0.884354 0.0000% 1926 0.121186 8.251770 -2.0001% 1925 0.337837 2.960007 0.6731% 1924 0.086405 11.573424 2.0549% 1923 1.921049 0.520549 0.0000% 1922 0.406677 2.458954 -0.6823% 1927 1.750060 0.571409 -2.0001% 1925 0.533800 1.873361 0.6731% 1924 0.065661 15.229842 2.0549% 1923 0.099046 10.096306 2.8137% 1921 0.180661 5.535222 -7.1894% 1920 0.121429 8.235265 -13.0688% 1919 0.176002 5.681767 15.7925% 1918 0.193380 5.171172 14.2845% 1917 0.426278 2.345886 16.6637% 1916 0.256763 3.894648 20.0069% 1915 0.281052 3.558055 9.1939% 1914 0.763125 1.310402 2.3510% 1913 1.214314 0.823510 1.1940% 1912 0.041638 24.016441 -1.1800% 1875 0.582204 1.717610 1.1940% 1912 0.575334 1.738120 1.1977% 1911 0.268616 3.722793 2.4765% 1910 1.094533 0.913632 3.8464% 1908 0.043492 22.992989 0.0000% 1907 0.035747 27.974476 -2.5073% 1906 0.975645 1.024963 0.0000% 1879 0.308885 3.237456 5.2689% 1878 0.224845 4.447510 2.6987% 1904 0.239485 4.175631 1.3740% 1902 0.025424 39.333184 -1.3553%
thermal