% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 29654 % Primary Name: MCCOLL NO. 2 % Record Type: TAVG % Country: United States % State: SC % Latitude: 34.68330 +/- 0.00005 % Longitude: -79.60000 +/- 0.00005 % Elevation (m): 64.01 +/- 0.15 % # of Months: 16 % % Alternate Names: Missing Station ID - 385635 % % IDs: coop - 385635 % ghcnd - USC00385635 % ncdc - 12004909 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % Multi-network Metadata System % % Site Hash: aa929c3756e85e327a66abd11578e919 % Raw Data Hash: 0349b8afc090098f5861c1e7e8a7aa7d % Adj Data Hash: 36c3a0e3f1a5603aa927fb1aae25eae8 % % 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 1940 2 NaN NaN NaN NaN NaN NaN 6.586 -0.771 1940 3 NaN NaN NaN NaN NaN NaN 10.335 -1.339 1940 4 NaN NaN NaN NaN NaN NaN 15.999 -0.815 1940 5 NaN NaN NaN NaN NaN NaN 20.239 -1.044 1940 6 NaN NaN NaN NaN NaN NaN 25.817 1.083 1940 7 NaN NaN NaN NaN NaN NaN 26.568 0.001 1940 8 NaN NaN NaN NaN NaN NaN 25.668 -0.419 1940 9 NaN NaN NaN NaN NaN NaN 22.348 -0.691 1940 10 NaN NaN NaN NaN NaN NaN 16.289 -0.396 1940 11 NaN NaN NaN NaN NaN NaN 11.890 0.339 1940 12 NaN NaN NaN NaN NaN NaN 9.005 1.949 1941 1 NaN NaN NaN NaN NaN NaN 5.955 -0.028 1941 2 5.031 -2.860 0 0 5.031 -2.860 3.905 -3.452 1941 3 NaN NaN NaN NaN NaN NaN 8.606 -3.068 1941 4 19.017 1.668 0 0 19.017 1.668 18.296 1.482 1941 5 23.287 1.469 0 0 23.287 1.469 22.111 0.828 1941 6 25.395 0.126 0 0 25.395 0.126 25.032 0.298 1941 7 27.288 0.186 0 0 27.288 0.186 26.924 0.357 1941 8 26.721 0.099 0 0 26.721 0.099 26.529 0.442 1941 9 25.189 1.615 0 0 25.189 1.615 24.856 1.817 1941 10 20.550 3.330 0 0 20.550 3.330 20.293 3.608 1941 11 12.321 0.236 1 0 NaN NaN 12.316 0.765 1941 12 NaN NaN NaN NaN NaN NaN 8.423 1.367 1942 1 6.627 0.110 0 0 6.627 0.110 5.935 -0.048 1942 2 NaN NaN NaN NaN NaN NaN 4.129 -3.228 1942 3 12.151 -0.058 1 0 NaN NaN 12.592 0.918 1942 4 NaN NaN NaN NaN NaN NaN 17.774 0.960 1942 5 24.041 2.223 1 0 NaN NaN 21.661 0.378 1942 6 26.330 1.061 1 0 NaN NaN 25.667 0.933 1942 7 28.230 1.129 0 0 28.230 1.129 27.446 0.880 1942 8 25.882 -0.740 1 0 NaN NaN 25.584 -0.503 1942 9 24.075 0.501 0 0 24.075 0.501 24.200 1.160 1942 10 NaN NaN NaN NaN NaN NaN 17.204 0.518 1942 11 NaN NaN NaN NaN NaN NaN 12.920 1.369 1942 12 NaN NaN NaN NaN NaN NaN 6.385 -0.671 1943 1 NaN NaN NaN NaN NaN NaN 7.318 1.335 1943 2 NaN NaN NaN NaN NaN NaN 7.868 0.511 1943 3 NaN NaN NaN NaN NaN NaN 10.925 -0.749 1943 4 NaN NaN NaN NaN NaN NaN 16.001 -0.813 1943 5 NaN NaN NaN NaN NaN NaN 22.076 0.793 1943 6 NaN NaN NaN NaN NaN NaN 27.148 2.414 1943 7 NaN NaN NaN NaN NaN NaN 26.364 -0.203 1943 8 NaN NaN NaN NaN NaN NaN 26.697 0.610 1943 9 NaN NaN NaN NaN NaN NaN 21.842 -1.197