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Smart polymers and interfaces for dynamic cell-biomaterials interactions

Published online by Cambridge University Press:  12 September 2012

Stephen Kustra
Affiliation:
Carnegie Mellon University, Pittsburgh, PA; skustra@andrew.cmu.edu
Christopher J. Bettinger
Affiliation:
Carnegie Mellon University, Pittsburgh, PA; cbetting@andrew.cmu.edu

Abstract

Fundamental aspects of the interactions between cells and biomaterials provide a crucial framework for the design of many systems that interact with the human body. A comprehensive understanding of multifactorial processes may provide an adequate basis for the rational design of implantable devices ranging from nanoparticles for drug delivery and scaffolds for tissue engineering, to artificial organs for augmentation and rehabilitation. Recent progress in the elucidation of cell-biomaterials interactions has been predicated on advances in polymer chemistry, materials engineering, and device microfabrication. The confluence of these developments has stimulated a newfound ability to design soft materials and interfaces with precise chemical, physical, and mechanical properties. While static surfaces can yield insight into the interaction of mammalian cells with medical materials, the study of fundamental cell-biomaterials phenomena will benefit significantly from the ability to present biologically active signals to cells with spatiotemporal control. Specifically, the use of dynamic materials and interfaces can mirror the intrinsic dynamic behavior of living cells. This article highlights recent advances in soft materials design, interfacial engineering, and synthetic polymer networks in the context of producing dynamic materials to study cell-biomaterials interactions. Emerging challenges and future research directions are also discussed.

Information

Type
Research Article
Copyright
Copyright © Materials Research Society 2012
Figure 0

Table I. Summary of dynamic materials and their associated stimuli.

Figure 1

Figure 1. Controlled electrical desorption of self-assembled monolayers to assess polarized cell migration. (a) Two representative asymmetric patterns used in biased migration experiments are shown. The dark area represents the cell adhesive domain and the approximate shape of the cell prior to release of the migration barrier (the self-assembled monolayer). The Golgi and the centrosome are located closer to the half of a cell with the blunt end. The various components of the cell are identified as follows: actin (red), the Golgi (green), the nucleus (blue), microtubules (red), and the centrosome (green), respectively. HUAEC, human umbilical artery endothelial cells. (b) Asymmetric pattern and corresponding bright field image of a fibroblast are shown. (c) Time-lapse images (in minutes) show the motility of a polarized fibroblast after the removal of the migration barrier. (d) Kidney cells derived from monkeys (COS-7 cells) show a similar behavior to fibroblasts. This system depicts the ability to observe real-time changes in a cytoskeletal structure. Reprinted with permission from Reference 41. ©2005, National Academy of Sciences.

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Figure 2. Dynamic desorption of self-assembled monolayers (SAMs) using laser-scanning lithography. (a) Gold-coated glass coverslips are functionalized with alkanethiols. Select regions are thermally desorbed using laser-scanning lithography (LSL). Bare regions are exposed to additional alkanethiols. This process is continued to allow for patterning of multiple SAMs. (b–d) Multifaceted surfaces can be created to present coordinated ligands, including adhesion-promoting peptides (GRGD) and fibronectin (HFN). The multifaceted surface displays independent arrays of GRGD (red horizontal patterns) and HFN (blue vertical patterns). These dynamic interfaces can be used to study lamella formation and migration in endothelial cells. (e) Endothelial cells are initially elongated in a direction parallel to the long axis of the HFN patterns. The cells then produce membrane extensions along GRGD patterns and form lamella near fibronectin. Scale bars represent 20 microns. Reprinted with permission from Reference 45. ©2011, Wiley.

Figure 3

Figure 3. (a) Fabrication of uniaxial and biaxial nanowrinkles for use as a cell culture platform. (b) Biaxial and (c) uniaxial scanning electron microscopy images of shrunk polystyrene sheets with a layer of gold (10 nm). Controlled wrinkling patterns can be used as a cell culture platform for real-time microscopy and cytoskeletal dynamic studies. Reprinted with permission from Reference 78. ©2009, Wiley.

Figure 4

Figure 4. (a) Thermal effect of cell culture substrate transition from a grooved surface to a flat surface using an SMP network. After cells were cultured for 9.5 h at 30°C, the substrate was triggered by placing a sample in a 37°C incubator. The traces below the image represent a cross-section of the contours of the culture surface. (b) The change in substrate topography controls cell behavior. Confocal images of cells stained with phalloidin on a temporary grooved structure have microstructures in alignment with the groove direction (white arrow). After the surface transitions, the cells rearrange, are randomly oriented, and show stress fiber formation. Scale bar in (b) is 100 μm. Reprinted with permission from Reference 80. ©2011, Elsevier.

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Figure 5. Methods for photodegradable hydrogel synthesis and patterning. (a) Photodegradable hydrogels formed by redox-initiated, free-radical chain polymerization, which is indicated by R*. The resultant network is comprised of polyacrylate kinetic chains (green) connected by PEG-based cross-links (black) with photocleavable moieties (blue) in the backbone. (b) Using a chrome mask, the surface of the photocleavable hydrogel can be patterned with features of depths that depend upon exposure time. Features can be generated within minutes of irradiation time. (c) Use of a laser-scanning microscope (LSM) with a 405 nm laser can also be used to create three-dimensional patterns by precisely moving the laser in the x–y plane using a scanner. The z-dimension is controlled with a higher minimum feature resolution by either controlling the focal plane of the laser or the location of the stage. Reprinted with permission from Reference 112. ©2010, Nature Publishing Group.