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7.12 Lithospheric extension and decompression melting  231

                                  0
                                                    ΔT
                                 20                   1  z 1
                                                        z 2
                                 40             melt
                               depth [km]   60          z    liquidus



                                 80                      3

                                100                    solidus

                                120
                                   0     500    1000   1500   2000
                                            temperature [°C]
            Figure 7.22. Melt is generated when the geotherm crosses the solidus.

            rocks do not melt completely, only partially, after the solidus is crossed. The temperature
            must increase by several hundred degrees more before the rock melts completely. The
            temperature (and pressure) where the last fraction of the rock melts is the liquidus.We
            notice that melt is not generated because the rock becomes heated, but because it’s brought
            upwards. The rock is slightly cooled when it moves upwards, and it is the decreasing pres-
            sure from decreasing depth that causes the rock to cross the solidus. Melting is for this
            reason called pressure release melting or decompression melting. The solidus and the liq-
            uidus are now approximated by linear functions of depth as shown in Figure 7.22, and they
            are written as
                             T s (z) = T s,0 + Az and T l (z) = T l,0 + Az.   (7.127)

            The temperature of the liquidus and the solidus at surface conditions are T s,0 and T l,0 ,
            respectively, and the steepness A is a constant parameter. Knowledge of the solidus allows
            us to find the minimum amount of stretching required for melting to start, which is when
            the geotherm touches the solidus. We assume that the McKenzie model based on rapid
            and uniform stretching provides a good approximation for the geotherm. The temperature
            is assumed unchanged for a volume of mantle that follows the flow of the asthenosphere
            when it moves upwards during extension. Notes 7.11 and 7.12 look at this assumption
            by estimating the temperature change along (adiabatic) geotherms when compressibility
            and melting are accounted for. Melting starts when the temperature T a at the base of the
            lithosphere is brought up to the depth where it crosses the solidus
                                                a
                                        T s,0 + A   = T a                     (7.128)
                                               β min

            and where a is the thickness of the lithosphere at steady state conditions. The minimum
            amount of stretching becomes
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