 | -351.28 | 807.92 |
| 80 | -322.69 | 4654.00 | 213.94 | 817.26 |
| 90 | -1073.97 | 3919.00 | 712.04 | 789.23 |
| 100 | -1693.76 | 3307.00 | 1122.96 | 743.73 |
| 110 | -2170.65 | 2694.00 | 1439.14 | 662.85 |
| 120 | -2510.75 | 2205.00 | 1664.63 | 573.34 |
| 130 | -2733.21 | 1837.00 | 1812.12 | 480.57 |
| 140 | -2864.23 | 1592.00 | 1898.98 | 389.36 |
| 150 | -2931.23 | 1225.00 | 1943.40 | 279.91 |
| 160 | -2958.51 | 1102.00 | 1961.49 | 192.53 |
| 170 | -2964.55 | 857.00 | 1965.50 | 101.06 |
| 180 | -2960.65 | 735.00 | 1962.91 | 21.58 |
| 190 | -2950.49 | -490.00 | 1956.18 | -29.01 |
| 200 | -2930.07 | -441.00 | 1942.64 | -70.24 |
| 210 | -2887.92 | -367.00 | 1914.69 | -111.72 |
| 220 | -2805.70 | -294.00 | 1860.18 | -149.22 |
| 230 | -2659.68 | -245.00 | 1763.37 | -175.11 |
| 240 | -2423.40 | 0.00 | 1606.72 | -211.59 |
| 250 | -2072.00 | 122.00 | 1373.73 | -215.11 |
| 260 | -1587.64 | 245.00 | 1052.60 | -196.29 |
| 270 | -965.23 | 490.00 | 639.95 | -173.77 |
| 280 | -216.57 | 857.00 | 143.58 | -151.36 |
| 290 | 628.49 | 1225.00 | -416.69 | -116.25 |
| 300 | 1524.44 | 1715.00 | -1010.70 | -92.75 |
| 310 | 2415.57 | 2205.00 | -1601.52 | -69.60 |
| 320 | 3242.74 | 2939.00 | -2149.94 | -75.18 |
| 330 | 3949.94 | 3429.00 | -2618.81 | -58.49 |
| 340 | 4489.44 | 4287.00 | -2976.50 | -61.30 |
| 350 | 4825.24 | 5389.00 | -3199.13 | -43.33 |
| 360 | 4935.03 | 8328.00 | -3271.93 | 40.45 |
Дезаксіальний КШМ (e=-0.003 м)
| j | J, м/с2 | P1, Н | P2, Н | N, Н |
| 0 | 4935.32 | 8328.00 | -3272.12 | 60.67 |
| 10 | 4807.94 | 26445.00 | -3187.67 | 926.00 |
| 20 | 4454.13 | 17881.00 | -2953.09 | 998.26 |
| 30 | 3895.97 | 13472.00 | -2583.03 | 1006.05 |
| 40 | 3169.66 | 10288.00 | -2101.48 | 946.45 |
| 50 | 2323.61 | 8083.00 | -1540.56 | 888.48 |
| 60 | 1415.11 | 6614.00 | -938.22 | 864.42 |
| 70 | 504.92 | 5389.00 | -334.76 | 831.59 |
| 80 | -349.55 | 4654.00 | 231.75 | 840.65 |
| 90 | -1101.51 | 3919.00 | 730.30 | 811.78 |
| 100 | -1720.62 | 3307.00 | 1140.77 | 765.29 |
| 110 | -2195.57 | 2694.00 | 1455.66 | 682.76 |
| 120 | -2532.73 | 2205.00 | 1679.20 | 591.57 |
| 130 | -2751.63 | 1837.00 | 1824.33 | 497.22 |
| 140 | -2878.79 | 1592.00 | 1908.64 | 404.71 |
| 150 | -2941.89 | 1225.00 | 1950.47 | 293.39 |
| 160 | -2965.39 | 1102.00 | 1966.05 | 205.17 |
| 170 | -2967.79 | 857.00 | 1967.64 | 112.46 |
| 180 | -2960.36 | 735.00 | 1962.72 | 32.37 |
| 190 | -2946.70 | -490.00 | 1953.66 | -23.10 |
| 200 | -2922.73 | -441.00 | 1937.77 | -64.01 |
| 210 | -2876.92 | -367.00 | 1907.40 | -104.99 |
| 220 | -2790.99 | -294.00 | 1850.42 | -141.98 |
| 230 | -2641.32 | -245.00 | 1751.19 | -167.56 |
| 240 | -2401.70 | 0.00 | 1592.33 | -203.17 |
| 250 | -2047.57 | 122.00 | 1357.54 | -206.68 |
| 260 | -1561.41 | 245.00 | 1035.22 | -188.37 |
| 270 | -938.37 | 490.00 | 622.14 | -166.43 |
| 280 | -190.34 | 857.00 | 126.20 | -144.66 |
| 290 | 652.91 | 1225.00 | -432.88 | -110.65 |
| 300 | 1546.14 | 1715.00 | -1025.09 | -88.03 |
| 310 | 2433.93 | 2205.00 | -1613.70 | -65.78 |
| 320 | 3257.46 | 2939.00 | -2159.69 | -71.09 |
| 330 | 3960.94 | 3429.00 | -2626.10 | -54.72 |
| 340 | 4496.79 | 4287.00 | -2981.37 | -55.83 |
| 350 | 4829.03 | 5389.00 | -3201.64 | -34.53 |
| 360 | 4935.32 | 8328.00 | -3272.12 | 60.68 |
Дезаксіальний КШМ (e=-0.004 м)