% This file contains a station summary listing for a temperature % station in the Berkeley Earth database. This station is identified as: % % Berkeley ID#: 7920 % Primary Name: VICTORIA LANSDOWNE % Record Type: TAVG % Country: Canada % Latitude: 48.43000 +/- 0.00500 % Longitude: -123.32000 +/- 0.00500 % Elevation (m): 29.00 +/- 0.50 % # of Months: 102 % % IDs: ghcnd - CA001018640 % % Sources: Global Historical Climatology Network - Daily % % Site Hash: 812e3a12e461c7693130ed94cf98473a % Raw Data Hash: 25c730344e4e05460f4c1e72b8e85e9b % Adj Data Hash: 0fd9642686e07ad0ace2d95d5c3a08b8 % % 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 1953 1 NaN NaN NaN NaN NaN NaN 2.317 2.939 1953 2 NaN NaN NaN NaN NaN NaN 3.231 1.154 1953 3 NaN NaN NaN NaN NaN NaN 3.318 -0.075 1953 4 NaN NaN NaN NaN NaN NaN 6.013 -0.327 1953 5 NaN NaN NaN NaN NaN NaN 10.208 0.167 1953 6 NaN NaN NaN NaN NaN NaN 10.880 -1.897 1953 7 NaN NaN NaN NaN NaN NaN 14.888 -0.183 1953 8 NaN NaN NaN NaN NaN NaN 14.905 0.106 1953 9 NaN NaN NaN NaN NaN NaN 12.743 0.468 1953 10 NaN NaN NaN NaN NaN NaN 8.887 1.160 1953 11 NaN NaN NaN NaN NaN NaN 5.469 2.237 1953 12 NaN NaN NaN NaN NaN NaN 3.067 2.310 1954 1 2.208 0.183 0 0 2.208 0.183 -3.346 -2.724 1954 2 6.059 1.335 0 0 6.059 1.335 3.481 1.404 1954 3 4.855 -1.185 0 0 4.855 -1.185 1.876 -1.517 1954 4 7.583 -1.405 0 0 7.583 -1.405 4.121 -2.220 1954 5 11.702 -0.986 0 0 11.702 -0.986 10.004 -0.037 1954 6 13.055 -2.369 0 0 13.055 -2.369 10.715 -2.062 1954 7 14.787 -2.931 0 0 14.787 -2.931 13.130 -1.941 1954 8 14.971 -2.475 0 0 14.971 -2.475 13.264 -1.536 1954 9 13.753 -1.169 0 0 13.753 -1.169 12.350 0.075 1954 10 9.936 -0.437 0 0 9.936 -0.437 7.425 -0.302 1954 11 9.180 3.301 0 0 9.180 3.301 6.101 2.869 1954 12 5.453 2.049 0 0 5.453 2.049 2.212 1.455 1955 1 4.681 2.656 0 0 4.681 2.656 0.398 1.020 1955 2 3.622 -1.102 0 0 3.622 -1.102 1.113 -0.964 1955 3 3.708 -2.332 0 0 3.708 -2.332 -0.009 -3.402 1955 4 7.033 -1.955 0 0 7.033 -1.955 4.084 -2.257 1955 5 10.044 -2.644 0 0 10.044 -2.644 7.520 -2.521 1955 6 13.617 -1.807 0 0 13.617 -1.807 11.474 -1.303 1955 7 14.547 -3.171 0 0 14.547 -3.171 13.073 -1.998 1955 8 15.421 -2.025 0 0 15.421 -2.025 13.673 -1.126 1955 9 13.307 -1.615 0 0 13.307 -1.615 11.843 -0.432 1955 10 9.590 -0.783 0 0 9.590 -0.783 7.525 -0.202 1955 11 3.624 -2.255 0 0 3.624 -2.255 -0.371 -3.603 1955 12 3.336 -0.068 0 0 3.336 -0.068 -0.799 -1.556 1956 1 4.053 2.028 0 0 4.053 2.028 -0.749 -0.127 1956 2 2.279 -2.445 0 0 2.279 -2.445 -0.501 -2.578 1956 3 4.977 -1.063 0 0 4.977 -1.063 1.601 -1.792 1956 4 9.715 0.727 0 0 9.715 0.727 6.826 0.486 1956 5 13.360 0.672 0 0 13.360 0.672 11.456 1.415 1956 6 13.287 -2.137 0 0 13.287 -2.137 11.036 -1.741 1956 7 16.734 -0.984 0 0 16.734 -0.984 15.635 0.564 1956 8 16.397 -1.049 0 0 16.397 -1.049 14.965 0.166 1956 9 13.335 -1.587 0 0 13.335 -1.587 11.912 -0.363 1956 10 9.373 -1.000 0 0 9.373 -1.000 6.729 -0.997 1956 11 6.130 0.251 0 0 6.130 0.251 2.511 -0.721 1956 12 5.040 1.636 0 0 5.040 1.636 1.280 0.523 1957 1 0.441 -1.584 0 0 0.441 -1.584 -5.135 -4.513 1957 2 3.305 -1.419 0 0 3.305 -1.419 0.550 -1.527 1957 3 6.540 0.500 0 0 6.540 0.500 3.298 -0.095 1957 4 9.257 0.269 0 0 9.257 0.269 6.847 0.506 1957 5 13.690 1.002 0 0 13.690 1.002 12.055 2.014 1957 6 15.286 -0.138 0 0 15.286 -0.138 12.847 0.070 1957 7 15.385 -2.333 0 0 15.385 -2.333 13.486 -1.585 1957 8 15.659 -1.787 0 0 15.659 -1.787 13.786 -1.013 1957 9 15.681 0.759 0 0 15.681 0.759 14.424 2.150 1957 10 9.853 -0.520 0 0 9.853 -0.520 7.643 -0.083 1957 11 6.742 0.863 0 0 6.742 0.863 3.375 0.143 1957 12 6.025 2.621 0 0 6.025 2.621 3.273 2.516 1958 1 6.626 4.601 0 0 6.626 4.601 2.746 3.368 1958 2 7.836 3.112 0 0 7.836 3.112 5.787 3.710 1958 3 6.744 0.704 0 0 6.744 0.704 3.944 0.551 1958 4 9.430 0.442 0 0 9.430 0.442 6.561 0.221 1958 5 14.355 1.667 0 0 14.355 1.667 12.719 2.678 1958 6 17.058 1.634 0 0 17.058 1.634 15.502 2.725 1958 7 19.103 1.385 0 0 19.103 1.385 18.442 3.371 1958 8 17.462 0.016 0 0 17.462 0.016 16.280 1.481 1958 9 13.988 -0.934 0 0 13.988 -0.934 12.461 0.186 1958 10 10.626 0.253 0 0 10.626 0.253 8.562 0.836 1958 11 6.219 0.340 0 0 6.219 0.340 2.541 -0.691 1958 12 6.715 3.311 0 0 6.715 3.311 2.780 2.023 1959 1 4.534 2.509 0 0 4.534 2.509 0.057 0.679 1959 2 4.600 -0.124 0 0 4.600 -0.124 2.238 0.161 1959 3 6.800 0.760 0 0 6.800 0.760 3.301 -0.092 1959 4 9.042 0.054 0 0 9.042 0.054 6.142 -0.199 1959 5 11.742 -0.946 0 0 11.742 -0.946 9.603 -0.439 1959 6 14.604 -0.820 0 0 14.604 -0.820 12.691 -0.086 1959 7 17.186 -0.532 0 0 17.186 -0.532 15.760 0.689 1959 8 15.762 -1.684 0 0 15.762 -1.684 13.632 -1.167 1959 9 12.910 -2.012 1 0 NaN NaN 11.499 -0.775 1959 10 10.082 -0.291 0 0 10.082 -0.291 7.811 0.085 1959 11 6.088 0.209 0 0 6.088 0.209 2.220 -1.012 1959 12 5.053 1.649 0 0 5.053 1.649 1.759 1.002 1960 1 3.898 1.873 0 0 3.898 1.873 -0.910 -0.288 1960 2 5.352 0.628 0 0 5.352 0.628 2.986 0.909 1960 3 5.997 -0.043 0 0 5.997 -0.043 2.957 -0.436 1960 4 9.590 0.602 0 0 9.590 0.602 6.624 0.284 1960 5 11.650 -1.038 0 0 11.650 -1.038 9.111 -0.930 1960 6 14.504 -0.920 0 0 14.504 -0.920 12.027 -0.750 1960 7 17.031 -0.687 0 0 17.031 -0.687 16.219 1.148 1960 8 15.876 -1.570 0 0 15.876 -1.570 14.058 -0.741 1960 9 12.833 -2.089 1 0 NaN NaN 11.910 -0.365 1960 10 10.927 0.554 0 0 10.927 0.554 8.770 1.043 1960 11 6.853 0.974 0 0 6.853 0.974 3.255 0.023 1960 12 5.153 1.749 0 0 5.153 1.749 1.230 0.473 1961 1 6.155 4.130 0 0 6.155 4.130 2.014 2.636 1961 2 6.854 2.130 0 0 6.854 2.130 4.471 2.394 1961 3 7.269 1.229 0 0 7.269 1.229 4.233 0.841 1961 4 9.015 0.027 0 0 9.015 0.027 5.804 -0.537 1961 5 12.107 -0.581 0 0 12.107 -0.581 10.247 0.206 1961 6 15.838 0.414 0 0 15.838 0.414 14.190 1.413 1961 7 17.567 -0.151 0 0 17.567 -0.151 16.501 1.430 1961 8 17.836 0.390 0 0 17.836 0.390 16.729 1.929 1961 9 13.140 -1.782 0 0 13.140 -1.782 11.356 -0.919 1961 10 9.530 -0.843 0 0 9.530 -0.843 6.738 -0.988 1961 11 5.748 -0.131 0 0 5.748 -0.131 1.928 -1.304 1961 12 4.523 1.119 1 0 NaN NaN 0.775 0.018 1962 1 4.523 2.498 0 0 4.523 2.498 -0.282 0.340 1962 2 5.574 0.850 0 0 5.574 0.850 3.719 1.642 1962 3 5.430 -0.610 0 0 5.430 -0.610 1.925 -1.468 1962 4 9.640 0.652 0 0 9.640 0.652 6.645 0.304 1962 5 11.063 -1.625 0 0 11.063 -1.625 8.441 -1.601 1962 6 14.229 -1.195 0 0 14.229 -1.195 12.041 -0.736 1962 7 NaN NaN NaN NaN NaN NaN 14.373 -0.698 1962 8 NaN NaN NaN NaN NaN NaN 13.888 -0.911 1962 9 NaN NaN NaN NaN NaN NaN 12.793 0.518 1962 10 NaN NaN NaN NaN NaN NaN 8.812 1.085 1962 11 NaN NaN NaN NaN NaN NaN 4.732 1.500 1962 12 NaN NaN NaN NaN NaN NaN 2.911 2.154 1963 1 NaN NaN NaN NaN NaN NaN -2.692 -2.070 1963 2 NaN NaN NaN NaN NaN NaN 5.693 3.616 1963 3 NaN NaN NaN NaN NaN NaN 3.398 0.005 1963 4 NaN NaN NaN NaN NaN NaN 5.960 -0.381 1963 5 NaN NaN NaN NaN NaN NaN 10.654 0.613 1963 6 NaN NaN NaN NaN NaN NaN 12.292 -0.485