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There are different ways of defining magnetic poles.
The most common understanding is that they are the positions on
the Earth's surface where the geomagnetic field is vertical. These
poles are called dip poles, and the north and south dip poles
do not have to be (and are not now) antipodal. In principle the
dip poles can be found by experiment, conducting a magnetic survey
to determine where the field is vertical.
Another definition comes from global models of the geomagnetic
field. Models of this type, such as the International Geomagnetic
Reference Field (IGRF) include an equivalent (but fictional) magnetic
dipole at the centre of the Earth in their representation of the
field. This dipole defines an axis that intersects the Earth's surface
at two antipodal points. These points are called geomagnetic
poles. The axis of the equivalent dipole is currently inclined
at about 10° to the Earth's rotation axis. The IGRF can also
be used to compute dip pole positions. These model dip poles
do not agree with the measured dip pole positions. The geomagnetic
poles and model dip poles cannot be located by direct measurement.
The locations of the model dip and geomagnetic poles are shown
in Figures 1 and 2 and are given in Table 1.
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In practice, there are many difficulties in the experimental
determination of the locations of the dip poles, not least the remoteness
and harsh climatic conditions. The main difficulty arises from the
rapidly varying magnetic fields which originate in a region of near-Earth
space called the magnetosphere. This region is defined by the pressure
of the continuous stream of charged particles from the Sun, the
so-called solar wind, on the Earth's magnetic field. Many dynamic
electrical current systems exist on the surface of, and inside the
magnetosphere and are connected to the ionised upper atmosphere
at high latitudes. As a result, the dip poles move considerable
distances over one day, tracing out approximately oval-shaped loci
on a daily basis, with large variation from one day to the next
depending on solar activity.
Another complicating factor is the presence of magnetic
material in the underlying rocks, i.e. the crustal magnetic field.
This is not included in models such as the IGRF but may be another
reason for differences between the model dip poles and measured
dip poles.
Scientists, map makers and polar explorers have an
interest in the locations of the dip and geomagnetic poles. Although
one cannot make any observations in the region of the geomagnetic
poles that might indicate their positions, these poles are arguably
of greater significance than the dip poles. This is because the
auroral ovals, which are approximately 5° latitude bands where
the spectacular aurora are likely to be seen, are centred on the
geomagnetic poles. They are usually displaced slightly to the night-side
of the geomagnetic poles and are very variable in size: bands of
greatest activity occur between 15 and 25° from the geomagnetic
poles. In relation to this, many coordinate systems used in studies
of the Earth's magnetosphere have the dipole axis as one of their
defining axes. In addition, magnetic field
reversals are defined by the flipping of the geomagnetic poles.
These ancient poles are defined by the direction of the ancient
magnetic field frozen into certain kinds of rock, and in their derivation,
make the assumption that the field is simply that of a tilted dipole
located at the Earth's centre.
Table 1: Locations of the north and south dip poles and geomagnetic poles. Locations are computed from the 11th Generation International Geomagnetic Reference Field
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North dip pole
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South dip pole
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North geomagnetic pole
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South
geomagnetic pole
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Epoch
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Latitude
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Longitude
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Latitude
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Longitude
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Latitude
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Longitude
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Latitude
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Longitude
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1900.0
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70.46
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-96.19
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-71.72
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148.32
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78.68
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-68.79
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-78.68
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111.21
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1905.0
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70.66
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-96.48
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-71.46
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148.55
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78.68
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-68.75
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-78.68
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111.25
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1910.0
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70.79
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-96.72
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-71.15
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148.64
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78.66
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-68.72
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-78.66
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111.28
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1915.0
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71.03
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-97.03
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-70.80
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148.54
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78.64
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-68.57
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-78.64
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111.43
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1920.0
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71.34
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-97.39
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-70.41
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148.20
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78.63
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-68.38
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-78.63
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111.62
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1925.0
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71.79
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-98.00
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-69.99
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147.63
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78.62
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-68.27
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-78.62
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111.73
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1930.0
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72.27
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-98.69
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-69.52
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146.79
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78.60
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-68.26
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-78.60
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111.74
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1935.0
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72.80
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-99.34
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-69.06
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145.77
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78.57
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-68.36
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-78.57
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111.64
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1940.0
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73.30
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-99.87
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-68.57
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144.60
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78.55
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-68.51
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-78.55
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111.49
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1945.0
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73.93
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-100.24
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-68.15
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144.44
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78.55
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-68.53
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-78.55
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111.47
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1950.0
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74.64
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-100.86
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-67.89
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143.55
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78.55
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-68.85
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-78.55
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111.15
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1955.0
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75.18
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-101.41
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-67.19
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141.50
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78.54
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-69.16
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-78.54
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110.84
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1960.0
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75.30
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-101.03
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-66.70
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140.23
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78.58
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-69.47
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-78.58
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110.53
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1965.0
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75.63
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-101.34
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-66.33
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139.53
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78.60
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-69.85
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-78.60
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110.15
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1970.0
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75.88
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-100.98
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-66.02
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139.40
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78.66
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-70.18
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-78.66
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109.82
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1975.0
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76.15
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-100.64
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-65.74
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139.52
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78.76
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-70.47
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-78.76
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109.53
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1980.0
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76.91
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-101.68
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-65.42
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139.34
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78.88
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-70.76
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-78.88
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109.24
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1985.0
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77.40
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-102.61
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-65.13
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139.18
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79.04
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-70.90
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-79.04
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109.10
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1990.0
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78.09
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-103.68
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-64.91
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138.90
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79.21
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-71.13
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-79.21
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108.87
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1995.0
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79.09
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-105.42
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-64.79
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138.76
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79.39
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-71.42
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-79.39
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108.58
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2000.0
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80.97
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-109.64
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-64.66
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138.30
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79.61
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-71.57
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-79.61
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108.43
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2005.0
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83.19
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-118.24
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-64.55
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137.85
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79.82
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-71.81
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-79.82
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108.19
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2010.0 |
85.01 |
-132.66 |
-64.43 |
137.32 |
80.08 |
-72.22 |
-80.08 |
107.78 |
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2015.0
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86.07
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-153.27
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-64.30
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136.74
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80.36
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-72.62
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-80.36
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107.38
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