% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 37375 % Primary Name: SMITHFIELD % Record Type: TAVG % Country: United States % State: UT % Latitude: 41.83330 +/- 0.00005 % Longitude: -111.91670 +/- 0.00005 % Elevation (m): 1383.18 +/- 0.15 % # of Months: 66 % % Alternate Names: Missing Station ID - 427885 % % IDs: coop - 427885 % ghcnd - USC00427885 % ncdc - 12005641 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: 181b663b55a69c69628b6a59af43cafb % Raw Data Hash: 424fed81ad5c39e15ece66e9fc5040d7 % Adj Data Hash: 5b0bf9043e12eb0738977d727aeda2df % % 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 1923 9 NaN NaN NaN NaN NaN NaN 10.814 -0.265 1923 10 NaN NaN NaN NaN NaN NaN 3.117 -1.957 1923 11 NaN NaN NaN NaN NaN NaN -0.577 1.683 1923 12 NaN NaN NaN NaN NaN NaN -8.695 -1.269 1924 1 NaN NaN NaN NaN NaN NaN -12.115 -3.235 1924 2 NaN NaN NaN NaN NaN NaN -4.054 2.834 1924 3 NaN NaN NaN NaN NaN NaN -6.958 -3.207 1924 4 NaN NaN NaN NaN NaN NaN 1.436 -0.830 1924 5 NaN NaN NaN NaN NaN NaN 9.274 0.924 1924 6 NaN NaN NaN NaN NaN NaN 11.800 -0.919 1924 7 NaN NaN NaN NaN NaN NaN 16.585 -0.414 1924 8 NaN NaN NaN NaN NaN NaN 14.952 -0.876 1924 9 13.533 -1.918 0 0 15.157 -0.295 10.041 -1.038 1924 10 6.719 -2.726 0 0 8.343 -1.103 4.861 -0.213 1924 11 -0.097 -2.209 0 0 1.527 -0.586 -3.236 -0.976 1924 12 -11.081 -8.028 0 0 -9.457 -6.404 -11.369 -3.944 1925 1 NaN NaN NaN NaN NaN NaN -8.072 0.808 1925 2 -2.025 0.490 0 0 -0.402 2.114 -3.539 3.349 1925 3 2.405 1.783 0 0 4.028 3.407 -2.117 1.634 1925 4 6.962 0.324 0 0 8.585 1.947 3.566 1.301 1925 5 12.673 -0.050 0 0 14.296 1.574 9.721 1.371 1925 6 14.898 -2.193 0 0 16.522 -0.569 10.731 -1.988 1925 7 19.911 -1.460 0 0 21.535 0.163 17.795 0.795 1925 8 16.750 -3.451 0 0 18.373 -1.827 14.346 -1.483 1925 9 11.912 -3.540 0 0 13.535 -1.916 10.131 -0.948 1925 10 7.277 -2.168 0 0 8.901 -0.545 4.166 -0.908 1925 11 1.402 -0.711 0 4 0.980 -1.133 -2.640 -0.381 1925 12 -0.318 2.735 0 0 -0.740 2.313 -4.805 2.621 1926 1 -5.476 -0.968 0 0 -5.898 -1.390 -9.063 -0.183 1926 2 -2.200 0.315 0 0 -2.622 -0.107 -3.747 3.141 1926 3 2.887 2.266 0 0 2.465 1.843 -2.660 1.090 1926 4 9.967 3.329 0 0 9.545 2.907 5.220 2.955 1926 5 13.689 0.966 0 0 13.267 0.544 9.031 0.681 1926 6 19.355 2.264 0 0 18.933 1.842 13.492 0.774 1926 7 21.076 -0.296 0 0 20.654 -0.718 17.171 0.171 1926 8 20.374 0.174 0 0 19.952 -0.248 15.594 -0.234 1926 9 12.880 -2.571 0 0 12.458 -2.993 8.404 -2.675 1926 10 NaN NaN NaN NaN NaN NaN 5.919 0.845 1926 11 NaN NaN NaN NaN NaN NaN 0.599 2.859 1926 12 -5.302 -2.249 0 0 -5.724 -2.671 -7.925 -0.500 1927 1 -4.319 0.188 0 0 -4.741 -0.234 -7.311 1.569 1927 2 -1.000 1.515 0 0 -1.422 1.093 -5.504 1.384 1927 3 2.804 2.183 0 0 2.382 1.761 -4.526 -0.776 1927 4 7.290 0.652 0 0 6.868 0.230 1.970 -0.296 1927 5 11.571 -1.151 0 0 11.149 -1.573 6.768 -1.582 1927 6 18.077 0.986 0 0 17.655 0.564 12.470 -0.249 1927 7 20.768 -0.604 0 0 20.346 -1.026 17.069 0.070 1927 8 18.135 -2.065 0 0 17.713 -2.487 14.251 -1.578 1927 9 15.297 -0.155 0 0 14.875 -0.577 10.140 -0.939 1927 10 10.440 0.995 0 0 10.018 0.572 6.144 1.070 1927 11 5.961 3.848 0 0 5.539 3.426 1.154 3.413 1927 12 -4.581 -1.528 0 0 -5.003 -1.950 -10.817 -3.392 1928 1 -2.903 1.604 0 0 -3.325 1.182 -6.370 2.510 1928 2 -1.245 1.270 1 0 NaN NaN -7.720 -0.832 1928 3 5.532 4.911 1 0 NaN NaN -2.681 1.070 1928 4 7.032 0.394 0 0 6.610 -0.028 0.804 -1.462 1928 5 16.098 3.376 0 0 15.676 2.954 10.413 2.063 1928 6 16.377 -0.714 0 0 15.955 -1.136 10.136 -2.583 1928 7 21.866 0.495 1 0 NaN NaN 16.776 -0.223 1928 8 19.971 -0.230 0 0 19.549 -0.652 14.698 -1.131 1928 9 16.107 0.655 0 0 15.685 0.233 11.144 0.065 1928 10 9.639 0.193 0 0 9.217 -0.229 5.376 0.302 1928 11 3.307 1.194 0 0 2.885 0.772 -2.087 0.172 1928 12 -6.492 -3.439 0 0 -6.914 -3.861 -11.443 -4.018 1929 1 -6.947 -2.439 0 0 -7.369 -2.861 -11.751 -2.871 1929 2 -6.073 -3.558 0 0 -6.495 -3.980 -11.643 -4.756 1929 3 2.805 2.183 0 0 2.383 1.761 -4.477 -0.727 1929 4 6.598 -0.040 0 0 6.176 -0.462 0.425 -1.841 1929 5 11.782 -0.940 0 0 11.360 -1.362 7.208 -1.142 1929 6 15.598 -1.493 0 0 15.176 -1.915 11.144 -1.575 1929 7 22.332 0.961 0 0 21.910 0.539 18.027 1.028 1929 8 22.744 2.543 0 0 22.321 2.121 17.501 1.673 1929 9 13.679 -1.773 0 0 13.257 -2.195 9.020 -2.060 1929 10 10.429 0.983 0 0 10.007 0.561 5.909 0.835 1929 11 2.032 -0.081 0 0 1.610 -0.503 -3.367 -1.108 1929 12 0.776 3.829 0 0 0.354 3.407 -3.603 3.822 1930 1 -11.285 -6.778 0 0 -11.708 -7.200 -14.777 -5.897 1930 2 1.112 3.628 0 0 0.690 3.206 -2.629 4.259 1930 3 4.682 4.061 0 0 4.260 3.639 -3.233 0.518 1930 4 11.502 4.864 0 0 11.080 4.442 6.070 3.804 1930 5 10.673 -2.050 0 0 10.251 -2.472 7.274 -1.076 1930 6 NaN NaN NaN NaN NaN NaN 11.441 -1.277 1930 7 NaN NaN NaN NaN NaN NaN 17.924 0.925 1930 8 NaN NaN NaN NaN NaN NaN 16.400 0.571 1930 9 NaN NaN NaN NaN NaN NaN 10.788 -0.291 1930 10 NaN NaN NaN NaN NaN NaN 4.323 -0.750 1930 11 NaN NaN NaN NaN NaN NaN -5.298 -3.039 1930 12 NaN NaN NaN NaN NaN NaN -12.234 -4.808 1931 1 NaN NaN NaN NaN NaN NaN -9.655 -0.775 1931 2 NaN NaN NaN NaN NaN NaN -6.070 0.818 1931 3 NaN NaN NaN NaN NaN NaN -4.699 -0.948 1931 4 NaN NaN NaN NaN NaN NaN 3.186 0.921 1931 5 NaN NaN NaN NaN NaN NaN 7.915 -0.435