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7.16 Stretching and thinning of the sediments     255
                          Table 7.3. An example of computation of β-factors
                          where thickness of the sediments are taken into
                          account. This is an alternative version of the case in
                          Table 7.2.

                          i    s i     i   w i   f i  c i  β max,i  β i
                          1      1  2200     0  2.2  35030  1.00   1.56
                          2   1800  2200   300  2.2  22515  1.56   1.11
                          3   2300  2250   550  2.1  20271  1.73   1.90
                          4  10000  2550   950  1.5  10667  3.28   1.33
                          5  15000  2560  1050  1.5  8002  4.38    −



            became stretched and thinned. A larger factor β 1 is therefore needed to make the extra
            accommodation space for these early sediments, see note 7.16.The β-factor for the last
            rift phase has become less when accounting for the sediment thickness, but the late Juras-
            sic rifting has a larger β-factor. It is also reasonable that the accommodation spaces for
            the thick Cretaceous formations are made by the Jurassic rifting. If the thick Cretaceous
            formations were to have experienced the late Cretaceous and Paleocene rift phase with a
            β-factor nearly as large as 2, then they would have been unrealistically thick prior to rifting.
              It is possible to calculate how the lithosphere develops through the geohistory once the
            β-factors have been estimated. Figure 7.36 shows the lithosphere at the beginning and
            end of the three last rift phases and at the present time. The β-factors are computed by
            equations (7.203)to(7.206) for a series of columns along the transect. We can now see
            how the crust and the basin are stretched and thinned, and how extension creates a thermal
            transient in the lithosphere. Especially, the Late Jurassic rifting creates a noticeable thermal
            transient. Figure 7.36 also indicates that the thermal transients for rifting are considerably
            reduced in the time interval between the rift phases. The sedimentary basin though the
            geohistory is shown in Figure 7.37. It shows the deposition, stretching and thinning of
            the sediments. This modeling is a mass-conservative handling of the basin through the
            rift phases (see Wangen and Faleide, 2008). The state of the basin is also shown at the
            beginning of each rift phase and at the present time.

            Note 7.16 Example: The use of equations (7.203)to(7.206) compared to the example
            in Note 7.15 demonstrates what is different with this algorithm. The two first steps are
            the same – the computation of the factors f i and the estimate (7.192) for the initial crustal
            thickness. The equations (7.203)to(7.206) are then used to make the β-factors for i = 1to
            4. These β-factors are then multiplied together to make the products β max,i , which finally
            gives the crustal thickness c i = c 0 /β max,i . There are differences in the results for these two
            versions of computing the β-factors. Table 7.3 shows that the inclusion of the sediments
            makes the first rift phase more important, and the last rift phase less important. The early
            sediments must have been thicker because they have gone through several rift phases. The
            first rift phase must therefore have been stronger to make the extra accommodation space.
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