here, t 0 denotes the characteristic relaxation time, related to the time taken by the droplet to reach equilibrium after being disturbed by the adsorbed amphiphiles. n d,0 is the initial number of H 2 O in the droplet, and β is the exponent of the stretched exponential, which ranges between 0 and 1 (0 < β ≤ 1). The average droplet disintegration time using this methodology is, τ ′ = βt 0 (Figure ). In the w/t/o system, we computed the average droplet disintegration rates, relaxation times, and β of the stretched component as a function of the system temperature for the first 10 ns of droplet disintegration. We found that the disintegration of the nanodroplets becomes faster and the respective rates r, obtained using the formula (n(t + ∆t) -n(t))/∆t, where n(t) and n(t + ∆t) are the number of water in the intact nanodroplet at time t and t + ∆t, respectively, increase linearly with temperature, from -0.82