Elsevier

Marine Geology

Volume 439, September 2021, 106570
Marine Geology

Research Article
Seasonal changes in sediment erodibility in a sandy carbonate environment detected from turbidity time series

https://doi.org/10.1016/j.margeo.2021.106570Get rights and content

Highlights

  • Standard deviation of turbidity can be used as a proxy for sand resuspension.

  • Sand biostabilization was detected from continuous near-bed turbidity data.

  • Annual cycle of biostabilization likely occurs in Hamelin Pool, Western Australia.

Abstract

Sediment resuspension and sediment erodibility were investigated in Hamelin Pool (Western Australia), which is one of the few modern carbonate settings where stromatolites and ooids are actively forming. For this purpose, the first time series of wave height and water turbidity were recorded at a ~2.5 m deep subtidal location in Hamelin Pool from July 2017 to March 2018. Sediment grain size analyses indicate that this environment is nearly free of mud, so the optical turbidity sensor was able to detect the intra-wave modulation of sand resuspension. This allowed us to use the standard deviation of the turbidity within a burst – as opposed to the mean turbidity – as a proxy for sand resuspension. This approach was further validated by wave tank experiments, which also helped to identify the occurrence of biofouling and discard the affected data. Although the wave regime was similar throughout the year, sand resuspension changed with seasons. Sediment erodibility, defined as the sand resuspension normalized by the bed shear stress, was higher during the Austral winter and spring, and lower in summer and autumn. This decrease in erodibility coincided with an increase in temperature and solar irradiance. These two environmental factors likely modulate the growth of benthic microbes, which in turn affects sediment dynamics. This seasonal modulation of sediment dynamics may influence additional processes, including the delivery of sand grains to stromatolites and the precipitation of aragonite around ooids and in stromatolite laminae.

Introduction

Benthic microbial growth is seasonal due to its dependence on light and temperature (MacIntyre et al., 1996; van der Wal et al., 2008; Bowlin et al., 2012; de Jonge et al., 2012; Benyoucef et al., 2014), availability of nutrients (Sundbäck and Snoeijs, 1991; Hillebrand and Sommer, 1997), and hydrodynamic disturbances such as tides and waves (Mariotti and Fagherazzi, 2012; Mariotti et al., 2014). Because benthic microbes can stabilize sediments (Yallop et al., 1994; Kornman and Deckere, 1998; Lucas et al., 2003; Le Hir et al., 2007) – a process known as biostabilization – seasonal variability in microbial growth could have an important role in modulating sedimentary processes.

The occurrence of seasonal biostabilization has been extensively studied in muddy environments by direct measurements of the critical bed shear stress. For example, some studies used the Cohesive Strength Meter (Friend et al., 2003; Tolhurst et al., 2008; De Backer et al., 2010; Waqas et al., 2020), others used the Gust Erosion Chamber (Wiberg et al., 2013; Chen et al., 2017). In temperate climates, mud biostabilization during warmer months results in low erodibility because higher temperatures favor microbial growth (Underwood and Paterson, 1993; Andersen, 2001; Wiberg et al., 2013; Schmidt et al., 2016). Yet, these field measurements provide a coarse temporal resolution and limit the ability to detect and quantify seasonal changes in biostabilization.

In muddy environment, detection of sediment resuspension from turbidity measurements is very unlikely due to practical constraints. Biostabilization decreases sediment resuspension and should lead to a lower water turbidity (Pivato et al., 2019). Therefore, measurements of turbidity (normalized by the amount of resuspension intensity, e.g., the bed shear stress) could be used to detect changes in sediment erodibility. Although possible in principle, this approach has not been successful for at least two reasons. First, turbidity time series spanning multiple seasons are difficult to obtain. Second, the detection of biostabilization through the analysis of turbidity time series is problematic in muddy environments. Indeed, not only does the amount of suspended mud depend on local resuspension, but it also on lateral advection (Hill et al., 2003). Hence, unless biostabilization occurs over very large areas, e.g., several kilometers or more, it might not be clearly reflected in the turbidity signal. Therefore, effort to relate turbidity data with mud resuspension is ineffective.

Because of its high settling velocity, sand is suspended and settles back within a single wave cycle (Trouw et al., 2000; Davies and Thorne, 2005; Williams and Bell, 2006; Murray et al., 2012), producing a strong modulation of the turbidity signal. Therefore, the use of turbidity as an indicator of biostabilization is more likely to be effective in sandy environments, given that sand responds nearly instantaneously to local hydrodynamics. In practice, however, siliciclastic sandy environments always have some small amounts of mud that dominate the turbidity signal because the optical backscatter is one order of magnitude more sensitive to mud than to sand (Conner and De Visser, 1992). In practice this limits the usefulness of turbidity as a proxy for sand dynamics. Acoustic measurements might be used to measure sand dynamics even in the presence of mud (Thorne and Hanes, 2002), but the deployment of acoustic sensors in the field is difficult over long periods and is generally shorter than few months (Christensen et al., 2019).

Carbonate-depositing environments often lack terrigenous mud, although they can occasionally contain carbonate mud (Bathurst, 1971). It is plausible that sand resuspension can be accurately detected via turbidity measurements and possibly used to identify biostabilization and track its seasonality in areas where mud is demonstrably absent. Here, this idea was tested by focusing on Hamelin Pool (Western Australia), a hypersaline coastal embayment that is demonstrably mud-poor. This site is of particular relevance because it hosts benthic microbes that enable the formation of stromatolites and other lithified microbial structures (Jahnert and Collins, 2012).

We were not aware of any previous reports of the wave characteristics in Hamelin Pool, so hourly near-bed pressure and turbidity data were recorded over nine months at one subtidal location at this site. Wave tank laboratory experiments were also used to develop a simple method to distinguish the contributions of sand and mud resuspension to the turbidity signal. Analyses of the time series from Hamelin Pool detected seasonal changes in sand erodibility and were used to infer the occurrence of biostabilization.

Section snippets

Regional setting

Hamelin Pool is a semi-arid, subtropical embayment in Shark Bay, a double bay inlet along Australia's western coastline (Fig. 1). Hamelin Pool is a unique and highly variable environment that favors extensive accumulations of discrete microbial buildups known as stromatolites and weakly-lithified to unlithified microbial sheet mats (Logan et al., 1974; Hoffman, 1976; Playford, 1980; Jahnert and Collins, 2012; Playford et al., 2013; Collins and Jahnert, 2014; Suosaari et al., 2016b; Suosaari et

Data collection

Hourly near-bed pressure and turbidity in Hamelin Pool were measured from July 2017 to March 2018 using an RBR Ltd. data logger. The pressure measured by the instruments was corrected by subtracting the atmospheric pressure. Measurements were taken at Carbla Beach, at a location ~2.5 m deep and ~100 m from the shoreline. The pressure sensor was located 60 cm from the bottom (Fig. 1). Turbidity of the water column was measured by an optical backscatter sensor (OBS, Seapoint Sensors Inc.),

Wave characteristics and the modulation of turbidity and pressure signal

The water depth during the deployment period varied from 1.7 m to 3.2 m with the mean value of 2.4 m. Most of the waves were about 0.3 m high, with a maximum of 0.7 m. The peak periods were between 2 and 4 s. Wave height was about 30% larger during the spring and summer than during the winter and autumn (Fig. 3).

Within each burst, the turbidity co-oscillated with the wave-induced pressure with a lag of 1–2 s. A representative burst signal from the data is shown in Fig. 4A. The comparison of the

Interpretation of turbidity time series: separating mud and sand contributions

The wave-induced pressure oscillations are linearly related to the wave-induced orbital velocities (Dalrymple and Dean, 1991). Based on this, we infer that the intra-wave turbidity modulation can be used as a proxy for sand resuspension and explore this further by laboratory experiments in this study. The turbidity signal acquired in Hamelin Pool recorded the cyclic resuspension and settling of sand associated with the oscillating wave velocities (Fig. 4).

Because of its optical properties, mud

Conclusions

The nine-month-long field measurements of wave height and water turbidity in Hamelin Pool (Western Australia) and laboratory experiments enabled the development of a simple procedure to estimate mud and sand resuspension from near-bed turbidity time series in a wave-dominated setting. These measurements show that the standard deviation in turbidity can be used as a proxy for sand resuspension in environments characterized by a low concentration of mud.

Field measurements show that the wave

Funding

This research did not receive any specific grant from funding agencies in the public, commercial, or not-for-profit sectors.

Data availability

The research data collected in Hamelin Pool, Western Australia is available at doi:https://doi.org/10.6073/pasta/fd29ec0634b77bec39c7a1446c7f3421

Declaration of Competing Interest

The authors declare no competing interests.

Acknowledgements

Samples were collected from Shark Bay, Australia, under a Regulation 17 license, number 08-000373-1. We acknowledge the support for field work by the Simons Foundation Collaboration for funding this work through grants to Tanja Bosak (#327126 and #344707). We thank Dave Holley, Kelsey Moore, and the Fenney family for sampling support.

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