% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 37553 % Primary Name: CONNEAUT % Record Type: TAVG % Country: United States % State: OH % Latitude: 41.98330 +/- 0.00005 % Longitude: -80.56670 +/- 0.00005 % Elevation (m): 195.10 +/- 0.05 % # of Months: 46 % % Alternate Names: CONNEAUT WTR WKS % % IDs: coop - 331818 % ghcnd - USC00331818 % ncdc - 20015664 % nws - CNTO1 % nws - CONO1 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % US Cooperative Summary of the Month % Multi-network Metadata System % % Site Hash: ff2f9b935af2bfac3d81aa3e48faef1d % Raw Data Hash: 413379c95edb00f15a28dd12d72dc956 % Adj Data Hash: 1be5287a0ef88ee509bdedcf8ba3627d % % 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 1909 7 NaN NaN NaN NaN NaN NaN 19.168 -1.065 1909 8 NaN NaN NaN NaN NaN NaN 19.690 -0.049 1909 9 NaN NaN NaN NaN NaN NaN 15.478 -0.838 1909 10 NaN NaN NaN NaN NaN NaN 8.103 -2.419 1909 11 NaN NaN NaN NaN NaN NaN 7.486 2.647 1909 12 NaN NaN NaN NaN NaN NaN -3.941 -2.559 1910 1 NaN NaN NaN NaN NaN NaN -4.220 0.417 1910 2 NaN NaN NaN NaN NaN NaN -7.008 -2.593 1910 3 NaN NaN NaN NaN NaN NaN 4.690 4.459 1910 4 NaN NaN NaN NaN NaN NaN 8.331 1.624 1910 5 NaN NaN NaN NaN NaN NaN 10.356 -2.241 1910 6 NaN NaN NaN NaN NaN NaN 16.511 -1.257 1910 7 21.973 0.266 0 0 21.973 0.266 20.462 0.229 1910 8 21.731 0.518 0 0 21.731 0.518 19.202 -0.537 1910 9 17.478 -0.312 0 0 17.478 -0.312 16.007 -0.309 1910 10 12.802 0.806 0 0 12.802 0.806 11.533 1.011 1910 11 2.851 -3.461 0 0 2.851 -3.461 2.721 -2.119 1910 12 -3.561 -3.653 0 0 -3.561 -3.653 -5.359 -3.978 1911 1 -0.688 2.476 0 0 -0.688 2.476 -2.679 1.959 1911 2 -1.050 1.891 0 0 -1.050 1.891 -3.107 1.308 1911 3 0.560 -1.145 0 0 0.560 -1.145 -0.947 -1.178 1911 4 7.513 -0.667 0 0 7.513 -0.667 5.943 -0.763 1911 5 17.603 3.532 0 0 17.603 3.532 15.619 3.022 1911 6 20.272 1.030 0 0 20.272 1.030 18.423 0.655 1911 7 22.769 1.062 0 0 22.769 1.062 20.799 0.566 1911 8 21.676 0.463 0 0 21.676 0.463 19.822 0.083 1911 9 18.213 0.423 0 0 18.213 0.423 16.541 0.225 1911 10 10.821 -1.175 0 0 10.821 -1.175 9.859 -0.662 1911 11 2.818 -3.495 0 0 2.818 -3.495 2.781 -2.058 1911 12 2.579 2.486 0 0 2.579 2.486 1.136 2.517 1912 1 -8.990 -5.826 1 0 NaN NaN -10.532 -5.894 1912 2 -6.493 -3.552 1 0 NaN NaN -8.528 -4.113 1912 3 -2.156 -3.861 0 0 -2.156 -3.861 -3.825 -4.055 1912 4 8.011 -0.169 1 0 NaN NaN 6.692 -0.015 1912 5 15.360 1.288 1 0 NaN NaN 13.100 0.503 1912 6 17.583 -1.659 0 0 17.583 -1.659 16.031 -1.738 1912 7 21.785 0.079 0 0 21.785 0.079 19.864 -0.369 1912 8 19.476 -1.737 0 0 19.476 -1.737 17.341 -2.398 1912 9 19.140 1.350 0 0 19.140 1.350 17.809 1.493 1912 10 12.715 0.719 0 0 12.715 0.719 11.153 0.631 1912 11 6.335 0.022 0 0 6.335 0.022 5.713 0.874 1912 12 0.964 0.872 0 0 0.964 0.872 0.092 1.474 1913 1 1.948 5.112 0 0 1.948 5.112 -0.526 4.111 1913 2 -4.043 -1.102 0 0 -4.043 -1.102 -6.296 -1.881 1913 3 2.935 1.231 0 0 2.935 1.231 0.725 0.494 1913 4 8.242 0.061 0 0 8.242 0.061 7.520 0.814 1913 5 13.376 -0.696 0 0 13.376 -0.696 11.737 -0.860 1913 6 18.935 -0.307 0 0 18.935 -0.307 17.459 -0.309 1913 7 21.516 -0.191 0 0 21.516 -0.191 19.962 -0.271 1913 8 21.161 -0.052 0 0 21.161 -0.052 19.596 -0.143 1913 9 17.288 -0.502 0 0 17.288 -0.502 15.575 -0.741 1913 10 12.226 0.230 0 0 12.226 0.230 11.140 0.618 1913 11 6.777 0.464 0 0 6.777 0.464 6.520 1.681 1913 12 1.379 1.287 0 0 1.379 1.287 0.537 1.918 1914 1 -1.181 1.983 0 0 -1.181 1.983 -2.608 2.030 1914 2 NaN NaN NaN NaN NaN NaN -9.313 -4.898 1914 3 0.261 -1.443 0 0 0.261 -1.443 -0.701 -0.932 1914 4 6.800 -1.380 0 0 6.800 -1.380 5.822 -0.885 1914 5 12.614 -1.458 1 0 NaN NaN 13.365 0.767 1914 6 NaN NaN NaN NaN NaN NaN 17.416 -0.353 1914 7 NaN NaN NaN NaN NaN NaN 20.091 -0.142 1914 8 NaN NaN NaN NaN NaN NaN 19.711 -0.028 1914 9 NaN NaN NaN NaN NaN NaN 15.599 -0.718 1914 10 NaN NaN NaN NaN NaN NaN 12.357 1.835 1914 11 NaN NaN NaN NaN NaN NaN 4.625 -0.215 1914 12 NaN NaN NaN NaN NaN NaN -3.796 -2.414 1915 1 NaN NaN NaN NaN NaN NaN -5.496 -0.858 1915 2 NaN NaN NaN NaN NaN NaN -2.614 1.801 1915 3 NaN NaN NaN NaN NaN NaN -1.794 -2.025 1915 4 NaN NaN NaN NaN NaN NaN 9.587 2.881 1915 5 NaN NaN NaN NaN NaN NaN 10.187 -2.411