% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 33528 % Primary Name: SUMNER % Record Type: TAVG % Country: United States % State: IL % Latitude: 38.71670 +/- 0.00005 % Longitude: -87.86670 +/- 0.00005 % Elevation (m): 139.90 +/- 0.15 % # of Months: 40 % % Alternate Names: Missing Station ID - 118419 % % IDs: coop - 118419 % ghcnd - USC00118419 % ncdc - 12001733 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: 991007dd6979e2e247ac6843b514aed5 % Raw Data Hash: e406e013343bcf32e1f463dc1dbf7724 % Adj Data Hash: e77bd3b2d79fb209b0095d03bbc1b0c4 % % The data for this station is presented below in several columns and in % several forms. The temperature values are reported as "raw", % "adjusted", and "regional expectation". % % The "raw" values reflect the observations as originally ingested by % the Berkeley Earth system from one or more originating archive(s). % These "raw" values may reflect the merger of more than one temperature % time series if multiple archives reported values for this location. % Alongside the raw data we have also provided a flag indicating which % values failed initial quality control checks. A further column % dates at which the raw data may be subject to continuity "breaks" % due to documented station moves (denoted "1"), prolonged measurement % gaps (denoted "2"), documented time of observation changes (denoted "3") % and other empirically determined inhomogeneities (denoted "4"). % % In many cases, raw temperature data contains a number of artifacts, % caused by issues such as typographical errors, instrumentation changes, % station moves, and urban or agricultural development near the station. % The Berkeley Earth analysis process attempts to identify and estimate % the impact of various kinds of data quality problems by comparing each % time series to neighboring series. At the end of the analysis process, % the "adjusted" data is created as an estimate of what the weather at % this location might have looked like after removing apparent biases. % This "adjusted" data will generally to be free from quality control % issues and be regionally homogeneous. Some users may find this % "adjusted" data that attempts to remove apparent biases more % suitable for their needs, while other users may prefer to work % with raw values. % % Lastly, we have provided a "regional expectation" time series, based % on the Berkeley Earth expected temperatures in the neighborhood of the % station. This incorporates information from as many weather stations as % are available for the local region surrounding this location. Note % that the regional expectation may be a systematically a bit warmer or % colder than the weather stations by a few degrees due to differences % in mean elevation and other local characteristics. % % For each temperature time series, we have also included an "anomaly" % time series that removes both the seasonality and the long-term mean. % These anomalies may provide an easier way of seeing changes through % time. % % Reported temperatures are in Celsius and reflect monthly averages. As % these files are intended to be summaries for convenience, additional % information, including more detailed flagging and metadata, may be % available in our whole data set files. % % The Berkeley Earth analysis was run on 15-Nov-2013 19:55:48 % % Raw Data QC Continuity Adjusted Data Regional Expectation % Year, Month, Temperature, Anomaly, Failed, Breaks, Temperature, Anomaly, Temperature, Anomaly 1907 10 NaN NaN NaN NaN NaN NaN 11.766 -1.384 1907 11 NaN NaN NaN NaN NaN NaN 4.719 -1.438 1907 12 NaN NaN NaN NaN NaN NaN 1.352 1.071 1908 1 NaN NaN NaN NaN NaN NaN -1.110 1.526 1908 2 NaN NaN NaN NaN NaN NaN -1.404 -1.118 1908 3 NaN NaN NaN NaN NaN NaN 7.858 2.648 1908 4 NaN NaN NaN NaN NaN NaN 12.173 0.083 1908 5 NaN NaN NaN NaN NaN NaN 17.766 0.212 1908 6 NaN NaN NaN NaN NaN NaN 21.916 -0.598 1908 7 NaN NaN NaN NaN NaN NaN 24.243 -0.243 1908 8 NaN NaN NaN NaN NaN NaN 23.576 0.120 1908 9 NaN NaN NaN NaN NaN NaN 21.876 2.047 1908 10 13.779 -0.532 1 0 NaN NaN 13.178 0.027 1908 11 7.532 0.213 0 0 7.532 0.213 7.165 1.008 1908 12 2.889 1.445 0 0 2.889 1.445 1.613 1.332 1909 1 0.833 2.308 0 0 0.833 2.308 -0.837 1.799 1909 2 3.832 2.956 0 0 3.832 2.956 2.129 2.415 1909 3 6.323 -0.049 0 0 6.323 -0.049 4.671 -0.538 1909 4 12.728 -0.522 0 0 12.728 -0.522 11.517 -0.572 1909 5 16.976 -1.740 0 0 16.976 -1.740 15.618 -1.936 1909 6 23.335 -0.340 0 0 23.335 -0.340 22.828 0.314 1909 7 23.452 -2.196 0 0 23.452 -2.196 22.645 -1.841 1909 8 24.881 0.263 0 0 24.881 0.263 24.283 0.827 1909 9 19.610 -1.380 0 0 19.610 -1.380 18.740 -1.089 1909 10 12.132 -2.180 0 0 12.132 -2.180 10.843 -2.307 1909 11 11.700 4.381 0 0 11.700 4.381 11.192 5.035 1909 12 -3.034 -4.477 0 0 -3.034 -4.477 -4.619 -4.900 1910 1 -0.456 1.018 0 0 -0.456 1.018 -2.412 0.224 1910 2 -1.186 -2.062 0 0 -1.186 -2.062 -3.102 -2.816 1910 3 12.456 6.085 0 0 12.456 6.085 10.884 5.674 1910 4 12.760 -0.491 0 0 12.760 -0.491 12.194 0.105 1910 5 16.066 -2.650 0 0 16.066 -2.650 14.529 -3.025 1910 6 21.743 -1.932 0 0 21.743 -1.932 20.860 -1.654 1910 7 24.866 -0.781 0 0 24.866 -0.781 23.925 -0.561 1910 8 23.084 -1.534 0 0 23.084 -1.534 22.086 -1.370 1910 9 20.567 -0.424 0 0 20.567 -0.424 20.266 0.437 1910 10 14.858 0.546 0 0 14.858 0.546 14.559 1.408 1910 11 4.953 -2.366 0 0 4.953 -2.366 3.618 -2.539 1910 12 -1.192 -2.635 0 0 -1.192 -2.635 -2.569 -2.851 1911 1 2.102 3.576 0 0 2.102 3.576 -0.346 2.290 1911 2 3.998 3.122 0 0 3.998 3.122 2.080 2.366 1911 3 7.285 0.914 0 0 7.285 0.914 5.440 0.231 1911 4 12.002 -1.249 0 0 12.002 -1.249 10.781 -1.308 1911 5 20.483 1.767 0 0 20.483 1.767 19.968 2.414 1911 6 24.520 0.845 0 0 24.520 0.845 23.862 1.348 1911 7 24.626 -1.021 0 0 24.626 -1.021 24.027 -0.458 1911 8 24.265 -0.353 0 0 24.265 -0.353 23.237 -0.218 1911 9 22.668 1.678 0 0 22.668 1.678 21.910 2.082 1911 10 14.281 -0.031 0 0 14.281 -0.031 13.023 -0.128 1911 11 3.993 -3.326 0 0 3.993 -3.326 3.149 -3.009 1911 12 3.474 2.031 0 0 3.474 2.031 2.551 2.269 1912 1 -6.392 -4.918 0 0 -6.392 -4.918 -8.600 -5.964 1912 2 NaN NaN NaN NaN NaN NaN -5.045 -4.759 1912 3 NaN NaN NaN NaN NaN NaN 0.666 -4.543 1912 4 NaN NaN NaN NaN NaN NaN 13.062 0.973 1912 5 NaN NaN NaN NaN NaN NaN 18.225 0.671 1912 6 NaN NaN NaN NaN NaN NaN 20.506 -2.007 1912 7 NaN NaN NaN NaN NaN NaN 24.106 -0.380 1912 8 NaN NaN NaN NaN NaN NaN 22.248 -1.208 1912 9 NaN NaN NaN NaN NaN NaN 20.689 0.860 1912 10 NaN NaN NaN NaN NaN NaN 13.611 0.461 1912 11 NaN NaN NaN NaN NaN NaN 6.168 0.011 1912 12 NaN NaN NaN NaN NaN NaN 1.361 1.080 1913 1 NaN NaN NaN NaN NaN NaN 0.649 3.285