% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 40863 % Primary Name: HUBBARD % Record Type: TAVG % Country: United States % State: OR % Latitude: 45.20000 +/- 0.00005 % Longitude: -123.76670 +/- 0.00005 % Elevation (m): 81.99 +/- 0.15 % # of Months: 48 % % Alternate Names: Missing Station ID - 354072 % % IDs: coop - 354072 % ghcnd - USC00354072 % ncdc - 20016286 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: dd772c77040d57e54c3abb646e91bd18 % Raw Data Hash: dacc745cedbbc7dd590a6a02ae9c24ac % Adj Data Hash: 4bcfe477b3872860be6731badeefd538 % % 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 1892 1 NaN NaN NaN NaN NaN NaN 3.372 -0.123 1892 2 NaN NaN NaN NaN NaN NaN 5.810 0.247 1892 3 NaN NaN NaN NaN NaN NaN 7.513 1.154 1892 4 NaN NaN NaN NaN NaN NaN 6.871 -1.482 1892 5 NaN NaN NaN NaN NaN NaN 11.904 0.412 1892 6 NaN NaN NaN NaN NaN NaN 13.563 -0.581 1892 7 NaN NaN NaN NaN NaN NaN 15.117 -1.183 1892 8 NaN NaN NaN NaN NaN NaN 16.203 -0.063 1892 9 NaN NaN NaN NaN NaN NaN 14.606 -0.126 1892 10 NaN NaN NaN NaN NaN NaN 10.865 0.112 1892 11 NaN NaN NaN NaN NaN NaN 6.771 0.111 1892 12 NaN NaN NaN NaN NaN NaN 3.413 -0.986 1893 1 1.844 -2.510 0 0 1.844 -2.510 0.964 -2.531 1893 2 4.742 -1.679 0 0 4.742 -1.679 3.217 -2.346 1893 3 7.069 -0.149 0 0 7.069 -0.149 4.900 -1.460 1893 4 8.487 -0.725 0 0 8.487 -0.725 5.898 -2.455 1893 5 12.500 0.150 0 0 12.500 0.150 10.620 -0.871 1893 6 11.877 -3.125 0 0 11.877 -3.125 11.789 -2.355 1893 7 16.812 -0.348 0 0 16.812 -0.348 15.252 -1.049 1893 8 17.481 0.356 0 0 17.481 0.356 15.993 -0.274 1893 9 13.487 -2.104 0 0 13.487 -2.104 12.865 -1.868 1893 10 8.728 -2.883 0 0 8.728 -2.883 8.518 -2.234 1893 11 6.232 -1.288 0 0 6.232 -1.288 5.817 -0.843 1893 12 7.840 2.582 1 0 NaN NaN 5.822 1.423 1894 1 4.267 -0.087 0 0 4.267 -0.087 3.368 -0.127 1894 2 3.483 -2.939 0 0 3.483 -2.939 3.062 -2.501 1894 3 6.782 -0.437 0 0 6.782 -0.437 4.525 -1.834 1894 4 9.315 0.103 0 0 9.315 0.103 7.359 -0.994 1894 5 12.491 0.141 0 0 12.491 0.141 10.936 -0.556 1894 6 14.593 -0.410 0 0 14.593 -0.410 13.080 -1.064 1894 7 18.194 1.035 0 0 18.194 1.035 16.403 0.103 1894 8 19.061 1.936 0 0 19.061 1.936 17.780 1.514 1894 9 14.252 -1.339 0 0 14.252 -1.339 13.834 -0.898 1894 10 10.926 -0.685 0 0 10.926 -0.685 9.884 -0.868 1894 11 7.152 -0.367 0 0 7.152 -0.367 7.716 1.056 1894 12 3.068 -2.190 0 0 3.068 -2.190 3.097 -1.302 1895 1 2.586 -1.768 0 0 2.586 -1.768 2.395 -1.100 1895 2 5.370 -1.051 0 0 5.370 -1.051 6.093 0.531 1895 3 6.398 -0.821 0 0 6.398 -0.821 5.699 -0.661 1895 4 9.861 0.649 0 0 9.861 0.649 8.305 -0.048 1895 5 12.455 0.105 0 0 12.455 0.105 11.194 -0.297 1895 6 15.481 0.479 0 0 15.481 0.479 14.150 0.006 1895 7 17.869 0.710 0 0 17.869 0.710 16.089 -0.211 1895 8 17.435 0.310 0 0 17.435 0.310 15.741 -0.525 1895 9 12.548 -3.043 0 0 12.548 -3.043 12.472 -2.261 1895 10 11.131 -0.480 0 0 11.131 -0.480 11.308 0.555 1895 11 4.444 -3.075 0 0 4.444 -3.075 5.456 -1.204 1895 12 4.061 -1.197 0 0 4.061 -1.197 4.314 -0.085 1896 1 4.866 0.512 0 0 4.866 0.512 4.109 0.614 1896 2 6.755 0.334 0 0 6.755 0.334 6.915 1.352 1896 3 6.252 -0.967 0 0 6.252 -0.967 5.269 -1.090 1896 4 7.858 -1.354 0 0 7.858 -1.354 6.268 -2.085 1896 5 10.556 -1.795 0 0 10.556 -1.795 9.715 -1.777 1896 6 14.881 -0.122 0 0 14.881 -0.122 13.850 -0.293 1896 7 19.206 2.047 0 0 19.206 2.047 18.247 1.947 1896 8 17.887 0.762 0 0 17.887 0.762 16.696 0.430 1896 9 14.486 -1.105 0 0 14.486 -1.105 14.169 -0.563 1896 10 10.942 -0.669 0 0 10.942 -0.669 11.012 0.259 1896 11 2.619 -4.900 0 0 2.619 -4.900 2.941 -3.720 1896 12 NaN NaN NaN NaN NaN NaN 6.168 1.769 1897 1 3.392 -0.962 1 0 NaN NaN 3.370 -0.125 1897 2 NaN NaN NaN NaN NaN NaN 5.404 -0.158 1897 3 NaN NaN NaN NaN NaN NaN 3.361 -2.998 1897 4 NaN NaN NaN NaN NaN NaN 9.851 1.498 1897 5 NaN NaN NaN NaN NaN NaN 13.781 2.289 1897 6 NaN NaN NaN NaN NaN NaN 14.317 0.173 1897 7 NaN NaN NaN NaN NaN NaN 15.213 -1.087 1897 8 NaN NaN NaN NaN NaN NaN 17.648 1.381 1897 9 NaN NaN NaN NaN NaN NaN 13.701 -1.031 1897 10 NaN NaN NaN NaN NaN NaN 10.722 -0.030 1897 11 NaN NaN NaN NaN NaN NaN 5.767 -0.893 1897 12 NaN NaN NaN NaN NaN NaN 5.255 0.856 1898 1 NaN NaN NaN NaN NaN NaN 2.581 -0.914