| Literature DB >> 34911759 |
Yin Chang1, Rox Middleton1, Yu Ogawa2, Tom Gregory3, Lisa M Steiner1,4, Alexander Kovalev5, Rebecca H N Karanja6, Paula J Rudall3, Beverley J Glover7, Stanislav N Gorb5, Silvia Vignolini8.
Abstract
Chiral asymmetry is important in a wide variety of disciplines and occurs across length scales. While several natural chiral biomolecules exist only with single handedness, they can produce complex hierarchical structures with opposite chiralities. Understanding how the handedness is transferred from molecular to the macroscopic scales is far from trivial. An intriguing example is the transfer of the handedness of helicoidal organizations of cellulose microfibrils in plant cell walls. These cellulose helicoids produce structural colors if their dimension is comparable to the wavelength of visible light. All previously reported examples of a helicoidal structure in plants are left-handed except, remarkably, in the Pollia condensata fruit; both left- and right-handed helicoidal cell walls are found in neighboring cells of the same tissue. By simultaneously studying optical and mechanical responses of cells with different handednesses, we propose that the chirality of helicoids results from differences in cell wall composition. In detail, here we showed statistical substantiation of three different observations: 1) light reflected from right-handed cells is red shifted compared to light reflected from left-handed cells, 2) right-handed cells occur more rarely than left-handed ones, and 3) right-handed cells are located mainly in regions corresponding to interlocular divisions. Finally, 4) right-handed cells have an average lower elastic modulus compared to left-handed cells of the same color. Our findings, combined with mechanical simulation, suggest that the different chiralities of helicoids in the cell wall may result from different chemical composition, which strengthens previous hypotheses that hemicellulose might mediate the rotations of cellulose microfibrils.Entities:
Keywords: cellulose–hemicellulose interaction; chirality; helicoidal cell wall; mechanical properties of plant cell wall; structural colors
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Year: 2021 PMID: 34911759 PMCID: PMC8713805 DOI: 10.1073/pnas.2111723118
Source DB: PubMed Journal: Proc Natl Acad Sci U S A ISSN: 0027-8424 Impact factor: 11.205
Fig. 1.Polarized coloration and distribution of differently colored left- and right-handed cells on the epicarp of P. condensata fruits. (A) P. condensata: slightly ovoid shaped fruit of about 4 to 5 mm in diameter exhibiting striped coloration including the following: a white interseptum stripe (1), the blue nonstripe regions (2), and a red septum stripe (3). (B) Polarization-resolved optical micrograph of epicarp measured using left- (black arrow) and right-handed (white arrow) polarized light, respectively. In the images, structurally colored cells are recognizable (cell contour outlined with white dashed lines). The color of the cell is seen as a line along the Top Center due to the curvature of the cell and the numerical aperture of the objective. (C) Statistical analysis of colors and chirality of cells across four fruits revealing that right-handed cells (green plot) generate more red-shifted colors than left-handed cells (blue plot). (D) The cell ratio of left-handed and right-handed cells with specific reflected wavelength at the three differently colored regions marked in (A) are calculated and normalized to the total numbers of cells. A higher proportion of right-handed cells with longer reflected wavelengths in the stripe regions (1) and (3) contribute to the white or red macroscopic coloration.
Fig. 2.TEM images of the epicarp cross-section of a fruit of P. condensata and enlarged images of the cell walls of six individual cells as labeled. Different region of the epicarp, namely the cuticle layer, the region containing the structurally colored cells, and pigmented cells are shaded with different false colors of yellow, red, and brown, respectively. Note that only one handedness can be found in each cell with no mixture of handedness. Varied pitch lengths are observed in cells which explain the wide variation in reflection peak wavelength from both cell types. (Scale bar: 100 nm.)
Fig. 3.Nanoindentation on cells with different colors and handedness. (A) SEM cross-section image of the helicoidal cell wall after removal of the outer cuticle and a schematic illustration of indentation on cells with a Berkovich tip. (B) The top-view SEM image shows an ideal indent at the center of a cell. (C) Polarization-resolved optical micrograph in two positions of epicarp measured after indentation, using left- (black arrow) and right-handed (white arrow) polarized light. Each indent indicated by arrow heads can be related to a specific color and handedness (black: left-handed; white: right-handed) of the cell. (Scale bar: 20 μm.)
Fig. 4.Measured and simulated mechanical properties of the cellulose cell walls (blue marks for left-handed and green marks for right-handed cells). (A) Experimentally measured reduced modulus, E, as a function of the handedness and color of the helicoids. On average (the black dashed line), red-shifted cells have higher reduced modulus*, E. The reduced modulus takes into account the elastic deformation in both the surface of the sample and the tip of the indenter during contact. Here, the deformation of the tip is ignored, so the reduced modulus relates to the Young’s modulus () and Poisson’s ratio () of the sample: . A similar trend is shown for both chiralities despite the fact that left-handed cells are stiffer than the same color right-handed cells. Hardness, H, of differently colored cells is constant at 0.7 to 0.8 GPa. (B) The mechanical properties of general biological materials (light gray triangles) and of some specifically hardened biological materials (black triangles). Data are collected from literature across eight taxonomies (30). Pollia fruits have cell walls with high stiffness comparable to hardened biomaterials. (C) Computationally calculated stiffness of models with CMF diameter of 3 or 4 nm with varied filling fraction of 0.1, 0.2, or 0.3, respectively, and pitch lengths from 120 to 220 nm (represented by spots with different greyness: the darker spots indicate models with larger pitch lengths). The maximum and minimum values of stiffness in each condition were labeled on the graph.