0.066664 15.000506 1.1982% 1911 0.065875 15.180266 2.4765% 1910 1.208963 0.827155 3.8464% 1908 0.509779 1.961633 -2.5073% 1906 1.000000 1.000000 3.1640% 1986 4.821969 0.207384 2.6144% 1985 0.549747 1.819018 2.9715% 1984 0.887881 1.126277 3.6576% 1983 0.936875 1.067378 3.8998% 1982 3.367013 0.296999 6.3831% 1981 2.946740 0.339358 9.6843% 1980 12.791751 0.078175 9.0330% 1979 13.099832 0.076337 8.8650% 1978 2.831373 0.353186 7.2813% 1977 1.690927 0.591392 6.6558% 1976 3.252494 0.307456 6.4073% 1975 3.927121 0.254639 9.8159% 1974 3.698714 0.270364 9.0909% 1973 0.235939 4.238383 6.4509% 1972 5.812344 0.172048 4.7304% 1971 5.223540 0.191441 5.7132% 1970 5.915457 0.169049 5.5272% 1969 4.974911 0.201009 5.5714% 1968 0.350046 2.856765 5.0148% 1967 1.365019 0.732591 2.5719% 1966 2.317824 0.431439 3.5485% 1965 0.430026 2.325443 2.7360% 1964 2.611042 0.382989 1.5423% 1963 4.101343 0.243823 1.5697% 1962 3.666715 0.272724 2.2421% 1961 4.333112 0.230781 0.9709% 1960 1.292875 0.773470 1.6442% 1959 3.848161 0.259864 2.3579% 1958 0.848579
newt