The total osmotic pressure can then be written as [6,14�C17]:��mi

The total osmotic pressure can then be written as [6,14�C17]:��mix+��el+��ion=RTV1(ln��1+��2+�֦�22)+��RTV0(��22��2,0?(��2��2,0)1/3)+RT��Ctot(1)In Site URL List 1|]# Equation 1, subscript 1 and 2 of the volume fractions denote the solvent and polymer phase respectively. V1 is the molar volume of the solvent, �� is the molar number of elastic active polymer chains in the gel at the reference volume fraction 2,0, V0 is the gel volume for the reference state, R is the molar gas constant, T is the absolute temperature, and �� the Flory-Huggins interaction parameter taking into account the energy of interdispersing polymer and solvent molecules.

The role of the Flory-Huggins parameter in the hydrogel swelling has been addressed in more detail elsewhere [13] and as the swelling mechanism involving changes of the parameter was utilized rather in the frame of thermo- than selectively bioresponsive hydrogels, it is not the focus here.

The total difference in molar concentration of mobile ions between the gel and the surrounding aqueous solution, ��Ctot, is given by the Donnan equilibrium and theoretical expression including molecular parameters of the network and the valence of the electrolytes are described [6].Within this framework, an understanding of the mechanism explaining how responsive gels adopt a new equilibrium swelling volume, 1/2, can be identified by considering the effect of the various parameters in Equation 1.

For instance, bioresponsive hydrogels built by Dacomitinib incorporation of an antigen-antibody pair as a physical crosslink that dissociate in the presence of its specific antigen/antibody, yields a swelling response that mainly originates from changes in the crosslink density, parameter �� in Equation 1.

Alternatively, a bioresponsive hydrogel designed by immobilization of an enzyme that catalyzes the transformation of a substrate from its non-ionic form to its ionic form (e.g., glucose oxidase) will be primarily mediated by changes in the ��Ctot term in Equation 1.Traditionally, the determination of hydrogel-swelling characteristics has been performed either optically, i.e., by imaging a piece of gel using AV-951 a light microscope, or by weighing following blotting off excess water. More accurate detection methods have been realized by incorporating the hydrogels into sensors such as conductimetric [18], liquid column length [19], or optical sensing [20�C23]. Additionally, determination of changes in swelling using dynamic light scattering methods has been reported when the size of microgel particles was appropriate [24,25].

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