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1.1 Expressions of Earth’s Heat Sources  9
                         differences in subsurface temperatures may be negligible. These subtle effects
                         are illustrated in Figure 1.4, where two scenarios of heat refraction effects are
                         illustrated. The objective here is to show that high surface heat flow variations
                         do not necessarily correlate with large subsurface temperature differences since
                         geometrical effects have to be accounted for. Indeed, above a large aspect-ratio
                         insulating body, isotherms are uplifted so that surface heat flow above the anomaly
                         center corresponds to the equilibrium one. On the contrary, isotherms cannot be
                         distorted for a small aspect-ratio conducting body but the resulting surface heat
                         flow is enhanced.
                           In sedimentary basins, presence of salt may also induce heat refraction effects
                         since thermal conductivity of halite may be four times greater than surrounding
                         sediments (e.g., 1.5 W m −1  K −1  for sediments and around 6–7 W m −1  K −1  for rock
                         salt and halite, according to Clauser, 2006). Consequently, temperature gradient
                         within a thick evaporitic layer may thus be decreased by a factor of 4, leading to a
                         cooling effect of several tens of degrees centigrade for a 2–3-km-thick layer.

                                 A                 B
                           0
                             100 °C
                           4
                           8  200
                           Depth (km)  400                High heat producing  −3
                             300
                                                          granite: A = 10–20 µW m
                             500
                             600 °C
                          35
                          (a)            Mantle heat flow = 25 mW m −2
                            700
                                       A, Q = 10 µW m −3
                            600
                                       B, Q = 10 µW m −3
                            500
                           Temperature (°C)  400  B, Q = 20 µW m −3


                            300

                            200
                                                   ∆T = 42 °C  ∆T = 90 °C
                            100
                              0
                               0     5     10    15    20    25    30    35
                          (b)                    Depth (km)
                         Figure 1.5  Two-dimensional effect of a high heat producing
                         granite on temperature field (a) and geotherms (b). Here, a
                         fixed mantle heat flow of 25 mW m −2  is imposed, as well as
                         an averaged thermal conductivity of 3 W m  −1  K −1  and a bulk
                                                 −3
                         crustal heat production of 1 µWm .
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