Where the diffusion (D) is equal to the product of Boltzman’s constant (k_$B$) divided by the hydrodynamic radius of the particle (R) of the particle and the shear viscosity of the solvent ($\eta$). The movement (diffusion) of these particles is described by the Stokes-Einstein equation (Eq.1). This technique operates on the principle that particles move randomly in gas or liquid i.e.
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