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In solving mass transfer problems governed by diffusion, the formulation of appropriate boundary and initial conditions is as critical as the differential equation itself. These conditions provide the necessary constraints for obtaining unique and physically meaningful solutions to diffusion equations. When the solute concentration is a function of both space and time, such as in transient diffusion processes, the problem becomes a partial differential equation (PDE) that cannot be solved without specifying the concentration throughout the spatial domain at some initial time. This requirement leads us to the concept of the initial condition (IC). The initial condition defines the spatial distribution of solute concentration at time t = 0. In many practical situations, the initial condition is uniform, reflecting a system at rest before the onset of diffusion. Along with the initial condition, we must impose boundary conditions (BCs) to describe the behavior of the solute at the edges of the domain in space. These are derived from the physical interactions at the boundaries and are essential to completely define the problem. Several common types of boundary conditions arise in mass transfer, each corresponding to a distinct physical scenario.