“…Nezu and Nakagawa (1993) proposed the equations describing relative turbulence intensity distributions in single channels for a steady and uniform 2D flow. However, the conditions of water flow after a water plant or in a compound channel are significantly different and very complex (Ali et al, 2014;Czernuszenko et al, 2007;Dargahi, 2003;Kozioł, 2013Kozioł, , 2015Kozioł and Kubrak, 2015;Kozioł et al 2016;Mazurczyk, 2007;Nezu and Nakagawa, 1993;Nikora et al, 1994;Oliveto and Comuniello, 2009;Oliveto et al, 2011;Pagliara and Palermo, 2013;Rowiński et al, 1998;Rowiński et al, 2002;Shiono and Knight, 1991;Siniscalchi et al, 2012). The turbulence generation produces fluctuations of the flow velocity associated with big vortices, and the turbulent energy is converted into an energy cascade to smaller scale eddies until it is dissipated into heat by the molecular viscosity (Nezu and Nakagawa, 1993).…”