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4. Underwater sonar-based monitoring of the seas often involves sending ping-like signals from the sea surface to a receiving, and listening for the reflected signal s]. The sound speed underwater is a function of the static pressure P in [Pa], salinity of the water S in [parts per thousand], latitude Ψ of the location in [deg], temperature T in [deg C], and depth z in [km]. The static pressure is P-99.5(1-0.00263cos 2y)Z+0.239 where z is the depth in [km] and y is the latitude in [deg]. For the oceans, the sound speed is then determined by the relation (4.2) 1449.08+5Tro 1.33(S-35)- (4.2) 0.15225-0) +1.46105- where T is the temperature in [deg C] and S is the salinity in [parts per thousand]. (a) Consider a location with latitudew 40, temperature T-18 [°C], and water salinity S-37 [parts per thousand]. Generate a plot of the sound speed underwater for this location across the depth range of Z-(0, 3] [km. Use a sufficiently large number of points in the plot, which will be beneficial for the effort in (b). Generate this plot of underwater sound speed with positive depth in the downward y axis and sound speed in the x axis like that shown in Figure 3
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Aas (oes C) toe ctse given 十0.22922 Substituting 亿40 sfubstituting T: 18 Cs37 +1-32 c 2) e

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