% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 43072 % Primary Name: HERENDEEN BAY % Record Type: TAVG % Country: United States % State: AK % Latitude: 55.85000 +/- 0.00500 % Longitude: -160.25000 +/- 0.00500 % Elevation (m): 4.57 +/- 0.15 % # of Months: 9 % % Alternate Names: Missing Station ID - 503591 % % IDs: coop - 503591 % ghcnd - USC00503591 % ncdc - 30015263 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: ad514edda59194b3aa3495d57027d71e % Raw Data Hash: 5c9d66d8f9d956193d4ce5ac592a0a55 % Adj Data Hash: 538c39f50bf81d71d8c41d1bd4bb5937 % % 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 1918 1 NaN NaN NaN NaN NaN NaN -4.347 -1.072 1918 2 NaN NaN NaN NaN NaN NaN -4.038 -0.818 1918 3 NaN NaN NaN NaN NaN NaN -3.210 -0.973 1918 4 NaN NaN NaN NaN NaN NaN -0.401 -0.771 1918 5 NaN NaN NaN NaN NaN NaN 5.127 0.460 1918 6 NaN NaN NaN NaN NaN NaN 8.913 0.623 1918 7 NaN NaN NaN NaN NaN NaN 12.022 1.219 1918 8 NaN NaN NaN NaN NaN NaN 10.705 -0.279 1918 9 NaN NaN NaN NaN NaN NaN 8.200 -0.362 1918 10 NaN NaN NaN NaN NaN NaN 3.246 -0.173 1918 11 NaN NaN NaN NaN NaN NaN -2.623 -2.723 1918 12 NaN NaN NaN NaN NaN NaN -4.473 -1.221 1919 1 -8.550 -6.927 0 0 -8.550 -6.927 -8.788 -5.513 1919 2 NaN NaN NaN NaN NaN NaN -2.922 0.298 1919 3 1.320 1.904 0 0 1.320 1.904 -0.806 1.430 1919 4 0.410 -1.612 1 0 NaN NaN -0.606 -0.976 1919 5 4.141 -2.178 1 0 NaN NaN 3.956 -0.711 1919 6 NaN NaN NaN NaN NaN NaN 8.264 -0.026 1919 7 NaN NaN NaN NaN NaN NaN 10.784 -0.019 1919 8 11.350 -1.286 0 0 11.350 -1.286 11.056 0.071 1919 9 9.992 -0.223 1 0 NaN NaN 9.057 0.494 1919 10 5.873 0.802 0 0 5.873 0.802 4.351 0.932 1919 11 NaN NaN NaN NaN NaN NaN 0.290 0.190 1919 12 0.377 1.976 0 0 0.377 1.976 -2.914 0.338 1920 1 NaN NaN NaN NaN NaN NaN -5.538 -2.264 1920 2 NaN NaN NaN NaN NaN NaN -1.218 2.003 1920 3 1.729 2.314 0 0 1.729 2.314 -0.710 1.526 1920 4 NaN NaN NaN NaN NaN NaN -1.744 -2.114 1920 5 NaN NaN NaN NaN NaN NaN 4.262 -0.405 1920 6 NaN NaN NaN NaN NaN NaN 8.388 0.098 1920 7 NaN NaN NaN NaN NaN NaN 10.437 -0.366 1920 8 NaN NaN NaN NaN NaN NaN 9.196 -1.789 1920 9 NaN NaN NaN NaN NaN NaN 7.264 -1.299 1920 10 NaN NaN NaN NaN NaN NaN 2.903 -0.516 1920 11 NaN NaN NaN NaN NaN NaN 0.372 0.272 1920 12 NaN NaN NaN NaN NaN NaN -6.040 -2.788 1921 1 NaN NaN NaN NaN NaN NaN -6.185 -2.911 1921 2 NaN NaN NaN NaN NaN NaN -6.240 -3.020 1921 3 NaN NaN NaN NaN NaN NaN -0.035 2.202