% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 40424 % Primary Name: KIMBALL RANCH % Record Type: TAVG % Country: United States % State: WY % Latitude: 44.68330 +/- 0.00005 % Longitude: -109.20000 +/- 0.00005 % Elevation (m): 1450.85 +/- 0.15 % # of Months: 36 % % Alternate Names: Missing Station ID - 485165 % % IDs: coop - 485165 % ghcnd - USC00485165 % ncdc - 12006260 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: 2ff3951ee33bffe8b430b1a8a4db4054 % Raw Data Hash: 5a7c1b2a4d049859fe98d98f117c1732 % Adj Data Hash: 2c557a248e0b5ae4f650166c20154f9a % % 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 1898 11 NaN NaN NaN NaN NaN NaN -5.544 -2.274 1898 12 NaN NaN NaN NaN NaN NaN -9.569 -2.469 1899 1 NaN NaN NaN NaN NaN NaN -7.518 1.248 1899 2 NaN NaN NaN NaN NaN NaN -12.803 -6.712 1899 3 NaN NaN NaN NaN NaN NaN -8.042 -4.025 1899 4 NaN NaN NaN NaN NaN NaN 0.467 -0.521 1899 5 NaN NaN NaN NaN NaN NaN 4.588 -1.999 1899 6 NaN NaN NaN NaN NaN NaN 9.594 -1.511 1899 7 NaN NaN NaN NaN NaN NaN 14.937 -0.154 1899 8 NaN NaN NaN NaN NaN NaN 12.440 -1.640 1899 9 NaN NaN NaN NaN NaN NaN 9.871 0.687 1899 10 NaN NaN NaN NaN NaN NaN 2.035 -1.826 1899 11 5.921 4.073 1 0 NaN NaN -0.096 3.173 1899 12 -1.376 0.606 0 0 -1.376 0.606 -7.414 -0.314 1900 1 -0.021 3.627 0 0 -0.021 3.627 -5.574 3.192 1900 2 -5.268 -4.296 0 0 -5.268 -4.296 -8.409 -2.319 1900 3 2.034 0.933 1 0 NaN NaN -2.258 1.759 1900 4 8.919 2.812 0 0 8.919 2.812 2.650 1.662 1900 5 14.739 3.034 1 0 NaN NaN 8.663 2.076 1900 6 NaN NaN NaN NaN NaN NaN 13.906 2.800 1900 7 NaN NaN NaN NaN NaN NaN 14.496 -0.596 1900 8 NaN NaN NaN NaN NaN NaN 13.811 -0.269 1900 9 12.302 -2.000 0 0 12.302 -2.000 7.771 -1.412 1900 10 9.515 0.536 0 0 9.515 0.536 5.043 1.182 1900 11 1.312 -0.537 0 0 1.312 -0.537 -3.231 0.038 1900 12 1.043 3.025 1 0 NaN NaN -4.089 3.010 1901 1 0.690 4.338 0 0 0.690 4.338 -6.398 2.368 1901 2 -0.571 0.401 1 0 NaN NaN -8.200 -2.109 1901 3 -0.357 -1.458 1 0 NaN NaN -4.268 -0.251 1901 4 NaN NaN NaN NaN NaN NaN 0.885 -0.103 1901 5 10.056 -1.649 1 0 NaN NaN 9.818 3.231 1901 6 13.935 -2.288 0 0 13.935 -2.288 8.829 -2.276 1901 7 15.560 -4.649 1 0 NaN NaN 17.623 2.531 1901 8 NaN NaN NaN NaN NaN NaN 15.339 1.259 1901 9 NaN NaN NaN NaN NaN NaN 6.796 -2.387 1901 10 NaN NaN NaN NaN NaN NaN 6.526 2.664 1901 11 5.411 3.562 1 0 NaN NaN -0.624 2.646 1901 12 -0.402 1.579 1 0 NaN NaN -6.679 0.421 1902 1 -5.577 -1.929 0 0 -5.577 -1.929 -9.386 -0.620 1902 2 1.733 2.706 0 0 1.733 2.706 -3.808 2.282 1902 3 1.419 0.318 0 0 1.419 0.318 -5.524 -1.507 1902 4 NaN NaN NaN NaN NaN NaN 0.368 -0.620 1902 5 NaN NaN NaN NaN NaN NaN 7.759 1.172 1902 6 NaN NaN NaN NaN NaN NaN 10.247 -0.858 1902 7 NaN NaN NaN NaN NaN NaN 13.319 -1.772 1902 8 18.021 -1.177 1 0 NaN NaN 13.663 -0.417 1902 9 12.348 -1.954 0 0 12.348 -1.954 7.529 -1.655 1902 10 10.085 1.106 1 0 NaN NaN 5.003 1.141 1902 11 1.546 -0.302 1 0 NaN NaN -3.673 -0.404 1902 12 -1.495 0.486 1 0 NaN NaN -7.521 -0.422 1903 1 1.060 4.707 1 0 NaN NaN -6.445 2.321 1903 2 -6.309 -5.337 0 0 -6.309 -5.337 -10.751 -4.660 1903 3 -1.385 -2.486 0 0 -1.385 -2.486 -5.866 -1.849 1903 4 5.239 -0.867 1 0 NaN NaN 0.011 -0.977 1903 5 9.102 -2.603 1 0 NaN NaN 5.076 -1.511 1903 6 NaN NaN NaN NaN NaN NaN 11.325 0.220 1903 7 NaN NaN NaN NaN NaN NaN 13.393 -1.698 1903 8 NaN NaN NaN NaN NaN NaN 14.065 -0.015 1903 9 NaN NaN NaN NaN NaN NaN 6.547 -2.637 1903 10 NaN NaN NaN NaN NaN NaN 5.378 1.516 1903 11 NaN NaN NaN NaN NaN NaN -3.739 -0.469 1903 12 NaN NaN NaN NaN NaN NaN -5.612 1.488 1904 1 NaN NaN NaN NaN NaN NaN -8.708 0.058 1904 2 NaN NaN NaN NaN NaN NaN -5.056 1.034 1904 3 -1.700 -2.801 0 0 -1.700 -2.801 -5.264 -1.247 1904 4 7.981 1.874 0 0 7.981 1.874 2.012 1.024 1904 5 10.987 -0.719 0 0 10.987 -0.719 6.301 -0.287 1904 6 15.752 -0.471 0 0 15.752 -0.471 9.503 -1.602 1904 7 NaN NaN NaN NaN NaN NaN 13.663 -1.428 1904 8 NaN NaN NaN NaN NaN NaN 13.967 -0.113 1904 9 NaN NaN NaN NaN NaN NaN 9.208 0.024 1904 10 NaN NaN NaN NaN NaN NaN 5.497 1.636 1904 11 NaN NaN NaN NaN NaN NaN -0.004 3.266 1904 12 NaN NaN NaN NaN NaN NaN -5.732 1.367 1905 1 NaN NaN NaN NaN NaN NaN -7.678 1.087 1905 2 NaN NaN NaN NaN NaN NaN -8.999 -2.909 1905 3 NaN NaN NaN NaN NaN NaN -1.644 2.373 1905 4 NaN NaN NaN NaN NaN NaN 1.174 0.186 1905 5 NaN NaN NaN NaN NaN NaN 4.572 -2.015 1905 6 NaN NaN NaN NaN NaN NaN 9.289 -1.817