% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 25109 % Primary Name: HOLME % Record Type: TAVG % Country: United Kingdom % Latitude: 53.80000 +/- 0.00500 % Longitude: -0.75000 +/- 0.00500 % Elevation (m): 4.00 +/- 0.05 % # of Months: 50 % % IDs: gsod - 749007-99999 % icao - EGCS % usaf - 749007 % % Sources: Global Summary of the Day % % Site Hash: 30d0eba860838aaaf53d4f1be535fcd0 % Raw Data Hash: 572f55b84b13740bd031b21a0ebec722 % Adj Data Hash: 199a1ed232ed3f846f9db21a4728a63f % % 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 9 NaN NaN NaN NaN NaN NaN 11.966 -0.941 1940 10 NaN NaN NaN NaN NaN NaN 9.134 -0.445 1940 11 NaN NaN NaN NaN NaN NaN 5.953 0.391 1940 12 NaN NaN NaN NaN NaN NaN 3.556 -0.002 1941 1 NaN NaN NaN NaN NaN NaN -0.457 -3.079 1941 2 NaN NaN NaN NaN NaN NaN 1.880 -1.155 1941 3 NaN NaN NaN NaN NaN NaN 4.160 -0.832 1941 4 NaN NaN NaN NaN NaN NaN 5.650 -1.595 1941 5 NaN NaN NaN NaN NaN NaN 8.787 -1.903 1941 6 NaN NaN NaN NaN NaN NaN 14.287 0.456 1941 7 NaN NaN NaN NaN NaN NaN 16.736 1.409 1941 8 NaN NaN NaN NaN NaN NaN 14.057 -0.987 1941 9 14.349 1.067 1 0 NaN NaN 14.053 1.146 1941 10 10.007 0.053 0 0 10.007 0.053 10.022 0.443 1941 11 6.383 0.446 0 0 6.383 0.446 5.516 -0.046 1941 12 4.833 0.900 0 0 4.833 0.900 5.040 1.482 1942 1 0.468 -2.530 0 0 0.468 -2.530 0.169 -2.454 1942 2 0.411 -2.999 0 0 0.411 -2.999 -0.620 -3.655 1942 3 4.357 -1.010 0 0 4.357 -1.010 4.029 -0.963 1942 4 8.267 0.646 0 0 8.267 0.646 7.853 0.608 1942 5 10.710 -0.355 0 0 10.710 -0.355 10.337 -0.353 1942 6 14.528 0.322 0 0 14.528 0.322 13.941 0.110 1942 7 15.575 -0.127 0 0 15.575 -0.127 14.812 -0.514 1942 8 16.491 1.072 0 0 16.491 1.072 15.664 0.620 1942 9 13.430 0.147 0 0 13.430 0.147 12.925 0.018 1942 10 10.376 0.422 0 0 10.376 0.422 10.150 0.571 1942 11 4.906 -1.031 0 0 4.906 -1.031 4.816 -0.746 1942 12 5.737 1.803 0 0 5.737 1.803 5.628 2.070 1943 1 3.789 0.791 0 0 3.789 0.791 3.299 0.676 1943 2 5.437 2.027 0 0 5.437 2.027 5.012 1.977 1943 3 6.672 1.305 0 0 6.672 1.305 6.264 1.272 1943 4 10.676 3.055 0 0 10.676 3.055 9.815 2.570 1943 5 11.952 0.887 0 0 11.952 0.887 11.284 0.594 1943 6 14.450 0.244 0 0 14.450 0.244 14.058 0.228 1943 7 16.124 0.422 0 0 16.124 0.422 15.364 0.037 1943 8 15.536 0.117 0 0 15.536 0.117 14.889 -0.155 1943 9 13.200 -0.082 0 0 13.200 -0.082 12.626 -0.282 1943 10 10.285 0.331 0 0 10.285 0.331 10.162 0.583 1943 11 5.333 -0.604 0 0 5.333 -0.604 5.272 -0.290 1943 12 3.459 -0.474 0 0 3.459 -0.474 3.487 -0.071 1944 1 5.477 2.479 0 0 5.477 2.479 4.888 2.265 1944 2 3.490 0.081 0 0 3.490 0.081 2.823 -0.212 1944 3 5.317 -0.050 0 0 5.317 -0.050 4.935 -0.057 1944 4 9.915 2.294 0 0 9.915 2.294 9.074 1.828 1944 5 11.600 0.535 1 0 NaN NaN 10.637 -0.053 1944 6 12.874 -1.332 0 0 12.874 -1.332 12.809 -1.022 1944 7 15.918 0.216 0 0 15.918 0.216 15.532 0.205 1944 8 16.170 0.751 0 0 16.170 0.751 15.900 0.855 1944 9 12.170 -1.112 0 0 12.170 -1.112 11.762 -1.145 1944 10 8.833 -1.121 0 0 8.833 -1.121 8.814 -0.765 1944 11 5.669 -0.268 0 0 5.669 -0.268 5.242 -0.320 1944 12 2.747 -1.186 0 0 2.747 -1.186 3.013 -0.545 1945 1 -0.263 -3.261 0 0 -0.263 -3.261 -0.260 -2.883 1945 2 6.752 3.342 0 0 6.752 3.342 5.962 2.927 1945 3 7.695 2.328 0 0 7.695 2.328 7.687 2.695 1945 4 9.315 1.694 0 0 9.315 1.694 9.036 1.791 1945 5 11.599 0.534 0 0 11.599 0.534 11.330 0.639 1945 6 14.268 0.063 0 0 14.268 0.063 14.142 0.311 1945 7 16.711 1.010 0 0 16.711 1.010 16.213 0.886 1945 8 14.959 -0.460 0 0 14.959 -0.460 14.894 -0.150 1945 9 13.809 0.527 0 0 13.809 0.527 13.582 0.675 1945 10 11.094 1.140 1 0 NaN NaN 11.222 1.643 1945 11 NaN NaN NaN NaN NaN NaN 6.815 1.252 1945 12 NaN NaN NaN NaN NaN NaN 4.362 0.804 1946 1 NaN NaN NaN NaN NaN NaN 2.184 -0.439 1946 2 NaN NaN NaN NaN NaN NaN 4.838 1.803 1946 3 NaN NaN NaN NaN NaN NaN 4.809 -0.183 1946 4 NaN NaN NaN NaN NaN NaN 9.104 1.859 1946 5 NaN NaN NaN NaN NaN NaN 9.974 -0.716 1946 6 NaN NaN NaN NaN NaN NaN 12.895 -0.936 1946 7 NaN NaN NaN NaN NaN NaN 15.574 0.248 1946 8 NaN NaN NaN NaN NaN NaN 13.875 -1.169 1946 9 NaN NaN NaN NaN NaN NaN 13.100 0.192 1946 10 NaN NaN NaN NaN NaN NaN 9.402 -0.177