% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 27783 % Primary Name: MONTGOMERY ALABAMA/GUNTER FLD % Record Type: TAVG % Country: United States % State: AL % Latitude: 32.40000 +/- 0.00500 % Longitude: -86.25000 +/- 0.00500 % Elevation (m): 67.00 +/- 0.05 % # of Months: 50 % % IDs: gsod - 749073-99999 % icao - GUN % usaf - 749073 % % Sources: Global Summary of the Day % % Site Hash: d5bb388aac3f6f6af4a8937131fc631b % Raw Data Hash: d854146e8875ab75ea611dcca1fd1c0f % Adj Data Hash: 7c8122da5bae944678f8c7ad7937561d % % 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 1940 12 NaN NaN NaN NaN NaN NaN 10.146 2.063 1941 1 NaN NaN NaN NaN NaN NaN 7.560 0.793 1941 2 NaN NaN NaN NaN NaN NaN 5.389 -3.324 1941 3 NaN NaN NaN NaN NaN NaN 9.506 -3.285 1941 4 NaN NaN NaN NaN NaN NaN 18.408 0.836 1941 5 NaN NaN NaN NaN NaN NaN 22.489 0.765 1941 6 NaN NaN NaN NaN NaN NaN 26.019 0.558 1941 7 NaN NaN NaN NaN NaN NaN 26.968 -0.063 1941 8 NaN NaN NaN NaN NaN NaN 26.895 0.181 1941 9 NaN NaN NaN NaN NaN NaN 25.991 2.037 1941 10 NaN NaN NaN NaN NaN NaN 21.480 4.031 1941 11 NaN NaN NaN NaN NaN NaN 11.506 -0.388 1941 12 10.585 1.383 1 0 NaN NaN 9.393 1.311 1942 1 7.391 -0.496 0 0 7.391 -0.496 5.214 -1.553 1942 2 7.482 -2.351 0 0 7.482 -2.351 5.855 -2.858 1942 3 13.319 -0.592 0 0 13.319 -0.592 12.361 -0.429 1942 4 18.720 0.028 0 0 18.720 0.028 17.904 0.332 1942 5 22.591 -0.252 0 0 22.591 -0.252 21.186 -0.538 1942 6 25.935 -0.646 0 0 25.935 -0.646 25.869 0.408 1942 7 27.072 -1.079 0 0 27.072 -1.079 27.172 0.142 1942 8 25.785 -2.049 1 0 NaN NaN 25.842 -0.872 1942 9 23.457 -1.616 0 0 23.457 -1.616 23.101 -0.852 1942 10 19.120 0.552 0 0 19.120 0.552 17.815 0.366 1942 11 14.372 1.358 0 0 14.372 1.358 13.462 1.568 1942 12 10.020 0.818 0 0 10.020 0.818 8.786 0.704 1943 1 10.278 2.391 0 0 10.278 2.391 8.348 1.580 1943 2 10.790 0.957 0 0 10.790 0.957 9.206 0.493 1943 3 13.057 -0.853 0 0 13.057 -0.853 11.657 -1.134 1943 4 18.706 0.014 0 0 18.706 0.014 17.564 -0.008 1943 5 24.480 1.636 0 0 24.480 1.636 22.943 1.219 1943 6 28.237 1.656 0 0 28.237 1.656 27.825 2.364 1943 7 27.892 -0.258 0 0 27.892 -0.258 27.673 0.642 1943 8 28.088 0.254 0 0 28.088 0.254 27.987 1.273 1943 9 23.348 -1.725 0 0 23.348 -1.725 22.597 -1.356 1943 10 17.758 -0.810 0 0 17.758 -0.810 16.059 -1.390 1943 11 11.859 -1.154 0 0 11.859 -1.154 10.422 -1.472 1943 12 9.115 -0.087 0 0 9.115 -0.087 7.528 -0.554 1944 1 9.047 1.160 0 0 9.047 1.160 7.012 0.245 1944 2 14.084 4.252 1 0 NaN NaN 11.519 2.806 1944 3 15.004 1.093 0 0 15.004 1.093 13.461 0.671 1944 4 17.533 -1.159 0 0 17.533 -1.159 16.679 -0.893 1944 5 23.599 0.755 0 0 23.599 0.755 22.268 0.544 1944 6 27.567 0.986 0 0 27.567 0.986 27.203 1.741 1944 7 27.041 -1.109 0 0 27.041 -1.109 26.547 -0.484 1944 8 26.204 -1.630 1 0 NaN NaN 26.296 -0.418 1944 9 25.107 0.034 0 0 25.107 0.034 24.672 0.718 1944 10 18.891 0.322 0 0 18.891 0.322 16.944 -0.505 1944 11 13.430 0.416 0 0 13.430 0.416 12.054 0.160 1944 12 8.570 -0.632 0 0 8.570 -0.632 7.148 -0.934 1945 1 8.866 0.979 0 0 8.866 0.979 6.855 0.088 1945 2 12.200 2.368 0 0 12.200 2.368 10.181 1.468 1945 3 18.754 4.844 0 0 18.754 4.844 17.464 4.674 1945 4 19.943 1.251 0 0 19.943 1.251 18.750 1.178 1945 5 21.738 -1.106 0 0 21.738 -1.106 20.137 -1.587 1945 6 27.296 0.715 0 0 27.296 0.715 26.197 0.736 1945 7 27.111 -1.039 0 0 27.111 -1.039 26.809 -0.222 1945 8 27.464 -0.370 0 0 27.464 -0.370 26.920 0.206 1945 9 25.896 0.823 0 0 25.896 0.823 25.879 1.926 1945 10 18.330 -0.239 0 0 18.330 -0.239 16.677 -0.772 1945 11 14.498 1.484 0 0 14.498 1.484 13.399 1.505 1945 12 6.201 -3.001 0 0 6.201 -3.001 4.984 -3.098 1946 1 3.704 -4.183 1 0 NaN NaN 7.695 0.928 1946 2 NaN NaN NaN NaN NaN NaN 9.441 0.729 1946 3 NaN NaN NaN NaN NaN NaN 15.745 2.955 1946 4 NaN NaN NaN NaN NaN NaN 19.185 1.613 1946 5 NaN NaN NaN NaN NaN NaN 20.843 -0.881 1946 6 NaN NaN NaN NaN NaN NaN 24.536 -0.925 1946 7 NaN NaN NaN NaN NaN NaN 26.132 -0.899 1946 8 NaN NaN NaN NaN NaN NaN 25.276 -1.439 1946 9 NaN NaN NaN NaN NaN NaN 23.059 -0.894 1946 10 NaN NaN NaN NaN NaN NaN 17.365 -0.084 1946 11 NaN NaN NaN NaN NaN NaN 15.328 3.434 1946 12 NaN NaN NaN NaN NaN NaN 10.263 2.181 1947 1 NaN NaN NaN NaN NaN NaN 9.079 2.312