A novel stochastic model is proposed to characterize the adsorption kinetics of pollutants including dyes (direct red 80 and direct blue 1), fluoride ions, and cadmium ions removed by calcium pectinate (Pec-Ca), aluminum xanthanate (Xant-Al), and reed leaves, respectively. The model is based on a transformation over time following the Ornstein–Uhlenbeck stochastic process, which explicitly includes the uncertainty involved in the adsorption process. The model includes stochastic versions of the pseudo-first-order (PFO), pseudo-second-order (PSO), and pseudo-[Formula: see text]-order (PNO) models. It also allows the estimation of the adsorption parameters, including the maximum removal capacity ([Formula: see text]), the adsorption rate constant ([Formula: see text]), the reaction pseudoorder ([Formula: see text]), and the variability [Formula: see text]. The model fitted produced [Formula: see text] values similar to those of the nonstochastic versions of the PFO, PSO, and PNO models; however, the obtained values for each parameter indicate that the stochastic model better reproduces the experimental data. The [Formula: see text] values of the Pec-Ca-dye, Xant-Al-fluoride, and reed leaf-Cd+2 systems ranged from 2.0 to 9.7, 0.41 to 1.9, and 0.04 and 0.29 mg/g, respectively, whereas the values of [Formula: see text] ranged from 0.051 to 0.286, 0.743 to 75.73, and 0.756 to 8.861 (mg/g)1- n/min, respectively. These results suggest a variability in the parameters [Formula: see text] and [Formula: see text] inherent to the natures of the adsorbate and adsorbent. The obtained [Formula: see text] values ranged from 1.13 to 2.02 for the Pec-Ca-dye system, 1.0–3.5 for the Xant-Al-fluoride system, and 1.8–3.8 for the reed leaf-Cd+2 system. These ranges indicate the flexibility of the stochastic model to obtain fractional [Formula: see text] values, resulting in high [Formula: see text] values. The variability in each system was evaluated based on [Formula: see text]. The developed model is the first to describe pollutant removal kinetics based on a stochastic differential equation.
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