Recently, we developed a simple, three-parameter model that consi

Recently, we developed a simple, three-parameter model that considers reversible drug-carrier interaction and first-order release of lipophilic drugs from liposomes, leading to a closed-form analytical solution [20]. Here, the model is used to analyze drug release from a variety of nanocarriers, including liposomes and polymeric nanocapsules, NPs, fibers, and Inhibitors,research,lifescience,medical hollow fibers. The study is focused on analyzing the influences of carrier composition (i.e., molecular weight, copolymer composition, additives) and property (i.e., pore size,

hydrophobicity) and external stimuli (i.e., pH, temperature) on the release kinetics of drugs. Our goal is to reveal how carrier composition and property as well as external stimuli may modulate drug-carrier interaction

and diffusion-driven Inhibitors,research,lifescience,medical release. To achieve this goal, a systematic parameter study is pursued to illustrate how each model parameter influences release kinetics. The model is then fitted to more than 60 sets of release data obtained Inhibitors,research,lifescience,medical from various delivery systems. Last, statistical analysis using bootstrapping is pursued to validate the model in selected cases. 2. Theory 2.1. Diffusion-Driven Drug Release Many drug release systems can be represented by one of the configurations illustrated in Figure 1. In this study, we consider the encapsulated drug molecules in two states: (1) the drug has been molecularly Inhibitors,research,lifescience,medical dispersed in the system and (2) drug molecules form aggregates, crystals, complexes with excipient and/or are absorbed. The latter is collectively referred as an associated drug, while the former is referred as disassociated drug molecules ready for release. Considering the reversible association/disassociation Inhibitors,research,lifescience,medical and the nonconstant concentration of a disassociated drug, the diffusion process of the molecularly dispersed drug molecules in configurations (a) and (b) in Figure 1 follows the first-order

kinetics [18]: Figure 1 Schematics of drug release from various systems, including core-shell (a–c), porous (d), and monolithic systems (e). (a) A core functions as a drug reservoir while a shell found controls release rate. (b) A special core-shell system (e.g., hollow NPs, … dmdt=d(Vc)dt=−Ak1c or dcdt=−kSc, (1) where t is time, m and c are the drug amount and average drug concentration in a carrier, V and A are the volume and surface area of the carrier, and k1 is the rate constant. Here, k1 may be defined as k1 = DK/l, where D is the diffusion coefficient of the drug within the AT13387 cost rate-controlling shell, K is the partition coefficient of the drug between the shell and the core, and l is the thickness of the shell [18]. The parameter kS = Ak1/V in the rearranged form of (1) suggests that a high surface-to-volume ratio (A/V) of nanostructured carriers enhances drug release.

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