% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 12777 % Primary Name: PORT-BOUET % Record Type: TAVG % Country: Cote D'Ivoire % Latitude: 5.25000 +/- 0.00500 % Longitude: -3.93000 +/- 0.00500 % Elevation (m): 10.00 +/- 0.50 % # of Months: 48 % % IDs: ghcnd - IV000009999 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: 81bdb01881affb0199c7e4eec695188c % Raw Data Hash: 806f1396d19081fb4e3f7b438f85ed9a % Adj Data Hash: ef90210e818e62e0c103c2d6fe7b1bbb % % 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 1946 1 NaN NaN NaN NaN NaN NaN 26.616 -0.200 1946 2 NaN NaN NaN NaN NaN NaN 28.124 0.214 1946 3 NaN NaN NaN NaN NaN NaN 28.281 0.237 1946 4 NaN NaN NaN NaN NaN NaN 27.799 0.282 1946 5 NaN NaN NaN NaN NaN NaN 27.092 0.274 1946 6 NaN NaN NaN NaN NaN NaN 25.065 -0.343 1946 7 NaN NaN NaN NaN NaN NaN 24.348 -0.234 1946 8 NaN NaN NaN NaN NaN NaN 23.560 -0.687 1946 9 NaN NaN NaN NaN NaN NaN 24.785 -0.159 1946 10 NaN NaN NaN NaN NaN NaN 25.475 -0.250 1946 11 NaN NaN NaN NaN NaN NaN 26.966 0.276 1946 12 NaN NaN NaN NaN NaN NaN 26.497 0.043 1947 1 26.198 -0.872 0 0 26.198 -0.872 26.428 -0.388 1947 2 26.589 -1.575 0 0 26.589 -1.575 28.060 0.150 1947 3 27.940 -0.358 0 0 27.940 -0.358 28.057 0.013 1947 4 27.403 -0.368 0 0 27.403 -0.368 27.423 -0.094 1947 5 27.540 0.468 0 0 27.540 0.468 27.188 0.370 1947 6 26.228 0.566 0 0 26.228 0.566 25.716 0.308 1947 7 25.687 0.850 0 0 25.687 0.850 24.840 0.257 1947 8 24.763 0.261 0 0 24.763 0.261 24.652 0.404 1947 9 25.015 -0.184 0 0 25.015 -0.184 25.024 0.079 1947 10 26.544 0.565 0 0 26.544 0.565 25.773 0.049 1947 11 26.538 -0.406 0 0 26.538 -0.406 26.506 -0.185 1947 12 26.782 0.074 0 0 26.782 0.074 26.409 -0.045 1948 1 25.919 -1.151 0 0 25.919 -1.151 26.066 -0.751 1948 2 26.671 -1.493 1 0 NaN NaN 27.657 -0.253 1948 3 28.015 -0.284 0 0 28.015 -0.284 28.192 0.148 1948 4 27.485 -0.286 0 0 27.485 -0.286 27.228 -0.289 1948 5 27.073 0.000 0 0 27.073 0.000 26.603 -0.216 1948 6 25.688 0.026 0 0 25.688 0.026 24.858 -0.550 1948 7 24.261 -0.576 0 0 24.261 -0.576 24.237 -0.346 1948 8 24.145 -0.356 0 0 24.145 -0.356 24.012 -0.236 1948 9 24.667 -0.532 0 0 24.667 -0.532 24.684 -0.261 1948 10 26.442 0.464 0 0 26.442 0.464 25.916 0.192 1948 11 26.847 -0.098 0 0 26.847 -0.098 26.723 0.033 1948 12 26.942 0.234 0 0 26.942 0.234 26.717 0.263 1949 1 26.082 -0.988 0 0 26.082 -0.988 26.904 0.087 1949 2 26.889 -1.275 0 0 26.889 -1.275 28.082 0.172 1949 3 27.815 -0.484 0 0 27.815 -0.484 28.192 0.148 1949 4 28.595 0.824 0 0 28.595 0.824 27.877 0.360 1949 5 27.800 0.728 0 0 27.800 0.728 27.349 0.530 1949 6 26.465 0.803 0 0 26.465 0.803 25.435 0.027 1949 7 25.595 0.758 0 0 25.595 0.758 24.766 0.184 1949 8 24.347 -0.155 0 0 24.347 -0.155 24.155 -0.092 1949 9 25.322 0.123 0 0 25.322 0.123 25.184 0.239 1949 10 26.218 0.239 0 0 26.218 0.239 25.847 0.123 1949 11 26.967 0.022 0 0 26.967 0.022 26.827 0.136 1949 12 27.606 0.898 0 0 27.606 0.898 27.060 0.606 1950 1 26.781 -0.290 0 0 26.781 -0.290 26.660 -0.157 1950 2 27.655 -0.509 0 0 27.655 -0.509 27.673 -0.236 1950 3 28.344 0.045 0 0 28.344 0.045 28.147 0.102 1950 4 28.503 0.732 0 0 28.503 0.732 27.714 0.197 1950 5 27.405 0.332 0 0 27.405 0.332 26.971 0.153 1950 6 26.268 0.606 0 0 26.268 0.606 25.267 -0.141 1950 7 26.260 1.423 0 0 26.260 1.423 24.845 0.262 1950 8 24.369 -0.132 0 0 24.369 -0.132 23.746 -0.501 1950 9 24.425 -0.774 0 0 24.425 -0.774 24.368 -0.577 1950 10 25.671 -0.307 0 0 25.671 -0.307 25.200 -0.524 1950 11 27.412 0.467 0 0 27.412 0.467 26.767 0.077 1950 12 27.365 0.656 0 0 27.365 0.656 26.583 0.129 1951 1 NaN NaN NaN NaN NaN NaN 26.840 0.023 1951 2 NaN NaN NaN NaN NaN NaN 27.266 -0.644 1951 3 NaN NaN NaN NaN NaN NaN 27.796 -0.248 1951 4 NaN NaN NaN NaN NaN NaN 27.826 0.309 1951 5 NaN NaN NaN NaN NaN NaN 26.839 0.021 1951 6 NaN NaN NaN NaN NaN NaN 25.518 0.110 1951 7 NaN NaN NaN NaN NaN NaN 24.816 0.233 1951 8 NaN NaN NaN NaN NaN NaN 24.116 -0.131 1951 9 NaN NaN NaN NaN NaN NaN 25.453 0.508 1951 10 NaN NaN NaN NaN NaN NaN 25.529 -0.195 1951 11 NaN NaN NaN NaN NaN NaN 26.934 0.243 1951 12 NaN NaN NaN NaN NaN NaN 27.135 0.681