% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 12165 % Primary Name: PU-LI /POULI % Record Type: TAVG % Country: China % Latitude: 37.78300 +/- 0.00050 % Longitude: 75.23300 +/- 0.00050 % Elevation (m): 3158.00 +/- 0.05 % # of Months: 38 % % IDs: gsod - 518040-99999 % usaf - 518040 % % Sources: Global Summary of the Day % % Site Hash: f47409873242a837d5a83347772e49fe % Raw Data Hash: d58e5667b60a2759bb09f87386ab4893 % Adj Data Hash: f3cf30e9bafe14a2e95073bba858762a % % 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 1956 2 NaN NaN NaN NaN NaN NaN -14.287 1.789 1956 3 NaN NaN NaN NaN NaN NaN -7.390 -0.046 1956 4 NaN NaN NaN NaN NaN NaN 0.539 0.746 1956 5 NaN NaN NaN NaN NaN NaN 5.783 2.178 1956 6 NaN NaN NaN NaN NaN NaN 7.533 -0.063 1956 7 NaN NaN NaN NaN NaN NaN 11.387 1.304 1956 8 NaN NaN NaN NaN NaN NaN 9.436 0.127 1956 9 NaN NaN NaN NaN NaN NaN 6.372 1.348 1956 10 NaN NaN NaN NaN NaN NaN -1.471 0.234 1956 11 NaN NaN NaN NaN NaN NaN -8.330 0.805 1956 12 NaN NaN NaN NaN NaN NaN -16.520 -0.132 1957 1 NaN NaN NaN NaN NaN NaN -20.115 -0.025 1957 2 -15.411 -5.566 0 0 -15.411 -5.566 -19.888 -3.811 1957 3 -2.773 -1.662 0 0 -2.773 -1.662 -7.403 -0.059 1957 4 4.898 -1.127 0 0 4.898 -1.127 -1.704 -1.497 1957 5 8.800 -1.038 0 0 8.800 -1.038 1.987 -1.618 1957 6 11.162 -2.666 0 0 11.162 -2.666 6.200 -1.396 1957 7 16.393 0.078 0 0 16.393 0.078 9.406 -0.677 1957 8 15.156 -0.385 0 0 15.156 -0.385 8.303 -1.006 1957 9 10.278 -0.978 0 0 10.278 -0.978 4.067 -0.957 1957 10 4.238 -0.289 0 0 4.238 -0.289 -2.317 -0.612 1957 11 -2.533 0.370 0 0 -2.533 0.370 -9.059 0.075 1957 12 -10.224 -0.068 0 0 -10.224 -0.068 -15.651 0.737 1958 1 -9.220 4.637 0 0 -9.220 4.637 -17.244 2.846 1958 2 -6.091 3.753 0 0 -6.091 3.753 -13.960 2.117 1958 3 1.901 3.013 0 0 1.901 3.013 -5.219 2.125 1958 4 9.720 3.695 0 0 9.720 3.695 1.956 2.162 1958 5 8.230 -1.607 0 0 8.230 -1.607 1.482 -2.123 1958 6 13.804 -0.024 0 0 13.804 -0.024 7.553 -0.043 1958 7 17.197 0.882 0 0 17.197 0.882 10.485 0.402 1958 8 13.491 -2.050 0 0 13.491 -2.050 7.489 -1.819 1958 9 12.576 1.320 0 0 12.576 1.320 5.865 0.841 1958 10 3.912 -0.615 0 0 3.912 -0.615 -2.075 -0.370 1958 11 -3.819 -0.916 0 0 -3.819 -0.916 -9.838 -0.703 1958 12 -9.441 0.715 0 0 -9.441 0.715 -14.571 1.817 1959 1 -19.244 -5.386 0 0 -19.244 -5.386 -21.708 -1.619 1959 2 -11.845 -2.001 0 0 -11.845 -2.001 -17.327 -1.250 1959 3 -0.355 0.757 0 0 -0.355 0.757 -7.297 0.047 1959 4 6.544 0.519 0 0 6.544 0.519 0.752 0.959 1959 5 7.728 -2.110 0 0 7.728 -2.110 1.245 -2.360 1959 6 14.002 0.173 0 0 14.002 0.173 7.632 0.036 1959 7 16.271 -0.045 0 0 16.271 -0.045 9.721 -0.362 1959 8 17.583 2.042 0 0 17.583 2.042 10.201 0.893 1959 9 15.161 3.905 1 0 NaN NaN 7.222 2.198 1959 10 6.611 2.084 0 0 6.611 2.084 0.144 1.849 1959 11 -1.902 1.000 0 0 -1.902 1.000 -8.885 0.250 1959 12 -9.136 1.020 0 0 -9.136 1.020 -15.928 0.460 1960 1 -11.561 2.297 0 0 -11.561 2.297 -18.711 1.378 1960 2 -10.525 -0.680 0 0 -10.525 -0.680 -13.651 2.426 1960 3 -1.423 -0.311 1 0 NaN NaN -8.204 -0.860 1960 4 NaN NaN NaN NaN NaN NaN -2.610 -2.403 1960 5 NaN NaN NaN NaN NaN NaN 2.052 -1.553 1960 6 NaN NaN NaN NaN NaN NaN 7.792 0.196 1960 7 NaN NaN NaN NaN NaN NaN 10.037 -0.046 1960 8 NaN NaN NaN NaN NaN NaN 9.769 0.460 1960 9 NaN NaN NaN NaN NaN NaN 5.036 0.013 1960 10 NaN NaN NaN NaN NaN NaN -1.496 0.210 1960 11 NaN NaN NaN NaN NaN NaN -10.143 -1.009 1960 12 NaN NaN NaN NaN NaN NaN -15.698 0.690 1961 1 NaN NaN NaN NaN NaN NaN -19.463 0.626 1961 2 NaN NaN NaN NaN NaN NaN -17.574 -1.497 1961 3 NaN NaN NaN NaN NaN NaN -7.496 -0.152