% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 17653 % Primary Name: UJAE ATOLL/MARSHALL % Record Type: TAVG % Country: Marshall Islands % Latitude: 8.91700 +/- 0.00050 % Longitude: 165.75000 +/- 0.00050 % Elevation (m): 2.00 +/- 0.05 % # of Months: 14 % % IDs: gsod - 994490-99999 % icao - UJAP2 % usaf - 994490 % % Sources: Global Summary of the Day % % Site Hash: 3f2fdd08ddb8aaa29829551d7f3d8e26 % Raw Data Hash: c0514a311fce3099797d4a8517423fbc % Adj Data Hash: 0be2a65f750399dff1fd44ad5ba48652 % % 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 1989 3 NaN NaN NaN NaN NaN NaN 27.856 0.531 1989 4 NaN NaN NaN NaN NaN NaN 27.450 0.284 1989 5 NaN NaN NaN NaN NaN NaN 27.472 0.076 1989 6 NaN NaN NaN NaN NaN NaN 27.688 0.208 1989 7 NaN NaN NaN NaN NaN NaN 27.562 0.153 1989 8 NaN NaN NaN NaN NaN NaN 27.653 0.100 1989 9 NaN NaN NaN NaN NaN NaN 27.760 0.142 1989 10 NaN NaN NaN NaN NaN NaN 27.747 0.328 1989 11 NaN NaN NaN NaN NaN NaN 28.040 0.648 1989 12 NaN NaN NaN NaN NaN NaN 27.956 0.800 1990 1 NaN NaN NaN NaN NaN NaN 27.503 0.507 1990 2 NaN NaN NaN NaN NaN NaN 27.611 0.447 1990 3 27.615 0.461 1 0 NaN NaN 27.800 0.476 1990 4 27.844 0.849 0 0 27.844 0.849 27.903 0.738 1990 5 27.615 0.388 0 0 27.615 0.388 27.698 0.301 1990 6 27.719 0.409 0 0 27.719 0.409 27.900 0.420 1990 7 27.588 0.349 0 0 27.588 0.349 27.699 0.289 1990 8 27.968 0.585 0 0 27.968 0.585 28.159 0.605 1990 9 27.461 0.013 0 0 27.461 0.013 27.802 0.183 1990 10 27.989 0.741 0 0 27.989 0.741 28.014 0.595 1990 11 27.887 0.666 0 0 27.887 0.666 28.094 0.702 1990 12 27.710 0.724 0 0 27.710 0.724 27.823 0.667 1991 1 27.330 0.505 0 0 27.330 0.505 27.583 0.588 1991 2 27.157 0.164 1 0 NaN NaN 27.775 0.612 1991 3 27.095 -0.059 0 0 27.095 -0.059 27.548 0.223 1991 4 27.333 0.338 0 0 27.333 0.338 27.361 0.195 1991 5 NaN NaN NaN NaN NaN NaN 27.762 0.365 1991 6 NaN NaN NaN NaN NaN NaN 27.871 0.391 1991 7 NaN NaN NaN NaN NaN NaN 27.738 0.329 1991 8 NaN NaN NaN NaN NaN NaN 27.883 0.329 1991 9 NaN NaN NaN NaN NaN NaN 27.908 0.289 1991 10 NaN NaN NaN NaN NaN NaN 27.731 0.312 1991 11 NaN NaN NaN NaN NaN NaN 27.569 0.178 1991 12 NaN NaN NaN NaN NaN NaN 27.281 0.124 1992 1 NaN NaN NaN NaN NaN NaN 26.918 -0.077 1992 2 NaN NaN NaN NaN NaN NaN 27.226 0.062 1992 3 NaN NaN NaN NaN NaN NaN 27.516 0.192 1992 4 NaN NaN NaN NaN NaN NaN 27.499 0.333