# Passive acoustic measurement of flow velocity in the Straits of Florida

- Oleg A Godin
^{1}Email author, - Michael G Brown
^{2}, - Nikolay A Zabotin
^{3}, - Liudmila Y Zabotina
^{3}and - Neil J Williams
^{2}

**1**:16

https://doi.org/10.1186/s40562-014-0016-6

© Godin et al.; licensee Springer. 2014

**Received: **12 September 2014

**Accepted: **25 November 2014

**Published: **12 December 2014

## Abstract

Group speed of sound in moving fluids depends on the propagation direction, which breaks acoustic reciprocity. Acoustic nonreciprocity provides a means to measure fluid motion. Using nonreciprocity, one can measure fluid velocities that may be small compared to uncertainties in sound speed. Interferometry of diffuse acoustic noise, with receivers replacing the transceivers employed in active techniques, offers a simple, low-cost means of measuring nonreciprocity. Here, the feasibility of using passive measurements of acoustic nonreciprocity to estimate current velocity in the ocean is experimentally demonstrated for the first time. Estimates of depth-averaged flow velocity are retrieved from cross-correlations of low-frequency noise recorded in the Straits of Florida by near-bottom hydrophones separated by 5 and 10 km.

## Keywords

## Background

Measurements of velocity of oceanic currents are crucial for evaluating heat and mass transport, monitoring ocean dynamics, and understanding the ocean’s role in climate. Reciprocal transmissions of acoustic signals, i.e., sound propagation in opposite directions between two points, provide a way to measure path-averaged current velocity in the ocean with high temporal resolution, on a large scale, and over extended periods of time [1]-[10]. This approach is based on measurements of acoustic nonreciprocity, which is defined as differences between travel times or other acoustic quantities corresponding to sound propagation in opposite directions between two points. Acoustic nonreciprocity, which vanishes in motionless media, is a direct, sensitive measure of fluid motion, and is insensitive to uncertainties in the sound speed field and geometry of the experiment [4],[5],[11].

The use of active reciprocal transmissions for ocean remote sensing applications is limited by capital and operational costs associated with low-frequency acoustic sources as well as concerns about potential impacts of transmissions on marine life. Wave interferometry [12] and, in particular, underwater acoustic noise interferometry [13]-[17] offers a means to perform passive remote sensing by replacing probing signals generated by a dedicated source with two-point cross-correlations of diffuse ambient noise. Theory [18],[19] predicts that the cross-correlation function of diffuse noise measured at two locations in a generic inhomogeneous moving medium results in approximations to Green’s functions describing sound propagation in opposite directions between the two measurement points; positive and negative lags correspond to propagation in opposite directions [18]-[20]. Thus, two-point correlation functions allow one to quantify flow-induced acoustic nonreciprocity. Recently, passive measurements of acoustic nonreciprocity and wind velocity were experimentally demonstrated in atmospheric acoustics using interferometry of traffic noise [20].

In this paper, we use the data obtained in a noise interferometry experiment [17] in the Straits of Florida to investigate the feasibility of passive remote sensing of currents in the ocean. We present the first experimental demonstration that acoustic nonreciprocity induced by oceanic currents can be measured by noise interferometry and that the current velocity can be retrieved from the acoustic noise cross-correlations.

## Methods

^{−2}. Horizontal separations of the instruments were 5.01, 9.76, and 14.76 km for the 1–2, 2–3, and 1–3 instrument pairs, respectively. The three instruments approximately fell on a straight line with 1 northernmost and 3 southernmost. Each system had a hydrophone, electronics, and batteries contained in an aluminum housing on a short, taut mooring, with the hydrophone located 5 m off the seafloor. The electronics and recording components were based on units commercially available from Loggerhead Instruments, but the default system clock was replaced with a more accurate crystal oscillator. The nominal clock drift was 10

^{−8}, or about 1 ms/day.

The instruments were deployed on December 12–13, 2012 and retrieved three months later. Because of an electronics malfunction in one of the instruments on the seventh post-deployment day, only about six days of continuous, simultaneous records by all three systems are available. Those six days of data are used in this paper to calculate cross-correlations of acoustic noise between various hydrophone pairs. CTD (conductivity, temperature, depth) casts were performed on the deployment and recovery cruises. Temperature variations with depth and sound speed gradients were rather weak in December 2012, with the sound speed *c* = 1537.4 ± 2.4 m/s throughout the water column. During the experiment, tides with a total range of about 1 m were recorded on a tide gauge at Key Biscayne, 68–81 km from the instruments.

Ship-based ADCP (acoustic Doppler current profiler) measurements were made on the deployment cruise using a dual frequency (600 kHz and 75 kHz) system; see Figure 1. As shown in the figure, the depths covered by these instruments are approximately 2–10 m and 10–70 m, respectively. The 70 m lower limit is imposed by the sidelobe structure of the transmitted 75 kHz beam coupled with reflections off the bottom at 100 m. The time intervals during which the ship was in proximity to our instruments are marked on the figure. At those times/locations the depth-averaged eastward and northward current components are approximately 0.4 m/s and 0.6 m/s, respectively, corresponding to an average current speed of 0.7 m/s, directed approximately 55 degrees north of east. This direction roughly coincides with the orientation (instrument 3 to instrument 1) of our array. Currents in the lower 30 m of the water column are presumably lower, but we have no quantitative estimate of those currents, and we have also have no information on the post-deployment temporal evolution of currents at any depth.

*r*= 5 km and at even lower frequencies at longer ranges [17]. In this paper, we focus on the 20–50 Hz band, where coherence loss caused by tidal fluctuations is moderate and does not prevent emergence of deterministic features from noise cross-correlations (Figure 2). In this band the frequency response of the hydrophones is flat, and the acoustic field is less sensitive to seafloor structure than the field at lower frequencies.

Clock stability is a key requirement in both active and passive ocean remote sensing as a sub-millisecond accuracy is necessary for measurements of *O*(1) m/s flow velocities and sound speed variations. In our experiment, the three instrument clocks were synchronized prior to deployment by simultaneously transmitting a pulse to all three instruments. (A post-recovery synchronization pulse was also employed, but, because of the aforementioned electronics malfunction, could not be used.) In a different deployment of the same instruments in the Florida Straits in September-October 2013 relative clock drifts obtained from the pre-deployment and post-recovery clock synchronization were 1.189 ms/day for the 1–2 instrument pair and −0.774 ms/day for the 2–3 instrument pair. Acoustic data obtained in the September-October 2013 experiment will not be discussed in this paper.

To evaluate cross-correlations of underwater noise, measurements of pressure fluctuations on each instrument were split into 625 s segments. Statistical averaging was approximated by averaging over a large number of data segments. For each hydrophone, 4.55% of data segments with the highest average noise level were discarded to suppress contributions of strong, localized, transient sources. (For a random variable with a Gaussian distribution, this corresponds to discarding the outliers, which exceed the mean by more than two standard deviations). Power spectra of the recorded noise have multiple sharp peaks, which is typical of shipping noise. To suppress the effects of a rapid variation of the noise power spectrum with frequency, we followed Godin et al. [21] and evaluated the noise cross-correlation as a Fourier transform of the coherence function, rather than the cross-spectrum. This is equivalent to pre-whitening and normalization of the noise spectrum in each data segment and can be viewed as a frequency-domain counterpart of “one-bit correlation” in the time domain [12], which has been extensively utilized in noise interferometry.

## Results and discussion

Figure 2 illustrates the gradual emergence of deterministic features from cross-correlations of acoustic noise with increasing averaging time. For the 1–2 instrument pair, coherent features at positive and negative time lags emerge after less than 18 hours of noise averaging. Generally, the signal-to-noise ratio (SNR), i.e., the amplitude contrast between the coherent features (with time lags between about 3.2 s and 3.7 s) and the spurious arrivals, increases with increasing averaging time. Small differences in amplitude and time shifts of the fine structure of the correlation functions at positive and negative lag are seen. The amplitude differences can be attributed to noise anisotropy. Comparison of *C*_{12} with the cross-correlation functions *C*_{23} and *C*_{13} for the 2–3 and 1–3 instrument pairs shows that, with increasing instrument separation, SNR decreases and longer averaging times become necessary.

*C*

_{ ij }are approximations to the Green’s functions describing propagation from location

*i*to location

*j*[location

*j*to location

*i*]. In our data

*C*

_{ ij }(

*t*) and

*C*

_{ ij }(−

*t*) are nearly identical (owing to an approximately diffuse distribution of noise sources), apart from a time shift. In the following we estimate the time shift between

*C*

_{ ij }(

*t*) and

*C*

_{ ij }(−

*t*) by identifying the location of the peak in the cross-correlation function between

*C*

_{ ij }(

*t*) and

*C*

_{ ij }(−

*t*). (It is important not to confuse this secondary correlation function calculation with the process by which the

*C*

_{ ij }were estimated -- cross-correlating records of ambient noise measured at locations

*i*and

*j*.) The time shifts between

*C*

_{ ij }(

*t*) and

*C*

_{ ij }(−

*t*) that we seek to estimate are due to a combination of acoustic travel time nonreciprocity and clock errors. To separate these effects, we exploit the properties that, over time scales that are not too long, clock errors grow linearly, while the nonreciprocity contribution is constant. The 6 day data set was divided into four consecutive segments of equal 1.5 day duration. For each segment, we evaluated the noise cross-correlation functions

*C*

_{ ij }and calculated the normalized correlation function

*K*

_{ ij }of the measured noise cross-correlations

*C*

_{ ij }(

*t*) at the positive and negative time lags

*t*:

*C*

_{13}). The integration interval (

*t*

_{1},

*t*

_{2}) in Eq. (1) was chosen to contain the coherent features in the respective

*C*

_{ ij }(

*t*). Peak values of

*K*

_{ ij }characterize the degree of similarity between

*C*

_{ ij }at positive and negative time delays. For perfectly diffuse noise, infinite averaging time, and weak currents the peak value equals unity. In addition to main peaks, each

*K*

_{ ij }(

*τ*) has additional peaks due to finite noise bandwidth. The position of each main peak gives an estimate of the time shift of the corresponding data segment.

The best-fitting lines to our two sets of four time shift estimates are shown in Figure 4c. The slopes of those lines, caused by clocks drifting at a near-constant rate, are 0.917 ms/day and −0.490 ms/day for the 1–2 and 2–3 instrument pairs, respectively. The zero-time (clock synchronization time) intercepts of those lines, corresponding to current-induced time shifts, are τ_{12} = −2.00 ms and τ_{23} = −4.10 ms. We emphasize here that, although one cannot distinguish between current-induced and clock-drift-induced contributions to a time shift using an isolated estimate, the only sensible interpretation of the linear trends shown in Figure 4c is that over the 6 day measurement period the clocks were drifting at a near-constant rate and the current was very nearly steady. (It would take a remarkable coincidence for two nonlinear trends to effectively cancel each other.) Additional support for the assumptions underlying our interpretation of Figure 4c is described below.

Special cases of the procedure that we have described to retrieve clock drift and travel time nonreciprocity from ambient noise cross-correlations have been previously employed in seismology [22]-[24], where there was no nonreciprocity, and in atmospheric acoustics [20], where there was no clock drift. To test our method of estimating time shifts, we applied it to the ambient noise recorded between synchronization pulses in the laboratory experiment on clock stability. The relative drifts of clocks measured by matching the leading fronts of the synchronization pulses and from cross-correlations of ambient noise were found to agree within 0.1% (Figures 3a, b). Our relative clock drift estimates based on Figure 4c are of the same magnitude as the clock drifts measured (i) in September-October 2013 using pre-deployment and post-recovery clock synchronization pulses, and (ii) in the May 2014 laboratory experiment. The reported values of the relative clock drifts, including our estimates based on Figure 4c, are consistent with the clock drifts being nearly constant over time periods of the order of a few weeks and slowly varying over periods of the order of a few months.

*C*

_{12}and

*C*

_{23}, computed after having corrected for estimated clock drift and averaging over the entire 6-day data set, are shown in Figures 5a and b. In those correlation functions clock-drift-induced blurring is eliminated, SNR is higher than in the 1.5 day averages, and the nonreciprocity time shift is isolated. The corresponding functions

*K*

_{12}(

*τ*) and

*K*

_{23}(

*τ*) shown in Figure 5c have peak values of 0.954 and 0.763, respectively; the corresponding time shifts,

*τ*

_{12}= −2.00 ms and

*τ*

_{23}= −4.10 ms, are in very good agreement (coincidentally identical here) with the estimates of the same quantities based on Figure 4c. As reflected by the peak values of

*K*

_{12}and

*K*

_{23}, the uncertainty of the

*τ*

_{23}estimate is greater than that of the

*τ*

_{12}estimate. This difference is attributable to greater distance between the 2–3 instrument pair, and the correspondingly lower SNR of the

*C*

_{23}correlation function. In spite of the greater uncertainty of the

*τ*

_{23}estimate, note that the ratio of the distances between the 2–3 and 1–2 instrument pairs is 9.76 km/5.01 km = 1.95, which is in good agreement with the ratio τ

_{23}/τ

_{12}= 2.05 and the assumption of a constant current along the 100 m isobath.

Under conditions of the experiment, the acoustic Green’s function for propagation between the instruments is composed of multiple surface- and bottom-reflected ray arrivals, and, in the 20–50 Hz frequency band that we consider, neither ray nor mode arrivals can be resolved in the time domain [17]. On an individual eigenray connecting points (0, 0, *z*_{
A
}) and (*r*, 0, *z*_{
B
}), the difference between acoustic travel times from *B* to *A* and *A* to *B* is [4]$\delta t=2{\displaystyle \underset{0}{\overset{r}{\int}}{u}_{x}{c}^{-2}dx}$ up to the terms of the third order in the ratio of the flow velocity **u** = (*u*_{
x
}, *u*_{
y
}, 0) and the sound speed *c*. The integration is along the eigenray traced in the absence of currents. By considering the straight segments of the eigenray between reflections, in a range-independent waveguide with a constant sound speed and depth-dependent flow velocity **u**(*z*), the travel time nonreciprocity equation simplifies to $\delta t=2{c}^{-2}rU,\phantom{\rule{1em}{0ex}}U={H}^{-1}{\displaystyle \underset{0}{\overset{H}{\int}}{u}_{x}\left(z\right)dz}\text{,}$ when both points are located on the seafloor. Here *H* is the ocean depth, the ocean surface is at *z* = 0, and *U* is the depth-averaged component of the flow velocity in the direction from the point *A* to point *B*. Note that the travel time nonreciprocity does not depend on the number of surface reflections and is the same for each eigenray. Within this approximation waveforms are the same for sound propagation with and against the flow.

Using the estimated value of *τ*_{12} for *δt*, we find *U* = −0.47 m/s. The result obtained from our estimate of *τ*_{23} is 5% higher. The minus sign indicates that the flow is from the instrument 2 to instrument 1, i.e., towards the northeast. This estimate is slightly lower than the deployment cruise ADCP-based estimate, 0.7 m/s, of the average current in the upper 70 m. We consider this agreement to be good, given that currents in the lower 30 m are expected to be lower than currents in the upper 70 m. A northeastward depth-averaged current of ~0.5 m/s near the 100 m isobath can be attributed to a meander [25],[26] of the Florida current (L. K. Shay, personal communication).

The dominant sources of errors in the *U* measurement are errors associated with estimation of *τ*_{12}. These were estimated, as in active tomography (see, e.g., p. 197 in [4]), from the acoustic bandwidth and SNR in the noise cross-correlation function *C*_{12} (Figure 5a), and were found to be ~0.1 ms. As mentioned above, the accuracy of the clock drift removal assuming linear drift over 1 week is also within 0.1 ms. The expected time shift measurement error is thus approximately (0.1^{2} + 0.1^{2})^{1/2} ms, corresponding to a current estimation error of ~7%.

## Conclusion

Using simple, single-hydrophone recording systems, we have demonstrated experimentally the feasibility of making passive measurements of acoustic nonreciprocity in the ocean at scales large compared to the ocean depth. Interferometry of low-frequency ambient and shipping noise is shown to provide sub-millisecond accuracy in measurements of the acoustic travel time nonreciprocity and to give robust estimates of the depth-averaged flow velocity, despite very limited *a priori* information about the noise sources and sound propagation conditions. Further research is necessary to improve accuracy and extend the measurements to longer ranges. Anticipated future development of inexpensive low-power atomic clocks should lead to improved accuracy while simplifying the analysis. It is expected that wider frequency bands of ambient noise will prove useful for passive measurements on refracted acoustic paths and in less dynamic environments representative of the deep ocean. Flow velocity measurements complement previously demonstrated [14] passive measurements of the sound speed profile (and, therefore, water temperature) and open the possibility of using acoustic noise interferometry to measure heat fluxes in the ocean.

## Declarations

### Acknowledgments

Data processing was performed on the Janus supercomputer, which is supported by the National Science Foundation (award number CNS-0821794) and the University of Colorado Boulder. We thank Jules Hummon of the University of Hawaii Data Acquisition System ADCP group for assistance with processing the ADCP data and preparation of Figure 1b. Constructive comments by two anonymous referees helped to improve presentation. This work was supported, in part, by the National Science Foundation, grants OCE1129860 and OCE1129524, NAVAIR, award N68335-12-C-0104, and the Office of Naval Research, grant N00014-12-10182.

## Authors’ Affiliations

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## Copyright

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