% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 34110 % Primary Name: HARLEY DOME % Record Type: TAVG % Country: United States % State: UT % Latitude: 39.16670 +/- 0.00005 % Longitude: -109.13330 +/- 0.00005 % Elevation (m): 1601.10 +/- 0.05 % # of Months: 47 % % IDs: coop - 423706 % ghcnd - USC00423706 % ncdc - 20026225 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % US Cooperative Summary of the Month % Multi-network Metadata System % % Site Hash: fe3c5635c111a13c48461ae20648382f % Raw Data Hash: 154dac691a635bacd0d41bb21530b850 % Adj Data Hash: 940fef0f531663b998cb7c73f70fbbf1 % % 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 1958 8 NaN NaN NaN NaN NaN NaN 20.839 1.360 1958 9 NaN NaN NaN NaN NaN NaN 15.128 0.364 1958 10 NaN NaN NaN NaN NaN NaN 9.381 1.109 1958 11 NaN NaN NaN NaN NaN NaN 1.260 0.738 1958 12 NaN NaN NaN NaN NaN NaN -1.343 3.903 1959 1 NaN NaN NaN NaN NaN NaN -4.566 1.811 1959 2 NaN NaN NaN NaN NaN NaN -1.577 1.179 1959 3 NaN NaN NaN NaN NaN NaN 0.907 -0.520 1959 4 NaN NaN NaN NaN NaN NaN 6.732 0.267 1959 5 NaN NaN NaN NaN NaN NaN 12.451 0.354 1959 6 NaN NaN NaN NaN NaN NaN 18.973 1.590 1959 7 NaN NaN NaN NaN NaN NaN 21.365 0.294 1959 8 23.443 0.845 1 0 NaN NaN 19.389 -0.090 1959 9 18.056 0.173 0 0 18.056 0.173 13.905 -0.860 1959 10 11.278 -0.113 0 0 11.278 -0.113 7.903 -0.370 1959 11 3.333 -0.307 0 0 3.333 -0.307 0.547 0.025 1959 12 -0.778 1.349 0 0 -0.778 1.349 -3.185 2.061 1960 1 -4.500 -1.241 0 0 -4.500 -1.241 -6.368 0.010 1960 2 -1.944 -2.307 0 0 -1.944 -2.307 -5.314 -2.559 1960 3 5.500 0.954 0 0 5.500 0.954 1.825 0.398 1960 4 10.722 1.139 0 0 10.722 1.139 7.285 0.820 1960 5 15.556 0.340 0 0 15.556 0.340 11.851 -0.246 1960 6 22.611 2.110 0 0 22.611 2.110 18.080 0.698 1960 7 26.000 1.811 0 0 26.000 1.811 21.750 0.679 1960 8 24.278 1.680 0 0 24.278 1.680 19.838 0.359 1960 9 20.222 2.339 0 0 20.222 2.339 16.406 1.641 1960 10 11.611 0.221 0 0 11.611 0.221 8.714 0.442 1960 11 4.944 1.304 0 0 4.944 1.304 1.690 1.167 1960 12 -1.389 0.738 0 0 -1.389 0.738 -4.795 0.451 1961 1 -2.111 1.148 0 0 -2.111 1.148 -5.383 0.995 1961 2 2.278 1.915 0 0 2.278 1.915 -0.610 2.145 1961 3 5.278 0.732 0 0 5.278 0.732 1.562 0.134 1961 4 9.778 0.195 0 0 9.778 0.195 5.840 -0.624 1961 5 16.222 1.007 0 0 16.222 1.007 12.836 0.739 1961 6 24.000 3.499 0 0 24.000 3.499 19.027 1.644 1961 7 26.000 1.811 0 0 26.000 1.811 21.422 0.352 1961 8 24.667 2.069 0 0 24.667 2.069 20.464 0.985 1961 9 14.667 -3.216 0 0 14.667 -3.216 11.629 -3.136 1961 10 10.056 -1.335 0 0 10.056 -1.335 8.133 -0.139 1961 11 2.111 -1.530 0 0 2.111 -1.530 -0.215 -0.738 1961 12 -5.611 -3.484 0 0 -5.611 -3.484 -7.136 -1.890 1962 1 -6.944 -3.685 0 0 -6.944 -3.685 -8.323 -1.946 1962 2 1.889 1.526 0 0 1.889 1.526 -0.427 2.329 1962 3 2.833 -1.712 0 0 2.833 -1.712 -1.316 -2.743 1962 4 12.278 2.695 0 0 12.278 2.695 8.545 2.080 1962 5 15.000 -0.215 0 0 15.000 -0.215 11.921 -0.176 1962 6 21.222 0.721 0 0 21.222 0.721 16.906 -0.476 1962 7 24.611 0.422 0 0 24.611 0.422 20.306 -0.765 1962 8 23.667 1.069 0 0 23.667 1.069 19.367 -0.112 1962 9 18.833 0.951 0 0 18.833 0.951 15.256 0.491 1962 10 12.278 0.887 0 0 12.278 0.887 10.078 1.806 1962 11 5.222 1.582 0 0 5.222 1.582 3.302 2.779 1962 12 -3.444 -1.317 0 0 -3.444 -1.317 -3.961 1.284 1963 1 -12.444 -9.185 0 0 -12.444 -9.185 -10.350 -3.972 1963 2 2.556 2.193 0 0 2.556 2.193 0.735 3.491 1963 3 3.722 -0.823 0 0 3.722 -0.823 0.905 -0.522 1963 4 9.333 -0.250 0 0 9.333 -0.250 6.449 -0.015 1963 5 17.722 2.507 0 0 17.722 2.507 14.217 2.120 1963 6 20.389 -0.112 0 0 20.389 -0.112 16.803 -0.580 1963 7 NaN NaN NaN NaN NaN NaN 22.118 1.048 1963 8 NaN NaN NaN NaN NaN NaN 19.432 -0.047 1963 9 NaN NaN NaN NaN NaN NaN 16.726 1.961 1963 10 NaN NaN NaN NaN NaN NaN 12.068 3.796 1963 11 NaN NaN NaN NaN NaN NaN 2.590 2.068 1963 12 NaN NaN NaN NaN NaN NaN -5.549 -0.304 1964 1 NaN NaN NaN NaN NaN NaN -7.505 -1.127 1964 2 NaN NaN NaN NaN NaN NaN -5.595 -2.839 1964 3 NaN NaN NaN NaN NaN NaN -2.440 -3.867 1964 4 NaN NaN NaN NaN NaN NaN 5.418 -1.047 1964 5 NaN NaN NaN NaN NaN NaN 12.075 -0.022 1964 6 NaN NaN NaN NaN NaN NaN 16.191 -1.192