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f
r
strike-slip
X 1
X 1
X 3
X 2
q
q
r
r
X 2
X 2
f
f
dip - slip
X 3
X 3
Figure 9.7 Double force and moment transport.
Thus, only transport in the φ-direction gives a non-null result. In Cartesian geo-
metry the double couple involved is
δ x 2 0 δ( x 2 + δ x 2 /2)
δ( x 2 δ x 2 /2)
δ x 2
e 1 sinαδ( x 1 )δ( x 3 ) lim
.
(9.69)
Each of the two forces gain small extra components
θ
∂φ δ(φ ± δφ/2)δ( r
1
2 δφ
r 0 )δ(θ θ 0 )sinα
(9.70)
before division by δ x 2
and parallel transport into the limit as δ x 2
0. Since
δ x 2 =
r 0 sinθ 0 δφ, this produces the extra term
1
r 0 sinθ 0 δφ
1
r 0 sinθ 0 δφ
φ cosθ 0 δ(φ)δ( r
r 0 )δ(θ θ 0 )sinα,
(9.71)
expressed per unit volume. Hence, co-ordinate curvature contributes the term in
double-force density
φ cot θ 0
r 0 δsinα,
(9.72)
arising from the double-couple term for strike-slip faults and illustrated in the top
left of Figure 9.7.
In the case of the double-couple force system arising from the strike-slip expres-
sion and illustrated in the upper right of Figure 9.7, the unit vectors
±
r have been
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