Geology Reference
In-Depth Information
100
I 0 = +90
°
0
100
0
50
100
150
200
250
300
350
400
450
100
I 0 = +45°
0
0
50
100
150
200
250
300
350
400
450
100
100
I 0 =
45
°
0
0
50
100
150
200
250
300
350
400
450
100
100
I 0 =
90
°
0
100
0
50
100
150
200
250
300
350
400
450
1
2
2A
3
3A
4
4A
5
5A
5B
5C
5D 5E
6 6A
6B
6C
7
8
9
10
11
12
Fig. 5.12 Theoretical magnetic anomaly profiles, gener-
ated at a ridge with constant full spreading rate v D 30 mm
year 1 , originally located at 40 ı N with a paleo-strike
'
orientation with respect to the geographic North). The
magnetic signal changes according to the present day
latitude of the prisms, as evidenced by the variation with
the inclination I 0 of the ambient geomagnetic field
D 180 ı . It is assumed that the present day strike of
the prisms is “
0 ı (so that the ridge has not changed
D
100
0
0
100
50
100
150
200
250
300
350
400
450
1
2
2A
3
3A
4
4A
5
5A
5B
5C
5D 5E
6 6A
6B
6C
7
8
9
10
11
12
the prisms is “ D 35 ı (so that the ridge has not changed
orientation with respect to the geographic North). The
ambient geomagnetic field inclination is I 0 D 45 ı
Fig. 5.13 Theoretical magnetic anomaly profile, gener-
ated at a ridge with constant full spreading rate v D 30 mm
year 1 , originally located at 40 ı N with a paleo-strike
'
135 ı . It is assumed that the present day strike of
D
magnetic anomalies. The effect of ridge jumps
is to introduce gaps and duplications in the se-
quence of chrons. Figure 5.14 shows an example
of magnetization model distorted by the presence
of a ridge jump, along with the corresponding dis-
continuities in the age progression plot as a func-
tion of the distance from the ridge. The detection
of minor ridge jumps in a real magnetic profile
is not a simple task, especially when the profile
does not encompass both flanks of the spreading
axis.
Therefore, it is good practice to be cautious
when introducing a ridge jump in the block
model: very often a reinterpretation of the
anomalies allows to obtain anyway an acceptable
fit of the data.
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