Elastomeric Gel Research Articles

Instability and dewetting of ultrathin solid viscoelastic films on homogeneous and heterogeneous substrates

Instability and dewetting engendered by the van der Waals force in soft thin (<100 nm) linear viscoelastic solid (e.g., elastomeric gel) films on uniform and patterned surfaces are explored. Linear stability analysis shows that, although the elasticity of the film controls the onset of instability and the corresponding critical wavelength, the dominant length-scale remains invariant with the elastic modulus of the film. The unstable modes are found to be long-wave, for which a nonlinear long-wave analysis and simulations are performed to uncover the dynamics and morphology of dewetting. The stored elastic energy slows down the temporal growth of instability significantly. The simulations also show that a thermodynamically stable film with zero-frequency elasticity can be made unstable in the presence of physico-chemical defects on the substrate and can follow an entirely different pathway with far fewer holes as compared to the viscous films. Further, the elastic restoring force can retard the growth of a depression adjacent to the hole-rim and thus suppress the formation of satellite holes bordering the primary holes. These findings are in contrast to the dewetting of viscoelastic liquid films where nonzero frequency elasticity accelerates the film rupture and promotes the secondary instabilities. Thus, the zero-frequency elasticity can play a major role in imposing a better-defined long-range order to the dewetted structures by arresting the secondary instabilities.

A coupled theory of fluid permeation and large deformations for elastomeric materials

An elastomeric gel is a cross-linked polymer network swollen with a solvent (fluid). A continuum-mechanical theory to describe the various coupled aspects of fluid permeation and large deformations (e.g., swelling and squeezing) of elastomeric gels is formulated. The basic mechanical force balance laws and the balance law for the fluid content are reviewed, and the constitutive theory that we develop is consistent with modern treatments of continuum thermodynamics, and material frame-indifference. In discussing special constitutive equations we limit our attention to isotropic materials, and consider a model for the free energy based on a Flory–Huggins model for the free energy change due to mixing of the fluid with the polymer network, coupled with a non-Gaussian statistical–mechanical model for the change in configurational entropy—a model which accounts for the limited extensibility of polymer chains. As representative examples of application of the theory, we study (a) three-dimensional swelling-equilibrium of an elastomeric gel in an unconstrained, stress-free state; and (b) the following one-dimensional transient problems: (i) free-swelling of a gel; (ii) consolidation of an already swollen gel; and (iii) pressure-difference-driven diffusion of organic solvents across elastomeric membranes.

Quartz Crystal Microbalance Studies of the Contact between Soft, Viscoelastic Solids

Mechanical contact between a viscoelastic lens and a viscoelastic film has been probed by means of a quartz crystal microbalance operated in the impedance analysis mode. The frequency shift induced by the formation of the contact decreases with increasing film thickness because of the finite penetration depth of the acoustic shear wave. The dependence of frequency and bandwidth on film thickness and contact area is described within a sheet-contact model, which can be employed to quantitatively analyze mechanical contact in a wide range of materials problems. The model was tested by bringing a quartz crystal coated with an elastomeric gel into contact with a hemispherical cap of a similar gel. Both gels consisted of the thermoreversible gel Kraton G swollen in mineral oil. The experiments support the model well.

Acrylamide‐agarose copolymers: Improved resolution of high molecular mass proteins in two‐dimensional gel electrophoresis

A method was developed in order to analyse high molecular mass proteins by two-dimensional (2-D) electrophoresis using a copolymer of acrylamide and allyl agarose instead of Bis cross-linked polyacrylamide (PA) gels in sodium dodecyl sulphate-electrophoresis. In this work, the matrix composition was optimised to improve the resolution of proteins larger than 200 kDa. The new gel type does not entrap large proteins and protein complexes at the application site. Mechanical properties were investigated through rheological measurements, which suggested the formation of a highly entangled elastomeric soft gel. A high 2-D resolution of proteins, extracted from membranes of red blood cells, was obtained in these gels. An example of tryptic digestion, peptide extraction and matrix-assisted laser desorption/ionisation-time of flight mass spectrometry was reported. The results demonstrate that the new gel is fully compatible with mass spectrometry protein analysis.

Quantification of prosthetic outcomes: Elastomeric gel liner with locking pin suspension versus polyethylene foam liner with neoprene sleeve suspension

For this randomized crossover trial, we compared two common transtibial socket suspension systems: the Alpha liner with distal locking pin and the Pe-Lite liner with neoprene suspension sleeve. Our original hypotheses asserted that increased ambulatory activity, wear time, comfort, and satisfaction would be found with the elastomeric suspension system. Thirteen subjects completed the study. Following 2.5-month accommodation to each condition, ambulatory activity was recorded (steps/minute for 2 weeks), and subjects completed three questionnaires specific to prosthesis use and pain: the Prosthesis Evaluation Questionnaire (PEQ), a Brief Pain Inventory (BPI) excerpt, and the Socket Comfort Score (SCS). Upon completion, subjects selected their favored system for continued use. Ten subjects preferred the Pe-Lite and three the Alpha. Subjects spent 82% more time wearing the Pe-Lite and took 83% more steps per day. Ambulatory intensity distribution did not differ between systems. No statistically significant differences were found in questionnaire results. Subject feedback for each system was both positive and negative.

Polyelectrolyte‐in‐Ionic‐Liquid Electrolytes

AbstractNovel polymer electrolyte materials based on a polyelectrolyte‐in‐ionic‐liquid principle are described. A combination of a lithium 2‐acrylamido‐2‐methyl‐1‐propanesulfonic acid (AMPSLi) and N,N′‐dimethylacrylamide (DMMA) are miscible with the ionic liquid, 1‐ethyl‐3‐methylimidazolium dicyanamide (EMIDCA). EMIDCA has remarkably high conductivity (≥ 2 · 10−2 S · cm−1) at room temperature and acts as a good solvating medium for the polyelectrolyte. At compositions of AMPSLi less than or equal to 75 mol‐% in the copolymer (P(AMPSLi‐co‐DMAA)), the polyelectrolytes in EMIDCA are homogeneous, flexible elastomeric gel materials at 10 − 15 wt.‐% of total polyelectrolyte. Conductivities higher than 8 · 10−3 S · cm−1 at 30 °C have been achieved. The effects of the monomer composition, polyelectrolyte concentration, temperature and lithium concentration on the ionic conductivity have been studied using thermal and conductivity analysis, and pulsed field gradient nuclear magnetic resonance techniques.Comparison of the measured and calculated lithium conductivity at 30 °C.magnified imageComparison of the measured and calculated lithium conductivity at 30 °C.

Moderately Concentrated Solutions of Polystyrene. 6. Gel Formation in Carbon Disulfide

Gel formation of moderately concentrated solutions of anionically polymerized polystyrene in carbon disulfide is studied to conclude that association of the two sulfur atoms on CS 2 with phenyl rings on different polystyrene chains results in a few cross-link loci per polymer chain, creating an elastomeric gel. The equilibrium compliance J e of a gel sample is evaluated from creep and recoverable strain measurements, and a light scattering method to analyze constrained oscillations in the gel is used to determine the storage modulus G'(ω) and the dynamic viscosity η'(ω) for ω small enough that G'(ω) G e = 1/J e . The sharp increase of the relative viscosity as T is reduced to within a few degrees of T gel is modeled by the viscosity for a branched chain, with the number of cross-links per primary chain approaching unity as T goes to T gel . The carbon disulfide/polystyrene interaction is supported by light scattering measurements on dilute solutions of polystyrene in a toluene-CS 2 mixed solvent, which show preferential solvation of polystyrene by CS 2 and the observation that the temperature T gel required to form a gel with moderately concentrated solutions of polystyrene in a toluene-CS 2 mixed solvent is essentially independent of the toluene concentration. Further, the temperature dependence of the NMR spin-lattice relaxation time of the 13 C nucleus of CS 2 in solutions with polystyrene is about the same as that observed for J e . It is noted that for high molecular weight polymer, T gel scales with the condition for effective chain overlap, expressed by c[η] o α c , 3 with α c the expansion factor at concentration c, and [η] o the intrinsic viscosity under Flory Θ conditions.