AFM methods for studying the morphology and micromechanical properties of the membrane of human buccal epithelium cell

Author:

Torkhov N. A.,Buchelnikova V. A.,Mosunov A. A.,Ivonin I. V.

Abstract

AbstractUsing AFM methods in air under normal conditions in a wide range of local force effects ($${F}_{const}$$ F const < 40 μN) the relief, functional micromechanical properties (elasticity coefficient $$K$$ K , Young’s modulus $$E$$ E , elastic $${\Delta h}_{dfrm}$$ Δ h dfrm and plastic $${\Delta h}_{stiff}$$ Δ h stiff deformations) and adhesive properties (work $$A$$ A of adhesive forces $${F}_{adh}={F}_{adh}(x;y)$$ F adh = F adh ( x ; y ) ) of the membranes of living adult cells of human buccal epithelium were studied in the presence of a protective layer < 100 nm of buffer solution that prevented the cells from drying. Almost all geometric and functional characteristics of the membrane in the local approximation at the micro- and nanolevels are affected by size effects and obey the laws of fractal geometry. The Brownian multifractal relief of the membrane is characterized by dimension $${D}_{f}$$ D f < 2.56 and irregularities < 500 nm vertically and < 2 μm horizontally. Its response to elastic (≤ 6 nN), active (6–21 nN), or passive (> 21 nN) stimulation ($${F}_{const}$$ F const ) is a non-trivial selective process and exhibits a correspondingly elastic ($$K=$$ K = 67.4 N/m), active ($$K=$$ K = 80.2 N/m) and passive ($$K=$$ K = 84.5 N/m) responses. $$K=K({F}_{const})$$ K = K ( F const ) and $$E=E({F}_{const})$$ E = E ( F const ) depend on $${F}_{const}$$ F const . Having undergone slight plastic deformations $${\Delta h}_{stiff}$$ Δ h stiff < 300 nm, the membrane is capable of restoring its shape. We mapped ($$E=E(x;y)$$ E = E ( x ; y ) , $${D}_{f}$$ D f = 2.56; $${\Delta h}_{dfrm}={\Delta h}_{dfrm}(x;y)$$ Δ h dfrm = Δ h dfrm ( x ; y ) , $${D}_{f}$$ D f = 2.68; $${\Delta h}_{stiff}={\Delta h}_{stiff}(x;y)$$ Δ h stiff = Δ h stiff ( x ; y ) , $${D}_{f }$$ D f = 2.42, $$A=A\left(x;y\right)$$ A = A x ; y and $${F}_{adh}={F}_{adh}(x;y)$$ F adh = F adh ( x ; y ) ) indicating its complex cavernous structure.

Funder

This study was supported by the Tomsk State University Development Programme

The authors would like express thanks to the supporting by Sevastopol State University

Publisher

Springer Science and Business Media LLC

Subject

Multidisciplinary

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