% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 19939 % Primary Name: AGUADILLA CITY % Record Type: TAVG % Country: Puerto Rico [United States] % State: PR % Latitude: 18.43330 +/- 0.00005 % Longitude: -67.15000 +/- 0.00005 % Elevation (m): 0.00 +/- 0.15 % # of Months: 38 % % Alternate Names: Missing Station ID - 660105 % % IDs: coop - 660105 % ghcnd - RQC00660105 % ncdc - 20023993 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: dd75de74d821e65f499880cbd41558e4 % Raw Data Hash: 1dab5666699fdbfe9b360bb9086beec9 % Adj Data Hash: 2d124928ad65e6aa65c3583be3f4bd6e % % 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 1898 5 NaN NaN NaN NaN NaN NaN 25.978 -0.056 1898 6 NaN NaN NaN NaN NaN NaN 26.763 -0.195 1898 7 NaN NaN NaN NaN NaN NaN 26.731 -0.593 1898 8 NaN NaN NaN NaN NaN NaN 27.032 -0.444 1898 9 NaN NaN NaN NaN NaN NaN 26.934 -0.458 1898 10 NaN NaN NaN NaN NaN NaN 26.779 -0.188 1898 11 NaN NaN NaN NaN NaN NaN 25.584 -0.768 1898 12 NaN NaN NaN NaN NaN NaN 24.841 -0.271 1899 1 NaN NaN NaN NaN NaN NaN 23.460 -0.775 1899 2 NaN NaN NaN NaN NaN NaN 23.661 -0.274 1899 3 NaN NaN NaN NaN NaN NaN 23.554 -0.621 1899 4 NaN NaN NaN NaN NaN NaN 24.142 -0.610 1899 5 26.644 -0.013 0 0 26.644 -0.013 25.646 -0.388 1899 6 27.120 -0.463 0 0 27.120 -0.463 26.344 -0.615 1899 7 27.773 -0.176 0 0 27.773 -0.176 26.809 -0.515 1899 8 27.081 -1.019 1 0 NaN NaN 26.777 -0.699 1899 9 NaN NaN NaN NaN NaN NaN 27.138 -0.254 1899 10 NaN NaN NaN NaN NaN NaN 26.088 -0.879 1899 11 25.298 -1.679 0 0 25.298 -1.679 25.941 -0.412 1899 12 24.330 -1.406 0 0 24.330 -1.406 24.501 -0.610 1900 1 25.773 0.914 0 0 25.773 0.914 24.324 0.089 1900 2 25.870 1.310 0 0 25.870 1.310 24.010 0.075 1900 3 25.755 0.956 0 0 25.755 0.956 23.973 -0.202 1900 4 26.545 1.169 0 0 26.545 1.169 24.652 -0.100 1900 5 27.065 0.407 0 0 27.065 0.407 26.150 0.116 1900 6 27.055 -0.528 0 0 27.055 -0.528 26.468 -0.491 1900 7 27.503 -0.445 0 0 27.503 -0.445 26.941 -0.383 1900 8 27.647 -0.454 0 0 27.647 -0.454 27.132 -0.344 1900 9 27.988 -0.028 0 0 27.988 -0.028 27.176 -0.217 1900 10 27.744 0.153 0 0 27.744 0.153 26.731 -0.236 1900 11 26.777 -0.200 0 0 26.777 -0.200 26.313 -0.039 1900 12 23.542 -2.194 0 0 23.542 -2.194 24.912 -0.200 1901 1 22.600 -2.260 0 0 22.600 -2.260 23.770 -0.465 1901 2 NaN NaN NaN NaN NaN NaN 24.098 0.162 1901 3 25.313 0.514 0 0 25.313 0.514 24.133 -0.042 1901 4 26.220 0.844 0 0 26.220 0.844 24.951 0.199 1901 5 27.244 0.586 0 0 27.244 0.586 26.158 0.125 1901 6 NaN NaN NaN NaN NaN NaN 26.898 -0.061 1901 7 NaN NaN NaN NaN NaN NaN 26.798 -0.526 1901 8 NaN NaN NaN NaN NaN NaN 27.410 -0.066 1901 9 NaN NaN NaN NaN NaN NaN 27.378 -0.014 1901 10 NaN NaN NaN NaN NaN NaN 26.773 -0.194 1901 11 25.635 -1.342 0 0 25.635 -1.342 25.903 -0.449 1901 12 24.371 -1.365 1 0 NaN NaN 24.835 -0.277 1902 1 23.647 -1.213 0 0 23.647 -1.213 23.788 -0.447 1902 2 24.245 -0.315 0 0 24.245 -0.315 23.958 0.023 1902 3 24.500 -0.299 0 0 24.500 -0.299 23.731 -0.444 1902 4 25.907 0.530 0 0 25.907 0.530 24.597 -0.154 1902 5 27.168 0.510 0 0 27.168 0.510 25.801 -0.233 1902 6 28.138 0.555 0 0 28.138 0.555 26.672 -0.287 1902 7 NaN NaN NaN NaN NaN NaN 27.070 -0.254 1902 8 NaN NaN NaN NaN NaN NaN 27.306 -0.170 1902 9 26.782 -1.235 0 0 26.782 -1.235 26.833 -0.560 1902 10 25.642 -1.949 0 0 25.642 -1.949 26.001 -0.966 1902 11 25.357 -1.620 0 0 25.357 -1.620 25.614 -0.739 1902 12 24.676 -1.060 0 0 24.676 -1.060 24.641 -0.471 1903 1 24.358 -0.501 0 0 24.358 -0.501 23.957 -0.278 1903 2 24.486 -0.074 0 0 24.486 -0.074 23.627 -0.308 1903 3 24.775 -0.024 1 0 NaN NaN 23.577 -0.597 1903 4 26.217 0.840 0 0 26.217 0.840 24.547 -0.205 1903 5 NaN NaN NaN NaN NaN NaN 25.979 -0.054 1903 6 NaN NaN NaN NaN NaN NaN 26.923 -0.036 1903 7 NaN NaN NaN NaN NaN NaN 26.955 -0.369 1903 8 NaN NaN NaN NaN NaN NaN 27.009 -0.467 1903 9 NaN NaN NaN NaN NaN NaN 26.691 -0.701 1903 10 NaN NaN NaN NaN NaN NaN 26.370 -0.597 1903 11 NaN NaN NaN NaN NaN NaN 25.754 -0.599 1903 12 NaN NaN NaN NaN NaN NaN 24.599 -0.513 1904 1 NaN NaN NaN NaN NaN NaN 23.567 -0.668 1904 2 NaN NaN NaN NaN NaN NaN 23.147 -0.788 1904 3 NaN NaN NaN NaN NaN NaN 22.804 -1.371 1904 4 NaN NaN NaN NaN NaN NaN 23.362 -1.389