% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 40438 % Primary Name: CRONK'S CANYON % Record Type: TAVG % Country: United States % State: ID % Latitude: 44.70000 +/- 0.00500 % Longitude: -114.05000 +/- 0.00500 % Elevation (m): 1402.08 +/- 0.15 % # of Months: 19 % % Alternate Names: Missing Station ID - 102273 % % IDs: coop - 102273 % ghcnd - USC00102273 % ncdc - 12001561 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: ef0000dad846cbf3fa994b7a94628aa9 % Raw Data Hash: e8afa8a89347915ffda1bd89c11b095c % Adj Data Hash: a76aab1cd7499de3bd3c09b41a89cfbc % % 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 1929 4 NaN NaN NaN NaN NaN NaN -0.123 -2.074 1929 5 NaN NaN NaN NaN NaN NaN 6.718 -0.575 1929 6 NaN NaN NaN NaN NaN NaN 10.242 -1.412 1929 7 NaN NaN NaN NaN NaN NaN 16.877 0.860 1929 8 NaN NaN NaN NaN NaN NaN 16.630 1.804 1929 9 NaN NaN NaN NaN NaN NaN 7.746 -2.388 1929 10 NaN NaN NaN NaN NaN NaN 5.366 1.216 1929 11 NaN NaN NaN NaN NaN NaN -4.525 -1.229 1929 12 NaN NaN NaN NaN NaN NaN -5.012 3.648 1930 1 NaN NaN NaN NaN NaN NaN -15.393 -5.287 1930 2 NaN NaN NaN NaN NaN NaN -2.824 4.050 1930 3 NaN NaN NaN NaN NaN NaN -2.916 0.736 1930 4 10.130 4.179 0 0 10.130 4.179 5.270 3.319 1930 5 12.965 1.671 0 0 12.965 1.671 7.082 -0.211 1930 6 16.577 0.922 0 0 16.577 0.922 10.664 -0.990 1930 7 21.568 1.550 0 0 21.568 1.550 17.331 1.314 1930 8 19.865 1.038 0 0 19.865 1.038 15.496 0.670 1930 9 14.540 0.406 0 0 14.540 0.406 9.842 -0.291 1930 10 7.124 -1.026 0 0 7.124 -1.026 3.452 -0.698 1930 11 -2.788 -3.493 0 0 -2.788 -3.493 -5.726 -2.431 1930 12 -11.205 -6.545 0 0 -11.205 -6.545 -12.621 -3.961 1931 1 -8.894 -2.787 0 0 -8.894 -2.787 -10.015 0.091 1931 2 NaN NaN NaN NaN NaN NaN -6.888 -0.014 1931 3 1.297 0.949 1 0 NaN NaN -4.201 -0.549 1931 4 7.220 1.269 0 0 7.220 1.269 2.187 0.236 1931 5 12.554 1.260 1 0 NaN NaN 8.325 1.033 1931 6 18.022 2.367 0 0 18.022 2.367 12.827 1.173 1931 7 21.198 1.181 0 0 21.198 1.181 17.834 1.817 1931 8 19.473 0.646 0 0 19.473 0.646 15.481 0.655 1931 9 14.002 -0.132 0 0 14.002 -0.132 9.612 -0.522 1931 10 8.021 -0.129 1 0 NaN NaN 4.958 0.808 1931 11 -3.308 -4.013 0 0 -3.308 -4.013 -6.232 -2.937 1931 12 NaN NaN NaN NaN NaN NaN -11.338 -2.678 1932 1 NaN NaN NaN NaN NaN NaN -13.471 -3.365 1932 2 NaN NaN NaN NaN NaN NaN -8.999 -2.125 1932 3 NaN NaN NaN NaN NaN NaN -5.527 -1.875 1932 4 NaN NaN NaN NaN NaN NaN 1.729 -0.222 1932 5 NaN NaN NaN NaN NaN NaN 7.218 -0.074 1932 6 NaN NaN NaN NaN NaN NaN 11.083 -0.572 1932 7 NaN NaN NaN NaN NaN NaN 15.472 -0.545 1932 8 NaN NaN NaN NaN NaN NaN 13.924 -0.902 1932 9 NaN NaN NaN NaN NaN NaN 10.172 0.038 1932 10 NaN NaN NaN NaN NaN NaN 3.590 -0.560 1932 11 NaN NaN NaN NaN NaN NaN -1.571 1.725