1879 0.610695 1.637478 5.2689% 1905 0.499996 2.000017 -3.7992% 1877 0.233725 4.278542 -5.9492% 1876 0.324306 3.083508 1.1977% 1911 0.139970 7.144410 2.4765% 1910 1.094533 0.913632 3.8464% 1908 0.217262 4.602743 -2.5073% 1906 0.579737 1.724919 5.2689% 1878 0.904776 1.105246 -3.7992% 1877 0.612417 1.632875 -3.6586% 1881 0.206026 4.853747 2.4963% 1880 0.952448 1.049926 0.0000% 1879 1.176512 0.849970 0.0000% 1879 0.620192 1.612404 5.2689% 1878 0.926812 1.078967 -3.7992% 1877 0.448856 2.227886 -5.9492% 1876 0.531632 1.881000 1.1977% 1911 0.553353 1.807165 2.4765% 1910 1.208963 0.827155 0.0000% 1909 0.460203 2.172954 0.0000% 1909 0.203506 4.913850 0.0000% 1909 0.163630 6.111351 0.0000% 1909 0.030511 32.774590 3.8464% 1908 0.493656 2.025702 0.0000% 1907 0.222849 4.487335 0.0000% 1907 0.033050 30.257197 -2.5073% 1906 0.044610 22.416480 5.2689% 1878 0.105261 9.500232 2.6987% 1904 0.176192 5.675640 -1.3372% 1883 0.892941 1.119895 0.0000% 1887 1.013553 0.986628 1.3553% 1886 0.039677 25.203794 1.3740% 1902 0.077658 12.877052 -2.6744% 1888 1.119518 0.893242 0.0000% 1887 0.882404 1.133267 -5.0576% 1882 0.071235 14.038135 -3.6586% 1881 1.223934 0.817038 2.4963%
thermostatic