Page 332 - Physical Principles of Sedimentary Basin Analysis
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314                        Flexure of the lithosphere

                                      10

                                           F = 0.25F u
                                       5

                                    log 10 (t 0 ) [Ma]   0  F = 2.5F u





                                      −5


                                     −10
                                        3     4     5     6     7     8
                                                   log (λ) [m]
                                                     10
                 Figure 9.16. The characteristic time t 0 plotted as a function of the wavelength for two different
                 compressive forces. (See the text for details.)


                 position than x = 0 shows a similar behavior of the Fourier coefficients.) The first Fourier
                 coefficient is a 1 ≈ 3500 m, but the first unstable coefficient is only a 15 = 1.3 m. The initial
                 deflection is almost dying out because the unstable Fourier coefficients are small, and they
                 need a long time to grow large.
                   If the compressive force is multiplied by 10 we get the deflections shown in Figure 9.15b.
                 The first unstable Fourier coefficient is now a 5 = 660 m. The deflection is not dying out in
                 this case, because of the large unstable Fourier coefficients that are growing. The unit time
                 is t u = 1.8 Ma because the force is now ten times larger than in Figure 9.15a.
                   In nature there are always small deflections with small wavelengths. These deflections
                 will grow large under compression after a sufficiently long time, assuming that the plate
                 behaves viscously. The condition for the deflections to grow large is t 
 t 0 , where t 0 =
                 t 0 (λ) is the characteristic time for the wavelength λ. Figure 9.16 shows the characteristic
                 time |t 0 | as a function of the wavelength λ for the two cases in Figure 9.15. The minimum
                 of t 0 in the regime λ<λ s is marked with dashed lines (see Exercise 9.17).
                 Exercise 9.16 Show that the time-dependent deflection (9.142) is a solution of
                 equation (9.140) for a viscous plate when the initial deflection of the plate is w(x) =
                 w 0 cos(kx).
                 Solution: The equation is solved by trying a solution of the same form as the initial
                 deflection,
                                           w(x, t) = Y(t) cos(kx).                 (9.149)

                 This method of solving a partial differential equation is called separation of variables
                 because the solution is written as a product of a function of only t and another function of
                 only x. When function (9.149) is inserted into equation (9.140) we get
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