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Figure 17.1: Multiple reflections from transmitter to receiver. where s ( t ) is the transmitted signal, an(t) the attenuation on the nth path (which may is be time-varying), t n ( t ) is the delay on the nth path, and e-jzrfcrn@)represents the phase change in the carrier with frequency fc due to the delay, with phase & ( t ) = 2 r t t n ( t )fc. a n ( t ) , ( t ) , and t n ( t ) can be considered as random processes. The noise n ( t ) is a complex, 6% stationary, zero-mean Gaussian random process with independent real and imaginary parts = and E[n(t)n*(s)] NoS(t - s). In the limit, if the number of reflectors can be regarded as existing over a continuum (e.g., for signals reflecting off the ionosphere), the received signal can be modeled as





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ridge, it becomes removed from underlying heat sources and cools This cooling has two effects First, the lithosphere contracts and increases in density Second, because the lithosphere asthenosphere boundary is controlled by temperature (Section 212), the cooling causes the lithosphere to increase in thickness away from the mid-ocean ridge This latter phenomenon has been con rmed by lithosphere thickness estimates derived from surface wave dispersion studies in the Paci c Ocean, which indicate that the thickness increases from only a few kilometers at the ridge crest to 30 km at 5 Ma age and 100 km at 50 Ma (Forsyth, 1977) The cooling and contraction of the lithosphere cause a progressive increase in the depth to the top of the lithosphere away from the ridge (Sclater & Francheteau, 1970), accompanied by a decrease in heat ow.

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It follows that the width of a ridge depends upon the spreading rate, and so provides an explanation for the relative widths of the rapidly spreading East Paci c Rise and more slowly spreading Mid-Atlantic Ridge Parsons & Sclater (1977) determined the nature of the age depth relationships of oceanic lithosphere, and suggested that the depth d (meters) is related to age t (Ma) by: d = 2500 + 350t1/2 It was found, however, that this relationship only holds for oceanic lithosphere younger than 70 Ma For older lithosphere the relationship indicates a more gradual increase of depth with age In order to explain this, Parsons & McKenzie (1978) suggested a model in which the cooling layer comprises two units rather than the single unit implied by Parsons & Sclater (1977).

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In this model the upper unit, through which heat moves by conduction, is mechanically rigid, and the lower unit is a viscous thermal boundary layer As the lithosphere travels away from a spreading center, both units thicken and provide the relationship depth proportional to the square root of age described above However, the lower unit eventually thickens to the point at which it becomes unstable and starts to convect This brings extra heat to the base of the upper layer and prevents it thickening at the same rate They suggested that the age depth relationship for oceanic lithosphere older than 70 Ma is then given by: d = 6400 3200exp( t/628).

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