Endothelial cell migration on surface-density gradients of fibronectin, VEGF, or both proteins

Cell migration is essential to many physiological processes, including angiogenesis, which is critical to the success of implanted biomaterials and tissue-engineered constructs. Gradients play an important role in cell migration. Previous work on cell migration has been mostly executed either in the concentration gradients of stimuli (e.g., VEGF) in bulk or hydrogels or on the surface-density gradients of ECM proteins (e.g., fibronectin) or small ligands (e.g., RGD). Little work has been done to investigate how cell migration responds to the surface-density gradients of growth factors. No work has been done to study how the surface gradients of both adhesive proteins and growth factors influence cell migration. In this work, we studied the effect of the surface-density gradients of fibronectin (FN), VEGF, or both proteins on endothelial cell migration. Gradients with different slopes were prepared to study how the gradient slope affects cell migration. The gradients were generated by first forming a counter-propagating C15COOH/C11OH self-assembled monolayer (SAM) gradient using a surface electrochemistry approach, followed by activating the -COOH moieties and covalently immobilizing proteins onto the surface. Fourier transform infrared spectra and X-ray photoelectron spectroscopy were used to characterize the SAM and protein gradients, respectively. A free cell migration assay using bovine aortic endothelial cells was performed on various gradient surfaces or on surfaces with uniform protein density. Results showed that cells on the surface-density gradients of FN, VEGF, or both proteins moved faster along the gradient direction than on the respective uniform control surface after 24-h cell culture. It is also shown that for each protein or protein combination, the directional cell displacement was not statistically different between two gradients with different slopes. Results show that the directional cell migration was increased by about 2-fold on the VEGF gradient as compared to the FN gradient and was further increased by another 2-fold on the combined gradients of both proteins as compared to the VEGF gradient alone. This is the first work to create surface-density gradients of VEGF and the first study to generate a combined surface gradient of growth factor and ECM protein to investigate their effect on cell migration on surfaces. This work broadens our understanding of the directional movement of endothelial cells. Our findings provide useful information for directing cell migration into tissue-engineered constructs and can be potentially used for those applications where cell migration is critical, such as angiogenesis.     

水蒸气对PtSn/ZnAl2O4催化剂结构的影响

利用X-射线衍射研究了经氢还原及还原后又经高温水蒸气处理的PtSn／ZnAl2O4催化剂,结果表明,催化剂的相结构是Sn载量的函数．还原态的Pt／ZnAl2O4催化剂中Pt以金属态存在,Pt／Sn原子比为1：1、1：3及1：10的PtSn／ZnAl2O4催化剂还原后分别生成PtZn、PtSn、尽Sn及Pt物相;高温水蒸气处理对Pt／ZnAl2O4样品的相结构及Pt晶粒尺寸无明显影响,但却使Ptsn／ZnAl2O4催化剂的相结构发生显著变化;对于1：l及1：3的Ptsn／ZnAl2O4,水蒸气使各自还原态中的PtZn、PtSn合金重构为Pt3Sn合金,同时使1：10PtSn／ZnAl2O4的民β-Sn及Pt物相消失,而生成了新的PtSn合金相．     

Unbinding of the streptavidin-biotin complex by atomic force microscopy: a hybrid simulation study

A hybrid molecular simulation technique, which combines molecular dynamics and continuum mechanics, was used to study the single-molecule unbinding force of a streptavidin-biotin complex. The hybrid method enables atomistic simulations of unbinding events at the millisecond time scale of atomic force microscopy (AFM) experiments. The logarithmic relationship between the unbinding force of the streptavidin-biotin complex and the loading rate (the product of cantilever spring constant and pulling velocity) in AFM experiments was confirmed by hybrid simulations. The unbinding forces, cantilever and tip positions, locations of energy barriers, and unbinding pathway were analyzed. Hybrid simulation results from this work not only interpret unbinding AFM experiments but also provide detailed molecular information not available in AFM experiments.     

Understanding the nonfouling mechanism of surfaces through molecular simulations of sugar-based self-assembled monolayers

This paper presents a molecular simulation study of the interactions of a protein (lysozyme) with self-assembled monolayers (SAMs) of mannitol and sorbitol terminated alkanethiols in the presence of explicit water molecules and ions. The all-atom simulations were performed to calculate the force generated on the protein as a function of its distance above the SAM surfaces. The structural and dynamic properties of water molecules both above the SAM surfaces and around the SAM head groups were analyzed to provide a better understanding of the nonfouling behavior of the sugar-based SAM surfaces. Results from this work suggest that both mannitol and sorbitol SAMs generate a tightly bound, structured water layer around the SAM chains. This hydration layer creates a repulsive force on the protein when it approaches the surface, resulting in a nonfouling surface despite the presence of hydrogen-bond donor groups. This work demonstrates the importance of strong surface-water interactions for surface resistance to nonspecific protein adsorption.     

Internal Architecture of Zwitterionic Polymer Brushes Regulates Nonfouling Properties

In this work, we study how film thickness and chain packing density affect the protein‐resistant properties of polymer brushes in complex media. Polymer brushes based on dual‐functional poly(carboxybetaine acrylamide) (pCB) were prepared via surface‐initiated photoiniferter‐mediated polymerization. By adjusting UV radiation time and solvent polarity, pCB films with different thicknesses can be achieved and characterized using an ellipsometer. The packing density of pCB polymer chains is directly related to the swelling ratio of swollen to collapsed film thicknesses. Results showed that the dry film thickness alone, used often in the literature, is not sufficient to correlate with nonfouling properties and the chain packing density must be considered for the design of nonfouling surface coatings.     

Supramolecular assembly of cyclodextrin-based nanoparticles on solid surfaces for gene delivery

In this work, a new approach for surface-mediated gene delivery based on inclusion complex formation between the solid surface and delivery vehicles is presented. beta-Cyclodextrin (CD) molecules form high-affinity inclusion complexes with adamantane. This complexation ability was used to specifically immobilize beta-CD-modified poly(ethylenimine) (CD-PEI) nanoparticles on adamantane- (AD-) modified self-assembled monolayers. To investigate the nanoparticle/surface interaction, CD-PEI-based and PEI-based nanoparticles were passed through a surface plasmon resonance flow cell containing the monolayers. CD-PEI nanoparticles are specifically immobilized on the chip surface by cyclodextrin-adamantane inclusion complex formation. Minimal nanoparticle adsorption was detected with PEI-based nanoparticles or on control surfaces. Competition studies with free cyclodextrins reveal that the multivalent interactions between CD-PEI nanoparticles and the adamantane-modified surface results in significantly higher binding affinity than single cyclodextrin-adamantane complexes. Immobilized nanoparticles were characterized by atomic force microscopy and quantified by fluorescence assay. Thus, the ability of CD-PEI nanoparticles to form inclusion complexes can be exploited to attain specific, high-affinity loading of delivery vehicles onto solid surfaces.     

Controlling DNA orientation on mixed ssDNA/OEG SAMs

We present and characterize a mixed self-assembled monolayer (SAM) consisting of single-stranded oligonucleotide (ssDNA)- and oligo(ethylene glycol) (OEG)-terminated thiols. The ssDNA/OEG SAMs are prepared by simultaneous coadsorption from a common thiol solution over a broad range of compositions. Electron spectroscopy for chemical analysis (ESCA) is used to measure the surface coverage of ssDNA, whereas surface plasmon resonance (SPR) sensor is used to measure the hybridization of complementary ssDNA and protein resistance. Through the complementary use of these techniques, we find that the composition of OEG in the assembly solution controls a key parameter: the surface coverage of ssDNA on the surface. There is evidence that it influences the orientation of the immobilized ssDNA probes. Lower OEG concentrations yield a surface with higher ssDNA coverage and less favorable orientation, whereas higher OEG concentrations produce a surface with lower DNA coverage and more favorable orientation. Competition between these two effects controls the hybridization efficiency of the ssDNA surface. Compared to ssDNA surfaces prepared with other diluent thiols, the use of OEG improves the protein resistance of the surface, making it more broadly applicable.     

Molecular simulation studies of the structure of phosphorylcholine self-assembled monolayers

We report a study of the structure of phosphorylcholine self-assembled monolayers (PC-SAMs) on Au(111) surfaces using both molecular mechanics (MM) and molecular dynamics (MD) simulation techniques. The lattice structure (i.e., packing densities and patterns) of the PC chains was determined first, by examining the packing energies of different structures by MM simulations in an implicit solvent. The chain orientation (i.e., antiparallel and parallel arrangements of the PC head groups) was then evaluated. The initial azimuthal angles of the PC chains were also adjusted to ensure that the optimal lattice structure was found. Finally, the two most probable lattice structures were solvated with explicit water molecules and their energies were compared after 1.5 ns of MD simulations to verify the optimal structures obtained from MM. We found that the optimal lattice structure of the PC-SAM corresponds to a radical7 x radical7 R19degree lattice structure (i.e., surface coverage of 50.4 A(2)molecule) with a parallel arrangement of the head groups. The corresponding thickness of the optimal PC-SAM is 13.4 A which is in agreement with that from experiments. The head groups of the PC chains are aligned on the surface in such a way that their dipole components are minimized. The P-->N vector of the head groups forms an angle of 82 degrees with respect to the surface normal. The tilt direction of molecular chains was observed to be towards their next nearest neighbor.     

Chaotrope vs. kosmotrope: which one has lower friction?

We examine the frictional properties of zwitterionic surfaces and explore whether chaotropic or kosmotropic charged groups are preferred to achieve lower friction. Self-assembled monolayers of carboxybetaine (CB-SAMs) and sulfurbetaine (SB-SAMs) are used as model surfaces as they contain the same positively charged group, but different negatively charged ones. The negatively charged groups are kosmotropic carboxylates in the CB-SAM surfaces and chaotropic sulfonate groups in the SB-SAM surfaces, respectively. The results show that the friction of the SB-SAM surfaces is even lower than that of the CB-SAM surfaces although both surfaces have low friction. This suggests that chaotropic charged groups are better in reducing friction than kosmotropic groups. The lower friction of the SB-SAM surfaces over the CB-SAM can be explained by the higher mobility of water near the SB-SAM surfaces, as shown in the survival autocorrelation function and the dipole autocorrelation function of hydration water molecules.     

Packing structures of single-stranded DNA and double-stranded DNA thiolates on Au(111): a molecular simulation study

The packing structures of single-stranded DNA (ssDNA) and double-stranded DNA (dsDNA) thiolates on implicit gold surfaces were studied in explicit aqueous solutions of 1M NaCl using molecular dynamics simulations. The simulations were based on individual DNA chains placed in hexagonal simulation boxes of different sizes, representing various packing densities. The total potential energy per DNA chain was compared. The optimal packing structures were determined based on the minimal potential energy within the limits of the conditions that were evaluated in this study. The optimal packing density of ssDNA was found to be 0.19 DNA chains/nm(2), which is consistent with that determined experimentally. Furthermore, the optimal packing density of dsDNA was shown to be approximately 58% of the packing density for ssDNA, indicating that the packing of ssDNA should be approximately 58% of its optimal packing in order to achieve the best hybridization.