6.1527% 1940 0.110731 9.030860 2.3623% 1939 1.671082 0.598415 -1.5482% 1938 0.113354 8.821954 -1.5312% 1937 0.891177 1.122112 3.9669% 1936 1.679960 0.595252 3.2811% 1934 1.605312 0.622932 8.9328% 1933 0.252245 3.964404 -2.6088% 1932 1.437411 0.695695 -11.5407% 1931 1.857184 0.538450 2.3623% 1939 0.076594 13.055788 -1.5482% 1938 0.290533 3.441950 -1.5312% 1937 0.088874 11.251890 3.9669% 1936 1.615505 0.619001 3.2811% 1934 1.742917 0.573751 8.9328% 1933 1.399912 0.714331 -2.6088% 1932 1.575334 0.634786 -11.5407% 1931 1.624941 0.615407 -8.4517% 1930 0.128043 7.809856 -2.7367% 1929 1.738120 0.575334 -0.6823% 1927 0.967115 1.034003 -2.0001% 1925 2.499937 0.400010 0.6731% 1924 1.182475 0.845684 2.0549% 1923 0.501708 1.993191 0.0000% 1928 1.972893 0.506870 0.0000% 1928 0.185744 5.383740 2.8137% 1921 0.946677 1.056327 -7.1894% 1920 0.503287 1.986939 1.3234% 1943 1.063390 0.940389 2.7232% 1942 0.494947 2.020417 0.0000% 1926 0.099727 10.027420 6.5229% 1941 2.059768 0.485491 6.1527% 1940 1.547672 0.646132 2.3623% 1939 0.835534 1.196839 -1.5482% 1938 0.859980 1.162818 -1.5312% 1937 0.064939 15.398980 3.9669% 1936 0.961845 1.039669 0.0000% 1935 0.187228 5.341090 3.2811%
thermostatic