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Fig. 6.8 Determination of
the inclination and
declination uncertainty
from the confidence cone
' 95
Fig. 6.9 Colatitude error,
dp , and relationship
between declination
uncertainty, • D ,and
trasversal uncertainty in the
paleopole direction, dm
direction in terms of confidence limits for the
inclination and the declination, as illustrated in
Fig. 6.8 . From simple trigonometry, we have
that:
The colatitude error dp can be calculated using
the dipole equation ( 6.40 ). It results:
dI •I D ' 95 d™
d™
2' 95
1 C 3cos 2 I
dp D
dI D
tan ' 95
cos I
2 ' 95 1 C 3cos 2
•I D ' 95 I tan •D D
(6.48)
1
D
(6.52)
where the second of these equations is usually
expressed in the approximated form:
The pair ( dp , dm ) is called oval of 95 % confi-
dence about the paleopole . In an alternative ap-
proach, each site direction is converted first into a
virtual geomagnetic pole (VGP). Then, the result-
ing set of VGPs is considered as a Fisher distribu-
tion and analyzed using the technique described
above. In this instance, conventions require that
the precision parameter and the 95 % confidence
cone be indicated by the capital symbols K and
A 95 , respectively (e.g., Van der Voo 1993 ). It can
be shown that the approximate relation between
the confidence cone A 95 and the uncertainties dp
and dm is:
' 95
cosI
•D Š
(6.49)
These uncertainties can be easily converted
into a confidence oval about the paleopole, with
mutually orthogonal semi-axes dp and dm ,as
illustrated in Fig. 6.9 . Applying the spherical law
of sines we obtain:
sin dm
sin ıD D sin p
(6.50)
A 95 p dpdm
(6.53)
Therefore,
' 95 sin p
cos I
Paleopoles
are
fundamental
quantities
dm Š •D sin p D
(6.51)
in
the
application
of
paleomagnetism
to
 
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