0.420708 2.376946 -8.4517% 1930 0.338094 2.957755 -2.7367% 1929 0.431938 2.315146 0.0000% 1922 0.954220 1.047976 -0.6823% 1927 2.100047 0.476180 6.5229% 1941 0.137998 7.246508 6.1527% 1940 0.055085 18.153614 2.3623% 1939 0.654619 1.527606 -1.5482% 1938 0.074807 13.367804 -1.5312% 1937 1.637478 0.610695 3.9669% 1936 0.863062 1.158665 0.0000% 1935 0.424256 2.357069 3.2811% 1934 0.829942 1.204904 8.9328% 1933 0.266656 3.750152 -2.6088% 1932 0.320326 3.121818 -11.5407% 1931 0.822792 1.215374 2.3623% 1939 0.863945 1.157481 -1.5482% 1938 0.054660 18.294761 -1.5312% 1937 0.861870 1.160267 3.9669% 1936 0.863062 1.158665 3.2811% 1934 1.544324 0.647533 8.9328% 1933 0.079019 12.655131 -2.6088% 1932 0.170872 5.852334 -11.5407% 1931 1.140321 0.876946 -8.4517% 1930 0.225041 4.443633 -2.7367% 1929 1.972893 0.506870 2.8137% 1921 1.918901 0.521132 -2.7367% 1929 0.081409 12.283697 -0.6823% 1927 1.814881 0.551000 0.0000% 1926 0.078815 12.687878 0.0000% 1926 0.067372 14.843022 0.0000% 1926 0.389917 2.564646 0.0000% 1926 1.130769 0.884354 -2.0001% 1925 1.020409 0.979999 0.6731% 1924 0.490115 2.040338 2.0549% 1923 1.028137 0.972633 0.0000% 1928 0.170356 5.870053 2.8137% 1921 0.806814 1.239443 -2.7367% 1929 2.000000 0.500000 -0.6823% 1927 0.232963 4.292536 0.0000% 1926 1.860761 0.537414 6.5229% 1941 0.175568 5.695787 6.1527% 1940 1.857184 0.538450 -8.4517% 1930 0.356781 2.802838 -7.1894% 1920 1.047976 0.954220 -13.0688% 1919 0.080664 12.397096 15.7925% 1918 2.235269 0.447373 14.2845%
accelerations