% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 12255 % Primary Name: TEJAN % Record Type: TAVG % Country: China % Latitude: 39.70000 +/- 0.00500 % Longitude: 76.35000 +/- 0.00500 % Elevation (m): 1242.84 +/- 62.76 % # of Months: 14 % % IDs: gsod - 517060-99999 % usaf - 517060 % % Sources: Global Summary of the Day % % Site Hash: edcded8ee02b48856aead985076ef8b7 % Raw Data Hash: a3f77a6be9096e2de0d1fb0f38fe69ae % Adj Data Hash: 480eb28889d3cb12d9726d4098de999a % % 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 1955 8 NaN NaN NaN NaN NaN NaN 24.658 1.306 1955 9 NaN NaN NaN NaN NaN NaN 18.530 -0.198 1955 10 NaN NaN NaN NaN NaN NaN 11.787 0.515 1955 11 NaN NaN NaN NaN NaN NaN 3.009 0.407 1955 12 NaN NaN NaN NaN NaN NaN -1.132 3.467 1956 1 NaN NaN NaN NaN NaN NaN -8.707 -1.690 1956 2 NaN NaN NaN NaN NaN NaN -0.127 1.952 1956 3 NaN NaN NaN NaN NaN NaN 6.871 0.054 1956 4 NaN NaN NaN NaN NaN NaN 15.154 0.714 1956 5 NaN NaN NaN NaN NaN NaN 20.607 1.599 1956 6 NaN NaN NaN NaN NaN NaN 22.287 -0.475 1956 7 NaN NaN NaN NaN NaN NaN 26.840 2.155 1956 8 24.167 -0.519 1 0 NaN NaN 23.741 0.390 1956 9 22.675 2.612 1 0 NaN NaN 19.809 1.081 1956 10 13.494 0.888 1 0 NaN NaN 11.724 0.452 1956 11 4.424 0.488 0 0 4.424 0.488 3.252 0.650 1956 12 -4.063 -0.799 0 0 -4.063 -0.799 -4.768 -0.170 1957 1 -5.293 0.390 0 0 -5.293 0.390 -6.486 0.530 1957 2 -4.739 -3.995 1 0 NaN NaN -4.989 -2.911 1957 3 10.463 2.312 0 0 10.463 2.312 8.529 1.713 1957 4 14.374 -1.399 0 0 14.374 -1.399 13.077 -1.362 1957 5 19.453 -0.889 0 0 19.453 -0.889 17.464 -1.544 1957 6 23.871 -0.224 1 0 NaN NaN 22.183 -0.579 1957 7 24.676 -1.344 0 0 24.676 -1.344 23.520 -1.165 1957 8 23.380 -1.306 0 0 23.380 -1.306 22.040 -1.312 1957 9 18.726 -1.336 0 0 18.726 -1.336 17.505 -1.223 1957 10 NaN NaN NaN NaN NaN NaN 10.659 -0.613 1957 11 NaN NaN NaN NaN NaN NaN 2.942 0.340 1957 12 NaN NaN NaN NaN NaN NaN -2.569 2.029 1958 1 NaN NaN NaN NaN NaN NaN -5.464 1.553 1958 2 NaN NaN NaN NaN NaN NaN -0.134 1.945 1958 3 NaN NaN NaN NaN NaN NaN 8.937 2.120 1958 4 NaN NaN NaN NaN NaN NaN 16.105 1.665 1958 5 NaN NaN NaN NaN NaN NaN 16.731 -2.277 1958 6 NaN NaN NaN NaN NaN NaN 22.602 -0.159 1958 7 NaN NaN NaN NaN NaN NaN 24.917 0.232 1958 8 NaN NaN NaN NaN NaN NaN 21.285 -2.066 1958 9 NaN NaN NaN NaN NaN NaN 19.180 0.452