% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 37416 % Primary Name: STEELE SWAMP % Record Type: TAVG % Country: United States % State: CA % Latitude: 41.86670 +/- 0.00005 % Longitude: -120.95000 +/- 0.00005 % Elevation (m): 1388.10 +/- 0.05 % # of Months: 23 % % Alternate Names: Missing Station ID - 48521 % % IDs: coop - 48521 % ghcnd - USC00048521 % ncdc - 20003247 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % US Cooperative Summary of the Month % Multi-network Metadata System % % Site Hash: 59a3f18d0aab9ab647907964c8b46ead % Raw Data Hash: 46c45f589a0405fec643cf050cc3574b % Adj Data Hash: e9c0fb872d9f8d08e496a15602fd1bcc % % 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 1947 5 NaN NaN NaN NaN NaN NaN 14.062 2.989 1947 6 NaN NaN NaN NaN NaN NaN 13.744 -1.689 1947 7 NaN NaN NaN NaN NaN NaN 17.548 -1.853 1947 8 NaN NaN NaN NaN NaN NaN 16.680 -1.854 1947 9 NaN NaN NaN NaN NaN NaN 16.149 0.691 1947 10 NaN NaN NaN NaN NaN NaN 10.328 0.362 1947 11 NaN NaN NaN NaN NaN NaN 3.192 -1.069 1947 12 NaN NaN NaN NaN NaN NaN 0.917 0.138 1948 1 NaN NaN NaN NaN NaN NaN 2.633 2.493 1948 2 NaN NaN NaN NaN NaN NaN 1.117 -1.214 1948 3 NaN NaN NaN NaN NaN NaN 1.068 -2.518 1948 4 NaN NaN NaN NaN NaN NaN 3.318 -3.128 1948 5 9.333 -1.462 0 0 9.333 -1.462 9.037 -2.036 1948 6 15.556 0.400 0 0 15.556 0.400 14.702 -0.730 1948 7 18.889 -0.235 0 0 18.889 -0.235 18.116 -1.286 1948 8 17.333 -0.924 0 0 17.333 -0.924 16.608 -1.926 1948 9 14.500 -0.680 0 0 14.500 -0.680 14.534 -0.924 1948 10 9.667 -0.022 0 0 9.667 -0.022 10.214 0.248 1948 11 2.222 -1.761 0 0 2.222 -1.761 3.306 -0.954 1948 12 -4.556 -5.057 0 0 -4.556 -5.057 -2.827 -3.606 1949 1 -12.778 -12.641 1 0 NaN NaN -5.289 -5.429 1949 2 -3.611 -5.665 0 0 -3.611 -5.665 -0.802 -3.133 1949 3 2.667 -0.642 0 0 2.667 -0.642 2.476 -1.110 1949 4 9.778 3.610 0 0 9.778 3.610 8.947 2.502 1949 5 11.667 0.871 0 0 11.667 0.871 11.790 0.717 1949 6 15.611 0.456 0 0 15.611 0.456 15.564 0.131 1949 7 19.944 0.820 0 0 19.944 0.820 19.572 0.171 1949 8 18.000 -0.257 0 0 18.000 -0.257 17.025 -1.509 1949 9 15.722 0.542 0 0 15.722 0.542 16.450 0.992 1949 10 7.444 -2.244 0 0 7.444 -2.244 8.911 -1.054 1949 11 7.222 3.239 0 0 7.222 3.239 7.521 3.260 1949 12 -1.611 -2.112 0 0 -1.611 -2.112 -0.212 -0.991 1950 1 NaN NaN NaN NaN NaN NaN -3.348 -3.489 1950 2 1.278 -0.776 0 0 1.278 -0.776 2.518 0.187 1950 3 3.278 -0.031 0 0 3.278 -0.031 2.545 -1.041 1950 4 6.389 0.221 0 0 6.389 0.221 6.827 0.381 1950 5 NaN NaN NaN NaN NaN NaN 11.474 0.402 1950 6 NaN NaN NaN NaN NaN NaN 14.366 -1.067 1950 7 NaN NaN NaN NaN NaN NaN 20.886 1.484 1950 8 NaN NaN NaN NaN NaN NaN 19.269 0.735 1950 9 NaN NaN NaN NaN NaN NaN 15.769 0.311 1950 10 NaN NaN NaN NaN NaN NaN 10.490 0.524 1950 11 NaN NaN NaN NaN NaN NaN 6.263 2.003 1950 12 NaN NaN NaN NaN NaN NaN 3.884 3.106 1951 1 NaN NaN NaN NaN NaN NaN 0.094 -0.046 1951 2 NaN NaN NaN NaN NaN NaN 2.448 0.117 1951 3 NaN NaN NaN NaN NaN NaN 2.369 -1.217 1951 4 NaN NaN NaN NaN NaN NaN 8.841 2.396