% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 16024 % Primary Name: SPINAZZOLA ITALY/MU 10 % Record Type: TAVG % Country: Italy % Latitude: 40.95000 +/- 0.00050 % Longitude: 16.09900 +/- 0.00050 % Elevation (m): 437.00 +/- 0.05 % # of Months: 15 % % IDs: gsod - 749297-99999 % usaf - 749297 % % Sources: Global Summary of the Day % % Site Hash: b4c9e312457f4d9229fb07cf31e82760 % Raw Data Hash: d6aaf21e3a7f9ab00a48e8de0ba9c2dc % Adj Data Hash: 02042fbcf22d7faa5bd4746655ef610e % % 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 1943 3 NaN NaN NaN NaN NaN NaN 10.753 0.319 1943 4 NaN NaN NaN NaN NaN NaN 14.015 0.903 1943 5 NaN NaN NaN NaN NaN NaN 17.375 -0.264 1943 6 NaN NaN NaN NaN NaN NaN 20.879 -1.073 1943 7 NaN NaN NaN NaN NaN NaN 24.529 -0.012 1943 8 NaN NaN NaN NaN NaN NaN 26.446 1.886 1943 9 NaN NaN NaN NaN NaN NaN 23.889 2.638 1943 10 NaN NaN NaN NaN NaN NaN 18.073 1.472 1943 11 NaN NaN NaN NaN NaN NaN 13.429 0.645 1943 12 NaN NaN NaN NaN NaN NaN 11.105 1.566 1944 1 NaN NaN NaN NaN NaN NaN 8.239 0.193 1944 2 NaN NaN NaN NaN NaN NaN 7.434 -1.332 1944 3 5.941 -3.213 1 0 NaN NaN 7.542 -2.892 1944 4 12.513 0.681 0 0 12.513 0.681 13.329 0.217 1944 5 16.581 0.221 0 0 16.581 0.221 17.443 -0.196 1944 6 21.572 0.900 0 0 21.572 0.900 22.251 0.300 1944 7 23.633 0.371 0 0 23.633 0.371 24.260 -0.281 1944 8 23.980 0.700 0 0 23.980 0.700 25.065 0.505 1944 9 20.674 0.703 0 0 20.674 0.703 21.506 0.254 1944 10 14.763 -0.559 0 0 14.763 -0.559 16.257 -0.345 1944 11 10.050 -1.455 0 0 10.050 -1.455 12.377 -0.407 1944 12 6.668 -1.590 0 0 6.668 -1.590 9.211 -0.328 1945 1 2.774 -3.992 0 0 2.774 -3.992 5.735 -2.311 1945 2 6.469 -1.017 1 0 NaN NaN 8.167 -0.599 1945 3 9.276 0.122 0 0 9.276 0.122 10.290 -0.144 1945 4 14.252 2.420 0 0 14.252 2.420 14.371 1.259 1945 5 21.365 5.006 1 0 NaN NaN 20.574 2.935 1945 6 NaN NaN NaN NaN NaN NaN 23.909 1.957 1945 7 NaN NaN NaN NaN NaN NaN 26.331 1.790 1945 8 NaN NaN NaN NaN NaN NaN 25.987 1.427 1945 9 NaN NaN NaN NaN NaN NaN 21.151 -0.100 1945 10 NaN NaN NaN NaN NaN NaN 15.109 -1.493 1945 11 NaN NaN NaN NaN NaN NaN 12.303 -0.481 1945 12 NaN NaN NaN NaN NaN NaN 9.225 -0.314 1946 1 NaN NaN NaN NaN NaN NaN 7.433 -0.612 1946 2 NaN NaN NaN NaN NaN NaN 8.836 0.070 1946 3 NaN NaN NaN NaN NaN NaN 10.538 0.104 1946 4 NaN NaN NaN NaN NaN NaN 13.932 0.821 1946 5 NaN NaN NaN NaN NaN NaN 18.701 1.063