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Microgels, such as polymeric hydrogels, are currently used as drug delivery devices (DDSs) for chemotherapeutics and/or unstable drugs. The clinical DDS DC bead® was studied with respect to loading and release, measured as relative bead-volume, of six amphiphilic molecules in a micropipette-assisted microscopy method. Theoretical models for loading and release was used to increase the mechanistic understanding of the DDS.

It was shown that equilibrium loading was independent of amphiphile concentration. The loading model showed that the rate-determining step was diffusion of the molecule from the bulk to the bead surface (‘film control’). Calculations with the developed and applied release model on the release kinetics were consistent with the observations, as the amphiphiles distribute unevenly in the bead. The rate determining step of the release was the diffusion of the amphiphile molecule through the developed amphiphile-free depletion layer. The release rate is determined by the diffusivity and the tendency for aggregation of the amphiphile where a weak tendency for aggregation (i.e. a large cac_b) lead to faster release. Salt was necessary for the release to happen, but at physiological concentrations the entry of salt was not rate-determining. This study provides valuable insights into the loading to and release from the DDS. Also, a novel release mechanism of the clinically used DDS is suggested.

We investigated the loading of an amphiphilic drug, amitriptyline hydrochloride (AMT), onto sodium polyacrylate hydrogels at low ionic strength and its release at high ionic strength. The purpose was to show how the self-assembling properties of the drug and the swelling of the gel network influenced the loading/release mechanisms and kinetics, important for the development of improved controlled-release systems for parenteral administration of amphiphilic drugs. Equilibrium studies showed that single microgels (similar to 100 mu m) in a large solution volume underwent a discrete transition between swollen and dense states at a critical drug concentration in the solution. For single macrogels in a small solution volume, the transition progressed gradually with increasing amount of added drug, with swollen and dense phases coexisting in the same gel; in a suspension of microgels, swollen and collapsed particles coexisted. Time-resolved micropipette-assisted microscopy studies showed that drug self-assemblies accumulated in a dense shell enclosing the swollen core during loading and that a dense core was surrounded by a swollen shell during release. The time evolution of the radius of single microgels was determined as functions of liquid flow rate, network size, and AMT concentration in the solution. Mass transport of AMT in the surrounding liquid, and in the dense shell, influenced the deswelling rate during loading. Mass transport in the swollen shell controlled the swelling rate during release. A steady-state kinetic model taking into account drug self-assembly, core-shell phase separation, and microgel volume changes was developed and found to be in semiquantitative agreement with the experimental loading and release data.

Polyelectrolyte microgels may undergo volume phase transition upon loading and the release of amphiphilic molecules, a process important in drug delivery. The new phase is "born" in the outermost gel layers, whereby it grows inward as a shell with a sharp boundary to the "mother" phase (core). The swelling and collapse transitions have previously been studied with microgels in large solution volumes, where they go to completion. Our hypothesis is that the boundary between core and shell is stabilized by thermodynamic factors, and thus that collapsed and swollen phases should be able to also coexist at equilibrium. We investigated the interaction between sodium polyacrylate (PA) microgel networks (diameter: 400-850 mu m) and the amphiphilic drug amitriptyline hydrochloride (AMT) in the presence of NaCl/phosphate buffer of ionic strength (I) 10 and 155 mM. We used a specially constructed microscopy cell and micromanipulators to study the size and internal morphology of single microgels equilibrated in small liquid volumes of AMT solution. To probe the distribution of AMT micelles we used the fluorescent probe rhodamine B. The amount of AMT in the microgel was determined by a spectrophotometric technique. In separate experiments we studied the binding of AMT and the distribution between different microgels in a suspension. We found that collapsed, AMT-rich, and swollen AMT-lean phases coexisted in equilibrium or as long-lived metastable states at intermediate drug loading levels. In single microgels at I = 10 mM, the collapsed phase formed after loading deviated from the core-shell configuration by forming either discrete domains near the gel boundary or a calotte shaped domain. At I = 155 mM, single microgels, initially fully collapsed, displayed a swollen shell and a collapsed core after partial release of the AMT load. Suspensions displayed a bimodal distribution of swollen and collapsed microgels. The results support the hypothesis that the boundary between collapsed and swollen phases in the same microgel is stabilized by thermodynamic factors.

Common ionisable amphiphilic drug molecules form micelles in aqueous solution. Loaded onto oppositely charged polyelectrolyte microgels they associate with the network chains to form dense complex phases. The self-assembling properties control the loading and release properties in drug delivery applications of microgel systems but little is known about the nature of the aggregates and the phase structure. In this paper, we investigated the size and organization of the self-assemblies formed by the hydrochloride salts of amitriptyline (AMT), chlorpromazine (CPZ), and doxepin (DXP) in sodium polyacrylate microgels. Small-angle X-ray scattering (SAXS) was used to determine the microstructure of drug loaded microgels in aqueous environment at ionic strengths relevant for drug loading (0.01 M) and release (0.15 M). The composition of drug loaded microgels was determined by means of a purpose built microscopy cell and UV spectroscopy measurements. Upon drug loading the microgels formed complex phases of low water content. SAXS experiments showed that the drugs formed oblate shaped or spherical micelles displaying local ordering but without long-range ordering even at very high micelle volume fractions. The local ordering resembled the packing of randomly packed hard oblates and spheres. The aggregation number of AMT varied between 10 and 49 depending on the composition. Incorporation of the uncharged base form of the drug caused a transformation of oblate shaped (aspect ratio ∼ 0.4) to spherical micelles, accompanied by an abrupt increase of the aggregation number. Variation of the ionic strength had minor effects on the aggregation number. CPZ formed oblate shape micelles (aspect ratios 0.3–0.4) with aggregation number between 9 and 30. DXP formed oblate shape micelles (aspect ratios 0.3–0.4) with aggregation numbers 10 − 11 at all studied compositions. The results provide a structural basis for, and justification of, previously assumed microstructures underlying mechanistic models of drug-microgel interactions and drug release.