% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 15938 % Primary Name: CERIGNOLA/MU % Record Type: TAVG % Country: Italy % Latitude: -41.26600 +/- 0.00050 % Longitude: 15.91600 +/- 0.00050 % Elevation (m): 123.00 +/- 0.05 % # of Months: 18 % % IDs: gsod - 749499-99999 % usaf - 749499 % % Sources: Global Summary of the Day % % Site Hash: c139f963f1703e3d7ec0c86aa849b233 % Raw Data Hash: 06d4d8bdee1393b5aa95b7b164ecacd2 % Adj Data Hash: 5e49cb27837732183db8186800603c3b % % 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 1942 12 NaN NaN NaN NaN NaN NaN 10.119 0.025 1943 1 NaN NaN NaN NaN NaN NaN 9.920 -0.809 1943 2 NaN NaN NaN NaN NaN NaN 10.339 -0.603 1943 3 NaN NaN NaN NaN NaN NaN 11.157 0.420 1943 4 NaN NaN NaN NaN NaN NaN 10.205 -0.064 1943 5 NaN NaN NaN NaN NaN NaN 9.762 -0.563 1943 6 NaN NaN NaN NaN NaN NaN 9.839 -0.270 1943 7 NaN NaN NaN NaN NaN NaN 8.406 -0.785 1943 8 NaN NaN NaN NaN NaN NaN 8.635 -0.075 1943 9 NaN NaN NaN NaN NaN NaN 8.704 0.024 1943 10 NaN NaN NaN NaN NaN NaN 8.447 -0.402 1943 11 NaN NaN NaN NaN NaN NaN 9.952 0.301 1943 12 9.246 -3.631 1 0 NaN NaN 10.948 0.853 1944 1 6.980 -6.531 1 0 NaN NaN 11.654 0.925 1944 2 NaN NaN NaN NaN NaN NaN 11.911 0.969 1944 3 7.659 -5.861 1 0 NaN NaN 11.072 0.334 1944 4 14.402 1.350 0 0 14.402 1.350 10.590 0.321 1944 5 18.604 5.497 1 0 NaN NaN 10.765 0.441 1944 6 23.219 10.326 1 0 NaN NaN 10.120 0.011 1944 7 25.367 13.393 1 0 NaN NaN 9.292 0.100 1944 8 25.688 14.195 1 0 NaN NaN 8.307 -0.403 1944 9 22.224 10.762 1 0 NaN NaN 9.008 0.329 1944 10 16.301 4.669 1 0 NaN NaN 9.257 0.407 1944 11 12.052 -0.382 0 0 12.052 -0.382 9.016 -0.634 1944 12 8.392 -4.485 1 0 NaN NaN 9.013 -1.081 1945 1 4.670 -8.841 1 0 NaN NaN 10.432 -0.297 1945 2 8.019 -5.706 1 0 NaN NaN 10.759 -0.183 1945 3 10.823 -2.698 0 0 10.823 -2.698 11.102 0.364 1945 4 15.743 2.691 0 0 15.743 2.691 11.178 0.909 1945 5 22.283 9.176 1 0 NaN NaN 11.392 1.067 1945 6 25.032 12.139 1 0 NaN NaN 10.781 0.671 1945 7 NaN NaN NaN NaN NaN NaN 8.661 -0.531 1945 8 NaN NaN NaN NaN NaN NaN 9.062 0.352 1945 9 NaN NaN NaN NaN NaN NaN 9.573 0.894 1945 10 NaN NaN NaN NaN NaN NaN 8.744 -0.105 1945 11 NaN NaN NaN NaN NaN NaN 10.117 0.466 1945 12 NaN NaN NaN NaN NaN NaN 9.301 -0.794 1946 1 NaN NaN NaN NaN NaN NaN 10.453 -0.276 1946 2 NaN NaN NaN NaN NaN NaN 10.806 -0.136 1946 3 NaN NaN NaN NaN NaN NaN 10.169 -0.568 1946 4 NaN NaN NaN NaN NaN NaN 10.347 0.078 1946 5 NaN NaN NaN NaN NaN NaN 10.309 -0.015 1946 6 NaN NaN NaN NaN NaN NaN 9.752 -0.357