% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 36424 % Primary Name: MAXON % Record Type: TAVG % Country: United States % State: IA % Latitude: 41.03330 +/- 0.00005 % Longitude: -92.78330 +/- 0.00005 % Elevation (m): 274.32 +/- 0.15 % # of Months: 45 % % Alternate Names: Missing Station ID - 135290 % % IDs: coop - 135290 % ghcnd - USC00135290 % ncdc - 30002436 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: 3d972ea4eeaf18dde596c735aa3a3b51 % Raw Data Hash: 2d1f23b17406b10b483ffd14af9f8844 % Adj Data Hash: babacdb4685781d3e8feedce0a1a0ebd % % 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 1892 1 NaN NaN NaN NaN NaN NaN -8.823 -2.211 1892 2 NaN NaN NaN NaN NaN NaN -1.116 2.042 1892 3 NaN NaN NaN NaN NaN NaN 0.321 -2.171 1892 4 NaN NaN NaN NaN NaN NaN 8.988 -1.519 1892 5 NaN NaN NaN NaN NaN NaN 13.163 -3.562 1892 6 NaN NaN NaN NaN NaN NaN 21.256 -0.500 1892 7 NaN NaN NaN NaN NaN NaN 23.462 -0.879 1892 8 NaN NaN NaN NaN NaN NaN 22.412 -0.693 1892 9 NaN NaN NaN NaN NaN NaN 18.736 0.297 1892 10 NaN NaN NaN NaN NaN NaN 13.243 0.944 1892 11 NaN NaN NaN NaN NaN NaN 2.087 -2.042 1892 12 NaN NaN NaN NaN NaN NaN -6.203 -3.363 1893 1 -10.132 -4.061 1 0 NaN NaN -12.060 -5.449 1893 2 -7.560 -4.941 1 0 NaN NaN -7.302 -4.144 1893 3 0.430 -2.602 0 0 0.430 -2.602 0.262 -2.230 1893 4 8.333 -2.714 0 0 8.333 -2.714 8.916 -1.591 1893 5 14.537 -2.727 0 0 14.537 -2.727 14.382 -2.342 1893 6 23.103 0.807 0 0 23.103 0.807 21.885 0.129 1893 7 25.520 0.639 0 0 25.520 0.639 24.533 0.192 1893 8 22.061 -1.584 0 0 22.061 -1.584 21.373 -1.732 1893 9 19.315 0.336 0 0 19.315 0.336 19.146 0.707 1893 10 12.097 -0.742 0 0 12.097 -0.742 13.258 0.959 1893 11 1.204 -3.465 0 0 1.204 -3.465 2.664 -1.465 1893 12 -4.713 -2.413 0 0 -4.713 -2.413 -3.926 -1.086 1894 1 -6.487 -0.416 0 0 -6.487 -0.416 -6.320 0.291 1894 2 -6.429 -3.810 0 0 -6.429 -3.810 -5.830 -2.671 1894 3 5.383 2.351 0 0 5.383 2.351 5.203 2.711 1894 4 11.630 0.583 0 0 11.630 0.583 11.997 1.489 1894 5 15.093 -2.171 0 0 15.093 -2.171 16.578 -0.146 1894 6 24.556 2.260 0 0 24.556 2.260 23.421 1.665 1894 7 26.703 1.822 0 0 26.703 1.822 25.250 0.909 1894 8 27.163 3.518 0 0 27.163 3.518 24.603 1.497 1894 9 19.574 0.595 0 0 19.574 0.595 18.970 0.532 1894 10 11.852 -0.987 0 0 11.852 -0.987 12.572 0.272 1894 11 0.259 -4.410 0 0 0.259 -4.410 1.737 -2.392 1894 12 -0.148 2.152 0 0 -0.148 2.152 -0.275 2.565 1895 1 -7.991 -1.920 0 0 -7.991 -1.920 -9.398 -2.787 1895 2 -3.283 -0.664 0 0 -3.283 -0.664 -7.362 -4.204 1895 3 3.011 -0.021 0 0 3.011 -0.021 1.533 -0.960 1895 4 13.199 2.152 0 0 13.199 2.152 12.874 2.367 1895 5 17.874 0.609 0 0 17.874 0.609 17.119 0.394 1895 6 23.175 0.879 0 0 23.175 0.879 21.288 -0.468 1895 7 23.710 -1.170 1 0 NaN NaN 22.409 -1.932 1895 8 23.808 0.163 0 0 23.808 0.163 22.924 -0.181 1895 9 21.782 2.803 0 0 21.782 2.803 20.271 1.832 1895 10 9.211 -3.628 0 0 9.211 -3.628 9.292 -3.008 1895 11 3.745 -0.924 0 0 3.745 -0.924 2.461 -1.668 1895 12 -1.907 0.393 0 0 -1.907 0.393 -2.880 -0.040 1896 1 -3.136 2.935 0 0 -3.136 2.935 -4.707 1.904 1896 2 -1.528 1.091 0 0 -1.528 1.091 -1.549 1.610 1896 3 0.789 -2.243 0 0 0.789 -2.243 -0.545 -3.037 1896 4 14.519 3.471 0 0 14.519 3.471 13.869 3.362 1896 5 20.036 2.772 0 0 20.036 2.772 19.042 2.317 1896 6 21.611 -0.685 0 0 21.611 -0.685 21.207 -0.549 1896 7 23.710 -1.171 1 0 NaN NaN 22.969 -1.372 1896 8 23.907 0.262 0 0 23.907 0.262 22.229 -0.876 1896 9 15.519 -3.460 0 0 15.519 -3.460 15.173 -3.266 1896 10 NaN NaN NaN NaN NaN NaN 10.413 -1.886 1896 11 NaN NaN NaN NaN NaN NaN 0.669 -3.460 1896 12 NaN NaN NaN NaN NaN NaN 0.964 3.804 1897 1 NaN NaN NaN NaN NaN NaN -7.595 -0.984 1897 2 NaN NaN NaN NaN NaN NaN -2.913 0.246 1897 3 NaN NaN NaN NaN NaN NaN 0.966 -1.527 1897 4 NaN NaN NaN NaN NaN NaN 9.911 -0.597 1897 5 NaN NaN NaN NaN NaN NaN 15.350 -1.374 1897 6 NaN NaN NaN NaN NaN NaN 21.421 -0.335 1897 7 NaN NaN NaN NaN NaN NaN 24.741 0.400 1897 8 NaN NaN NaN NaN NaN NaN 21.235 -1.871 1897 9 NaN NaN NaN NaN NaN NaN 22.427 3.988