“…Therefore, field automated surrogates for SSC measurement are required to overcome these limitations. Among these automated surrogates are optical turbidity meter–based methods (Campbell et al., 2005; Downing, 1996; Gentile et al., 2010; Gillett & Marchiori, 2019; Khairi et al., 2015; Matos et al., 2019; Navratil et al., 2011; Omar & MatJafri, 2009; Pallarès et al., 2021), acoustic transmission or backscattering methods (Huang et al., 2018; Li et al., 2018; Moore et al., 2013; Thorne & Hanes, 2002; Thorne & Meral, 2008; Thorne et al., 1991; Topping et al., 2007; Wenjie et al., 2019), focused beam reflectance measurement methods (which involve the use of a laser focused on a focal plane and retrieval of the backscattering data of a sediment particle) (Heath et al., 2002; Jeldres et al., 2020; Law & Bale, 1998), laser diffraction methods (Agrawal & Pottsmith, 1994; Blott et al., 2004; Czuba et al., 2015), nuclear methods (which involve the use of a gamma radioactive source to measure the density of turbid water) (Berke & Rakoczi, 1981; McHenry et al., 1968), spectral reflectance methods (which involve the use of a remote sensing technique to capture the increased volume reflectance of water areas) (Choubey, 1994; Han, 1997; Qu, 2014; Sváb et al., 2005), and differential pressure methods (which involve the measurement of differential pressure from two transmitters at different water depths) (Hsu & Cai, 2010; Lewis & Rasmussen, 1996; Petrovic et al., 2016; Sumi et al., 2002; Tollner et al., 2005).…”