% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 40700 % Primary Name: LEWISTON % Record Type: TAVG % Country: United States % State: MI % Latitude: 44.98330 +/- 0.00005 % Longitude: -84.33330 +/- 0.00005 % Elevation (m): 422.04 +/- 47.30 % # of Months: 48 % % Alternate Names: Missing Station ID - 204755 % % IDs: coop - 204755 % ghcnd - USC00204755 % ncdc - 30015139 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: d1d379acf9e0f381cf0ae08503c7aeb5 % Raw Data Hash: b27f6d789bf209d3eb1c95bae52bf208 % Adj Data Hash: 70e8f942a7ffb8692bab56dc8b551564 % % 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 1892 1 NaN NaN NaN NaN NaN NaN -9.698 -1.537 1892 2 NaN NaN NaN NaN NaN NaN -7.267 0.817 1892 3 NaN NaN NaN NaN NaN NaN -5.101 -1.809 1892 4 NaN NaN NaN NaN NaN NaN 2.257 -1.577 1892 5 NaN NaN NaN NaN NaN NaN 8.579 -1.571 1892 6 NaN NaN NaN NaN NaN NaN 14.917 -0.403 1892 7 NaN NaN NaN NaN NaN NaN 18.627 0.102 1892 8 NaN NaN NaN NaN NaN NaN 17.883 -0.163 1892 9 NaN NaN NaN NaN NaN NaN 13.782 -0.020 1892 10 NaN NaN NaN NaN NaN NaN 8.086 -0.406 1892 11 NaN NaN NaN NaN NaN NaN 0.214 -1.946 1892 12 NaN NaN NaN NaN NaN NaN -6.098 -1.490 1893 1 -11.805 -5.251 1 0 NaN NaN -12.609 -4.448 1893 2 -9.762 -3.285 0 0 -9.762 -3.285 -11.508 -3.425 1893 3 -3.648 -1.964 0 0 -3.648 -1.964 -5.263 -1.972 1893 4 3.630 -1.811 0 0 3.630 -1.811 1.460 -2.374 1893 5 11.308 -0.449 0 0 11.308 -0.449 8.077 -2.074 1893 6 21.389 4.462 0 0 21.389 4.462 16.793 1.473 1893 7 21.129 0.997 0 0 21.129 0.997 18.312 -0.212 1893 8 20.090 0.437 0 0 20.090 0.437 17.429 -0.617 1893 9 13.963 -1.446 0 0 13.963 -1.446 12.291 -1.512 1893 10 8.943 -1.156 0 0 8.943 -1.156 8.979 0.488 1893 11 0.944 -2.822 0 0 0.944 -2.822 1.892 -0.267 1893 12 -6.810 -3.809 0 0 -6.810 -3.809 -7.681 -3.073 1894 1 -5.426 1.128 0 0 -5.426 1.128 -7.051 1.109 1894 2 -7.702 -1.225 0 0 -7.702 -1.225 -9.701 -1.618 1894 3 1.828 3.513 0 0 1.828 3.513 -0.168 3.124 1894 4 7.889 2.448 0 0 7.889 2.448 5.275 1.440 1894 5 10.037 -1.721 0 0 10.037 -1.721 8.440 -1.711 1894 6 20.590 3.663 0 0 20.590 3.663 16.574 1.254 1894 7 21.667 1.535 0 0 21.667 1.535 18.991 0.466 1894 8 18.853 -0.800 0 0 18.853 -0.800 16.291 -1.755 1894 9 16.758 1.349 0 0 16.758 1.349 14.661 0.858 1894 10 8.710 -1.389 0 0 8.710 -1.389 8.779 0.287 1894 11 -1.981 -5.748 0 0 -1.981 -5.748 -0.653 -2.813 1894 12 -2.957 0.044 0 0 -2.957 0.044 -2.687 1.921 1895 1 -9.000 -2.446 0 0 -9.000 -2.446 -9.398 -1.237 1895 2 -10.060 -3.583 0 0 -10.060 -3.583 -11.185 -3.101 1895 3 -5.609 -3.925 0 0 -5.609 -3.925 -7.365 -4.074 1895 4 6.948 1.507 0 0 6.948 1.507 4.833 0.999 1895 5 15.169 3.412 0 0 15.169 3.412 11.058 0.907 1895 6 20.315 3.388 0 0 20.315 3.388 16.513 1.193 1895 7 19.255 -0.877 0 0 19.255 -0.877 16.589 -1.936 1895 8 18.829 -0.824 0 0 18.829 -0.824 16.724 -1.322 1895 9 16.785 1.376 0 0 16.785 1.376 14.783 0.981 1895 10 4.945 -5.153 0 0 4.945 -5.153 5.220 -3.271 1895 11 -0.122 -3.888 0 0 -0.122 -3.888 0.555 -1.605 1895 12 -3.708 -0.707 0 0 -3.708 -0.707 -4.013 0.595 1896 1 -6.220 0.334 0 0 -6.220 0.334 -7.210 0.951 1896 2 -6.852 -0.375 1 0 NaN NaN -7.801 0.282 1896 3 -5.197 -3.512 0 0 -5.197 -3.512 -6.805 -3.513 1896 4 8.347 2.906 0 0 8.347 2.906 5.609 1.774 1896 5 16.184 4.426 0 0 16.184 4.426 12.476 2.326 1896 6 18.975 2.048 1 0 NaN NaN 15.688 0.368 1896 7 20.300 0.168 1 0 NaN NaN 18.165 -0.359 1896 8 19.153 -0.500 0 0 19.153 -0.500 17.922 -0.124 1896 9 12.455 -2.954 0 0 12.455 -2.954 11.374 -2.429 1896 10 7.087 -3.011 0 0 7.087 -3.011 6.453 -2.039 1896 11 0.388 -3.378 0 0 0.388 -3.378 1.157 -1.002 1896 12 -4.260 -1.259 0 0 -4.260 -1.259 -4.394 0.214 1897 1 NaN NaN NaN NaN NaN NaN -7.088 1.073 1897 2 NaN NaN NaN NaN NaN NaN -7.312 0.771 1897 3 NaN NaN NaN NaN NaN NaN -4.614 -1.322 1897 4 NaN NaN NaN NaN NaN NaN 3.322 -0.513 1897 5 NaN NaN NaN NaN NaN NaN 8.102 -2.048 1897 6 NaN NaN NaN NaN NaN NaN 12.569 -2.751 1897 7 NaN NaN NaN NaN NaN NaN 20.336 1.811 1897 8 NaN NaN NaN NaN NaN NaN 16.189 -1.857 1897 9 NaN NaN NaN NaN NaN NaN 15.055 1.253 1897 10 NaN NaN NaN NaN NaN NaN 9.825 1.334 1897 11 NaN NaN NaN NaN NaN NaN 0.694 -1.465 1897 12 NaN NaN NaN NaN NaN NaN -6.115 -1.507