% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 33313 % Primary Name: MANHATTAN POWER HOUSE % Record Type: TAVG % Country: United States % State: NV % Latitude: 38.53330 +/- 0.00005 % Longitude: -117.08330 +/- 0.00005 % Elevation (m): 2108.00 +/- 0.05 % # of Months: 14 % % Alternate Names: MANHATTAN PWR HOUSE % % IDs: coop - 264835 % ghcnd - USC00264835 % ncdc - 20019093 % % Sources: US Cooperative Summary of the Day % Global Historical Climatology Network - Daily % US Cooperative Summary of the Month % Multi-network Metadata System % % Site Hash: 0e9e7e40e74440c40df38ea6cabf6fcb % Raw Data Hash: a3c6242da7af1d829540abdc25b15502 % Adj Data Hash: bb3ab5e49dc0365d05483b008a50ab07 % % 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 1949 6 NaN NaN NaN NaN NaN NaN 14.784 -0.858 1949 7 NaN NaN NaN NaN NaN NaN 20.353 -0.018 1949 8 NaN NaN NaN NaN NaN NaN 18.487 -0.579 1949 9 NaN NaN NaN NaN NaN NaN 15.755 1.224 1949 10 NaN NaN NaN NaN NaN NaN 7.839 -0.767 1949 11 NaN NaN NaN NaN NaN NaN 6.051 3.990 1949 12 NaN NaN NaN NaN NaN NaN -3.114 -0.749 1950 1 NaN NaN NaN NaN NaN NaN -4.305 -1.247 1950 2 NaN NaN NaN NaN NaN NaN 1.743 2.178 1950 3 NaN NaN NaN NaN NaN NaN 1.487 -0.414 1950 4 NaN NaN NaN NaN NaN NaN 6.461 0.899 1950 5 NaN NaN NaN NaN NaN NaN 9.829 -0.813 1950 6 16.056 -0.193 0 0 16.056 -0.193 14.269 -1.373 1950 7 20.333 -0.645 0 0 20.333 -0.645 20.463 0.093 1950 8 19.333 -0.340 0 0 19.333 -0.340 18.698 -0.368 1950 9 13.533 -1.605 0 0 13.533 -1.605 13.937 -0.595 1950 10 11.444 2.232 0 0 11.444 2.232 11.256 2.650 1950 11 6.500 3.832 0 0 6.500 3.832 4.841 2.779 1950 12 3.833 5.591 0 0 3.833 5.591 1.814 4.180 1951 1 -1.389 1.062 0 0 -1.389 1.062 -1.987 1.072 1951 2 0.278 0.105 0 0 0.278 0.105 0.610 1.045 1951 3 1.389 -1.120 0 0 1.389 -1.120 0.732 -1.169 1951 4 7.833 1.664 0 0 7.833 1.664 6.985 1.423 1951 5 10.500 -0.750 0 0 10.500 -0.750 10.842 0.199 1951 6 15.722 -0.526 0 0 15.722 -0.526 14.606 -1.036 1951 7 20.889 -0.089 0 0 20.889 -0.089 20.688 0.318 1951 8 NaN NaN NaN NaN NaN NaN 18.261 -0.805 1951 9 NaN NaN NaN NaN NaN NaN 15.464 0.932 1951 10 NaN NaN NaN NaN NaN NaN 7.838 -0.767 1951 11 NaN NaN NaN NaN NaN NaN 1.595 -0.467 1951 12 NaN NaN NaN NaN NaN NaN -5.065 -2.700 1952 1 NaN NaN NaN NaN NaN NaN -5.599 -2.541 1952 2 NaN NaN NaN NaN NaN NaN -2.131 -1.696 1952 3 NaN NaN NaN NaN NaN NaN -2.721 -4.622 1952 4 NaN NaN NaN NaN NaN NaN 6.714 1.152 1952 5 NaN NaN NaN NaN NaN NaN 11.800 1.158 1952 6 NaN NaN NaN NaN NaN NaN 13.747 -1.894 1952 7 NaN NaN NaN NaN NaN NaN 20.346 -0.025