Electric properties of macromolecules. IX. Dipole moment, polarizability, and optical anisotropy factor of collagen in solution from electric birefringence

Gelatin as It Is: History and Modernity

The data concerning the synthesis and physicochemical characteristics of one of the practically important proteins-gelatin, as well as the possibilities of its practical application, are systematized and discussed. When considering the latter, emphasis is placed on the use of gelatin in those areas of science and technology that are associated with the specifics of the spatial/molecular structure of this high-molecular compound, namely, as a binder for the silver halide photographic process, immobilized matrix systems with a nano-level organization of an immobilized substance, matrices for creating pharmaceutical/dosage forms and protein-based nanosystems. It was concluded that the use of this protein is promising in the future.

Isolated Collagen Mimetic Peptide Assemblies Have Stable Triple-Helix Structures

The origin of the triple-helix structure and high stability of collagen has been debated for many years. As models of the triple helix and building blocks for new biomaterials, collagen mimetic peptide (CMP) assemblies have been deeply studied in the condensed phase. In particular, it was found that hydroxylation of proline, an abundant post-translational modification in collagen, increases its stability. Two main hypotheses emerged to account for this behavior: 1) intra-helix stereoelectronic effects, and 2) the role of water molecules H-bound to hydroxyproline side-chains. However, in condensed-phase investigations, the influence of water cannot be fully removed. Therefore, we employed a combination of tandem ion mobility and mass spectrometries to assess the structure and stability of CMP assemblies in the gas phase. These results show a conservation of the structure and stability properties of triple helix models in the absence of solvent, supporting an important role of stereoelectronic effects. Moreover, evidence that small triple helix assemblies with controlled stoichiometry can be studied in the gas phase is given, which opens new perspectives in the understanding of the first steps of collagen fiber growth.

Birefringence and second harmonic generation on tendon collagen following red linearly polarized laser irradiation

Regarding the importance of type I collagen in understanding the mechanical properties of a range of tissues, there is still a gap in our knowledge of how proteins perform such work. There is consensus in literature that the mechanical characteristics of a tissue are primarily determined by the organization of its molecules. The purpose of this study was to characterize the organization of non-irradiated and irradiated type I collagen. Irradiation was performed with a linearly polarized HeNe laser (λ = 632.8 nm) and characterization was undertaken using polarized light microscopy to investigate the birefringence and second harmonic generation to analyze nonlinear susceptibility. Rats received laser irradiation (P = 6.0 mW, I = 21.2 mW/cm(2), E ≈ 0.3 J, ED = 1.0 J/cm(2)) on their healthy Achilles tendons, which after were extracted to prepare the specimens. Our results show that irradiated samples present higher birefringence and greater non-linear susceptibility than non-irradiated samples. Under studied conditions, we propose that a red laser with polarization direction aligned in parallel to the tendon long axis promotes further alignment on the ordered healthy collagen fibrils towards the electric field incident. Thus, prospects for biomedical applications for laser polarized radiation on type I collagen are encouraging since it supports greater tissue organization.

Epitaxially guided assembly of collagen layers on mica surfaces

Ordered assembly of collagen molecules on flat substrates has potential for various applications and serves as a model system for studying the assembly process. While previous studies demonstrated self-assembly of collagen on muscovite mica into highly ordered layers, the mechanism by which different conditions affect the resulting morphology remains to be elucidated. Using atomic force microscopy, we follow the assembly of collagen on muscovite mica at a concentration lower than the critical fibrillogenesis concentration in bulk. Initially, individual collagen molecules adsorb to mica and subsequently nucleate into fibrils possessing the 67 nm D-periodic bands. Emergence of fibrils aligned in parallel despite large interfibril distances agrees with an alignment mechanism guided by the underlying mica. The epitaxial growth was further confirmed by the formation of novel triangular networks of collagen fibrils on phlogopite mica, whose surface lattice is known to have a hexagonal symmetry, whereas the more widely used muscovite does not. Comparing collagen assembly on the two types of mica at different potassium concentrations revealed that potassium binds to the negatively charged mica surface and neutralizes it, thereby reducing the binding affinity of collagen and enhancing surface diffusion. These results suggest that collagen assembly on mica follows the surface adsorption, diffusion, nucleation, and growth pathway, where the growth direction is determined at the nucleation step. Comparison with other molecules that assemble similarly on mica supports generality of the proposed assembly mechanism, the knowledge of which will be useful for controlling the resulting surface morphologies.

Dynamic shear-influenced collagen self-assembly

The ability to influence the direction of polymerization of a self-assembling biomolecular system has the potential to generate materials with extremely high anisotropy. In biological systems where highly-oriented cellular populations give rise to aligned and often load-bearing tissue such organized molecular scaffolds could aid in the contact guidance of cells for engineered tissue constructs (e.g. cornea and tendon). In this investigation we examine the detailed dynamics of pepsin-extracted type I bovine collagen assembly on a glass surface under the influence of flow between two plates. Differential Interference Contrast (DIC) imaging (60x-1.4NA) with focal plane stabilization was used to resolve and track the growth of collagen aggregates on borosilicate glass for 4 different shear rates (500, 80, 20, and 9s(-1)). The detailed morphology of the collagen fibrils/aggregates was examined using Quick Freeze Deep Etch (QFDE) electron microscopy. Nucleation of fibrils on the glass was observed to occur rapidly (approximately 2 min) followed by continued growth of the fibrils. The growth rates were dependent on flow in a complex manner with the highest rate of axial growth (0.1 micro/s) occurring at a shear rate of 9s(-1). The lowest growth rate occurred at the highest shear. Fibrils were observed to both branch and join during the experiments. The best alignment of fibrils was observed at intermediate shear rates of 20 and 80s(-1). However, the investigation revealed that fibril directional growth was not stable. At high shear rates, fibrils would often turn downstream forming what we term "hooks" which are likely the combined result of monomer interaction with the initial collagen layer or "mat" and the high shear rate. Further, QFDE examination of fibril morphology demonstrated that the assembled fibrillar structure did not possess native D-periodicity. Instead, fibrils comprised a collection of generally aligned, monomers which were self-assembled to form a fibril-like aggregate. In conclusion, though constant shear-rate clearly influences collagen fibrillar alignment, the formation of highly-organized collagenous arrays of native-like D-banded fibrils remains a challenge. Modulation of shear in combination with surface energy patterning to produce a highly-aligned initial mat may provide significant improvement of both the fibril morphology and alignment.

Quantitative measurements of linear birefringence during heating of native collagen

BACKGROUND AND OBJECTIVE

Linear birefringence is an anisotropic property of rat tail tendon, which is largely composed of collagen. Our goal is to show that the dynamic range and sensitivity of the linear birefringence loss of collagen during heating are sufficient for kinetic modeling of the reaction.

STUDY DESIGN, MATERIALS AND METHODS

The linear birefringence loss was quantified for tendon denatured via both a heated-isotonic-saline bath and a heated stage. All measurements were made with a polarizing transmission microscope equipped with a Berek compensator.

RESULTS

The data show that the loss of linear birefringence is a first-order kinetic reaction. The native rat tail tendon birefringence, delta n = 3.0 +/- 0.6 x 10(-3) (mean +/- std. err.), is lost after denaturation occurs (delta n = 0). Application of the Arrhenius equation to the linear birefringence data yields the activation energy (Ea = 89 +/- 1 kcal/mole), pre-exponential coefficient (A = e130 +/- 1 s-1), enthalpy (delta H = 88 +/- 1 kcal/mole) and entropy (delta S = 197 +/- 2 cal/degree K.mole).

CONCLUSION

This study shows that dynamic changes in linear birefringence can be used to monitor thermally induced changes in collagen.

Mapping of Birefringence and Thermal Damage in Tissue by use of Polarization-Sensitive Optical Coherence Tomography

We demonstrate cross-sectional birefringence- and polarization-independent backscatter imaging of laser-induced thermal damage in porcine myocardium in vitro, using a polarization-sensitive optical coherence tomography system. We compare the generated images with histological sections of the tissue and demonstrate that birefringence is a more sensitive indicator of thermal damage than is backscattered light. Loss of birefringence in thermally damaged regions is quantified and shown to have significant contrast with undamaged sections of the tissue. A detailed theoretical analysis of the birefringence measurements is provided, including a calculation of the systematic errors associated with background noise, system imperfections, and tissue dichroism.

Electric and optical anisotropy and their osmotically induced changes of photoreceptor disk membrane vesicles

Electro-optical characterization of the photoreceptor disk membrane vesicle is performed by examining the electric field and concentration dependence of the study-state birefringence of aqueous suspensions of the vesicles. The electric polarizability anisotropy is found to be negative and of large magnitude: alpha 1 - alpha 2 = -(1-3) X 10 cm3. The optical anisotropy is determined to be also negative but of small magnitude: g 1 - g 2 = -1 X 10(-7). The specific Kerr constant deduced from the concentration dependence of the Kerr constant is found to be very large: Ksp = 7 X 10(-4) e.s.u. Upon deforming the vesicles osmotically from the spherical shell to the disk structure, the steady-state birefringence increases by an order of magnitude which is attributed solely to the increase in optical anisotropy attending the corresponding change in the geometric eccentricity of the vesicle. A plausible birefringence mechanism based on the known structural features of the vesicles is proposed, which would account for these findings.

Human spectrin. V. A comparative electro-optic study of heterotetramers and heterodimers

The electrically induced birefringence of human spectrin heterotetramer and heterodimer solutions at 5 degrees C has been studied. 1. The steady-state birefringence, delta, was found to be approximately proportional to the electric field strength, E, when E greater than or equal to 0.2 kV/mm. For spectrin solutions the specific linear coefficient, delta/(E x c), therefore is a more relevant parameter for describing birefringence saturation behavior when E greater than or equal to 0.2 kV/mm than the commonly used Kerr constant. At 5 degrees C were measured delta/(E x c) = (27 +/- 5) x 10(-8)m4 x V(-1) x kg(-1) for heterodimers and heterotetramers. 2. At 5 degrees C both heterotetramers and heterodimers exhibited more than one birefringence relaxation time and the shortest of these was for both molecules found to be 4.2 +/- 1.0 microseconds. This indicates that the spectrin molecules are highly flexible. The birefringence build-up time for heterotetramers and heterodimers was found to be 20 +/- 7 microseconds and 15 +/- 5 microseconds, respectively.

Human spectrin. II. An electro-optic study

The electrically induced birefringence of human spectrin heterodimer solutions has been studied. 1. Human spectrin heterodimers were found to have a specific Kerr constant Bsp = +(5 +/- 2) . 10(-11) m4/(V2 . kg). 2. Human spectrin exhibited a birefringence relaxation time tau decay = (2.0 +/- 0.3) microseconds. 3. The electro-optic study indicates that human spectrin heterodimers have a contour length of more than 40--50 nm.