% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 43070 % Primary Name: DAVIS RIVER POWER PLANT % Record Type: TAVG % Country: United States % State: AK % Latitude: 55.76670 +/- 0.00005 % Longitude: -130.18330 +/- 0.00005 % Elevation (m): 346.36 +/- 1018.98 % # of Months: 47 % % Alternate Names: DAVIS RVR PWR PLT % Missing Station ID - 502307 % % IDs: coop - 502307 % ghcnd - USC00502307 % ncdc - 30015255 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: 2fcf9904742fe66b9a2d9a366da1e033 % Raw Data Hash: 155adc1b7a8390e3b366986f165599f1 % Adj Data Hash: 5a8efe8a65439dfcbe7c7c925de17586 % % 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 1931 9 NaN NaN NaN NaN NaN NaN 8.879 -0.156 1931 10 NaN NaN NaN NaN NaN NaN 4.297 0.129 1931 11 NaN NaN NaN NaN NaN NaN -2.469 -1.781 1931 12 NaN NaN NaN NaN NaN NaN -2.709 1.148 1932 1 NaN NaN NaN NaN NaN NaN -5.940 -0.072 1932 2 NaN NaN NaN NaN NaN NaN -3.216 -0.549 1932 3 NaN NaN NaN NaN NaN NaN -0.761 0.015 1932 4 NaN NaN NaN NaN NaN NaN 3.912 1.166 1932 5 NaN NaN NaN NaN NaN NaN 6.694 -0.368 1932 6 NaN NaN NaN NaN NaN NaN 9.058 -1.429 1932 7 NaN NaN NaN NaN NaN NaN 10.438 -2.150 1932 8 NaN NaN NaN NaN NaN NaN 12.518 0.263 1932 9 8.863 -1.000 0 0 8.863 -1.000 7.862 -1.173 1932 10 5.477 0.480 0 0 5.477 0.480 4.939 0.771 1932 11 1.030 0.889 0 0 1.030 0.889 -0.623 0.065 1932 12 NaN NaN NaN NaN NaN NaN -5.172 -1.315 1933 1 -3.532 1.507 0 0 -3.532 1.507 -5.788 0.081 1933 2 -2.366 -0.528 0 0 -2.366 -0.528 -2.772 -0.105 1933 3 0.171 0.119 0 0 0.171 0.119 -1.191 -0.414 1933 4 3.760 0.185 0 0 3.760 0.185 2.214 -0.532 1933 5 7.463 -0.428 0 0 7.463 -0.428 6.819 -0.243 1933 6 9.233 -2.082 0 0 9.233 -2.082 8.321 -2.165 1933 7 10.994 -2.423 0 0 10.994 -2.423 10.051 -2.537 1933 8 12.797 -0.287 0 0 12.797 -0.287 13.123 0.868 1933 9 8.600 -1.264 0 0 8.600 -1.264 8.239 -0.796 1933 10 3.132 -1.865 0 0 3.132 -1.865 2.376 -1.792 1933 11 2.019 1.879 1 0 NaN NaN 2.061 2.749 1933 12 -8.995 -5.967 0 0 -8.995 -5.967 -10.104 -6.247 1934 1 -1.565 3.475 0 0 -1.565 3.475 -3.863 2.006 1934 2 0.723 2.561 0 0 0.723 2.561 0.760 3.427 1934 3 0.989 0.936 0 0 0.989 0.936 0.436 1.213 1934 4 4.455 0.880 0 0 4.455 0.880 3.966 1.220 1934 5 7.860 -0.031 0 0 7.860 -0.031 7.827 0.766 1934 6 10.775 -0.541 0 0 10.775 -0.541 10.052 -0.435 1934 7 12.756 -0.660 0 0 12.756 -0.660 12.256 -0.332 1934 8 12.890 -0.194 0 0 12.890 -0.194 13.000 0.745 1934 9 9.525 -0.339 0 0 9.525 -0.339 8.939 -0.096 1934 10 5.392 0.395 0 0 5.392 0.395 4.609 0.441 1934 11 2.277 2.136 0 0 2.277 2.136 1.342 2.030 1934 12 -2.629 0.399 1 0 NaN NaN -3.997 -0.140 1935 1 -5.710 -0.670 0 0 -5.710 -0.670 -8.132 -2.264 1935 2 0.120 1.958 0 0 0.120 1.958 0.758 3.425 1935 3 -1.352 -1.404 0 0 -1.352 -1.404 -2.728 -1.952 1935 4 2.720 -0.855 0 0 2.720 -0.855 1.794 -0.952 1935 5 7.158 -0.733 0 0 7.158 -0.733 6.221 -0.840 1935 6 10.667 -0.649 0 0 10.667 -0.649 9.395 -1.091 1935 7 13.898 0.482 0 0 13.898 0.482 12.798 0.210 1935 8 11.616 -1.468 0 0 11.616 -1.468 11.393 -0.862 1935 9 10.050 0.186 0 0 10.050 0.186 9.737 0.702 1935 10 3.663 -1.334 0 0 3.663 -1.334 3.226 -0.942 1935 11 -0.365 -0.506 0 0 -0.365 -0.506 -0.973 -0.285 1935 12 1.048 4.077 0 0 1.048 4.077 0.465 4.322 1936 1 -4.495 0.544 0 0 -4.495 0.544 -5.666 0.202 1936 2 NaN NaN NaN NaN NaN NaN -10.238 -7.572 1936 3 0.295 0.243 0 0 0.295 0.243 -1.710 -0.933 1936 4 4.073 0.499 0 0 4.073 0.499 2.866 0.120 1936 5 8.166 0.275 0 0 8.166 0.275 7.649 0.587 1936 6 13.767 2.451 0 0 13.767 2.451 12.607 2.120 1936 7 13.226 -0.191 0 0 13.226 -0.191 12.424 -0.164 1936 8 13.816 0.732 0 0 13.816 0.732 13.515 1.260 1936 9 9.678 -0.185 0 0 9.678 -0.185 9.017 -0.018 1936 10 NaN NaN NaN NaN NaN NaN 6.623 2.454 1936 11 NaN NaN NaN NaN NaN NaN 2.037 2.725 1936 12 NaN NaN NaN NaN NaN NaN -3.978 -0.121 1937 1 NaN NaN NaN NaN NaN NaN -8.779 -2.910 1937 2 NaN NaN NaN NaN NaN NaN -4.732 -2.065 1937 3 NaN NaN NaN NaN NaN NaN 1.575 2.351 1937 4 NaN NaN NaN NaN NaN NaN 2.824 0.078 1937 5 NaN NaN NaN NaN NaN NaN 6.784 -0.278 1937 6 NaN NaN NaN NaN NaN NaN 11.489 1.002 1937 7 NaN NaN NaN NaN NaN NaN 11.715 -0.873 1937 8 NaN NaN NaN NaN NaN NaN 11.006 -1.249 1937 9 NaN NaN NaN NaN NaN NaN 9.954 0.920