A sound speed profile shows the speed of sound in water at different vertical levels. It has two general representations:
Table 1 [1] shows an example of the first representation; figure 1 shows the same information using the second representation.
Depth (m) | Sound speed (m/s) | Depth (m) | Sound speed (m/s) |
---|---|---|---|
0 | 1540.4 | 500 | 1517.2 |
10 | 1540.5 | 600 | 1518.2 |
20 | 1540.7 | 700 | 1519.5 |
30 | 1534.4 | 800 | 1521.0 |
50 | 1523.3 | 900 | 1522.6 |
75 | 1519.6 | 1000 | 1524.1 |
100 | 1518.5 | 1100 | 1525.7 |
125 | 1517.9 | 1200 | 1527.3 |
150 | 1517.3 | 1300 | 1529.0 |
200 | 1516.6 | 1400 | 1530.7 |
250 | 1516.5 | 1500 | 1532.4 |
300 | 1516.2 | 1750 | 1536.7 |
400 | 1516.4 | 2000 | 1541.0 |
Although given as a function of depth [note 1] , the speed of sound in the ocean does not depend solely on depth. Rather, for a given depth, the speed of sound depends on the temperature at that depth, the depth itself, and the salinity at that depth, in that order. [3]
The speed of sound in the ocean at different depths can be measured directly, e.g., by using a velocimeter, or, using measurements of temperature and salinity at different depths, it can be calculated using a number of different sound speed formulae which have been developed. Examples of such formulae include those by Wilson, [4] Chen and Millero [5] and Mackenzie. [6] Each such formulation applies within specific limits of the independent variables. [7]
From the shape of the sound speed profile in figure 1, one can see the effect of the order of importance of temperature and depth on sound speed. Near the surface, where temperatures are generally highest, the sound speed is often highest because the effect of temperature on sound speed dominates. Further down the water column, as temperature decreases in the ocean thermocline, sound speed also decreases. At a certain point, however, the effect of depth, i.e., pressure, begins to dominate, and the sound speed increases to the ocean floor. [8] Also visible in figure 1 is a common feature in sound speed profiles: the SOFAR channel. The axis of this channel is found at the depth of minimum sound speed. Sounds emitted at or near the axis of this channel propagate for very long horizontal distances, owing to the refraction of the sound back to the channel's center. [2]
Sound speed profile data are a necessary component of underwater acoustic propagation models, especially those based on ray tracing theory.
The speed of sound is the distance travelled per unit of time by a sound wave as it propagates through an elastic medium. At 20 °C (68 °F), the speed of sound in air is about 343 metres per second, or one kilometre in 2.9 s or one mile in 4.7 s. It depends strongly on temperature as well as the medium through which a sound wave is propagating. At 0 °C (32 °F), the speed of sound is about 331 m/s.
Echo sounding or depth sounding is the use of sonar for ranging, normally to determine the depth of water (bathymetry). It involves transmitting acoustic waves into water and recording the time interval between emission and return of a pulse; the resulting time of flight, along with knowledge of the speed of sound in water, allows determining the distance between sonar and target. This information is then typically used for navigation purposes or in order to obtain depths for charting purposes.
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A thermocline is a thin but distinct layer in a large body of fluid in which temperature changes more drastically with depth than it does in the layers above or below. In the ocean, the thermocline divides the upper mixed layer from the calm deep water below.
The surface layer is the layer of a turbulent fluid most affected by interaction with a solid surface or the surface separating a gas and a liquid where the characteristics of the turbulence depend on distance from the interface. Surface layers are characterized by large normal gradients of tangential velocity and large concentration gradients of any substances transported to or from the interface.
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A pycnocline is the cline or layer where the density gradient is greatest within a body of water. An ocean current is generated by the forces such as breaking waves, temperature and salinity differences, wind, Coriolis effect, and tides caused by the gravitational pull of celestial bodies. In addition, the physical properties in a pycnocline driven by density gradients also affect the flows and vertical profiles in the ocean. These changes can be connected to the transport of heat, salt, and nutrients through the ocean, and the pycnocline diffusion controls upwelling.
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In acoustics, the sound speed gradient is the rate of change of the speed of sound with distance, for example with depth in the ocean, or height in the Earth's atmosphere. A sound speed gradient leads to refraction of sound wavefronts in the direction of lower sound speed, causing the sound rays to follow a curved path. The radius of curvature of the sound path is inversely proportional to the gradient.
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For information about the CTD-rosette equipment package as a whole, see: Rosette sampler
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