% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 13468 % Primary Name: FSM CAPITOL % Record Type: TAVG % Country: Federated States of Micronesia % State: PI % Latitude: 6.91667 +/- 0.00833 % Longitude: 158.16667 +/- 0.00833 % Elevation (m): 85.30 +/- 0.05 % # of Months: 12 % % IDs: coop - 914254 % % Sources: US Cooperative Summary of the Day % US Cooperative Summary of the Month % % Site Hash: 984104daa680382e22331aa74e1b40d2 % Raw Data Hash: 66d56aed02f3983704a6289bf6faaa97 % Adj Data Hash: 1e2c95073b3fba9eec9ab6e9d5d16abb % % 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 4 NaN NaN NaN NaN NaN NaN 26.887 0.048 1989 5 NaN NaN NaN NaN NaN NaN 27.117 0.019 1989 6 NaN NaN NaN NaN NaN NaN 26.869 -0.129 1989 7 NaN NaN NaN NaN NaN NaN 27.024 0.215 1989 8 NaN NaN NaN NaN NaN NaN 26.870 0.013 1989 9 NaN NaN NaN NaN NaN NaN 27.043 0.135 1989 10 NaN NaN NaN NaN NaN NaN 26.966 0.227 1989 11 NaN NaN NaN NaN NaN NaN 27.463 0.539 1989 12 NaN NaN NaN NaN NaN NaN 27.068 0.184 1990 1 NaN NaN NaN NaN NaN NaN 27.440 0.559 1990 2 NaN NaN NaN NaN NaN NaN 27.260 0.302 1990 3 NaN NaN NaN NaN NaN NaN 27.444 0.432 1990 4 27.000 0.876 0 0 27.000 0.876 27.452 0.613 1990 5 27.000 0.617 0 0 27.000 0.617 27.505 0.407 1990 6 26.448 0.166 0 0 26.448 0.166 27.266 0.268 1990 7 NaN NaN NaN NaN NaN NaN 26.768 -0.041 1990 8 25.889 -0.253 0 0 25.889 -0.253 26.896 0.039 1990 9 NaN NaN NaN NaN NaN NaN 26.957 0.049 1990 10 26.389 0.366 0 0 26.389 0.366 27.176 0.437 1990 11 NaN NaN NaN NaN NaN NaN 27.733 0.809 1990 12 26.587 0.418 1 0 NaN NaN 27.419 0.535 1991 1 NaN NaN NaN NaN NaN NaN 27.243 0.363 1991 2 27.024 0.782 1 0 NaN NaN 27.167 0.209 1991 3 NaN NaN NaN NaN NaN NaN 26.943 -0.068 1991 4 27.056 0.932 0 0 27.056 0.932 27.308 0.469 1991 5 26.197 -0.185 0 0 26.197 -0.185 27.405 0.306 1991 6 26.500 0.218 0 0 26.500 0.218 27.001 0.004 1991 7 26.444 0.351 0 0 26.444 0.351 27.075 0.266 1991 8 26.222 0.081 0 0 26.222 0.081 27.216 0.359 1991 9 NaN NaN NaN NaN NaN NaN 27.043 0.134 1991 10 NaN NaN NaN NaN NaN NaN 26.896 0.158 1991 11 NaN NaN NaN NaN NaN NaN 27.038 0.114 1991 12 NaN NaN NaN NaN NaN NaN 27.094 0.210 1992 1 NaN NaN NaN NaN NaN NaN 26.992 0.111 1992 2 NaN NaN NaN NaN NaN NaN 27.015 0.058 1992 3 NaN NaN NaN NaN NaN NaN 27.347 0.335 1992 4 NaN NaN NaN NaN NaN NaN 27.247 0.409 1992 5 NaN NaN NaN NaN NaN NaN 27.661 0.563 1992 6 NaN NaN NaN NaN NaN NaN 27.318 0.321 1992 7 NaN NaN NaN NaN NaN NaN 27.007 0.198 1992 8 NaN NaN NaN NaN NaN NaN 27.271 0.414