0.788200 1.1940% 1912 0.083997 11.905256 -1.1800% 1875 0.555551 1.800015 YEAR: 1919 2010 16.313737 0.061298 4% Est. 2007 34.493147 0.028991 4% Est. 2008 32.373715 0.030889 4% Est. 2004 26.696472 0.037458 4% Est. 2009 2.106849 0.474642 4% Est. 1989 17.026783 0.058731 3.8744% 1988 15.960956 0.062653 3.3218% 1987 8.041339 0.124357 3.1640% 1986 3.647419 0.274166 2.6144% 1985 13.524532 0.073940 2.9715% 1984 0.759882 1.315994 3.6576% 1983 14.429759 0.069301 3.8998% 1982 2.785536 0.358997 6.3831% 1981 12.051824 0.082975 9.6843% 1980 10.202853 0.098012 9.0330% 1979 9.034759 0.110684 8.8650% 1978 1.144217 0.873960 7.2813% 1977 9.614519 0.104009 6.6558% 1976 5.007780 0.199689 6.4073% 1975 7.906295 0.126481 9.8159% 1974 0.211554 4.726922 9.0909% 1973 4.304469 0.232317 6.4509% 1972 1.654795 0.604305 4.7304% 1971 3.415395 0.292792 5.7132% 1970 0.234197 4.269902 5.5272% 1969 5.853043 0.170851 5.5714% 1968 2.582265 0.387257 5.0148% 1967 4.432260 0.225619 2.5719% 1966 2.380942 0.420002 3.5485% 1965 4.278542 0.233725 2.7360% 1964 2.150327 0.465046 1.5423% 1963 4.101343 0.243823 1.5697% 1962 4.310705 0.231981 2.2421% 1961 5.199916 0.192311 0.9709% 1960 4.291446 0.233022 1.6442% 1959 0.653767 1.529597 2.3579% 1958 4.433047 0.225578 2.0623% 1957 3.829017 0.261164 3.5571% 1956 1.911594 0.523124 3.3098% 1955 3.399896 0.294127 3.4226% 1954 0.164962 6.062018 1.5421% 1953
physic