Using AFM methods in air under normal conditions in a wide range of local force effects (\documentclass[12pt]{minimal}
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				\begin{document}$${F}_{const}$$\end{document}Fconst< 40 μN) the relief, functional micromechanical properties (elasticity coefficient\documentclass[12pt]{minimal}
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				\begin{document}$$K$$\end{document}K, Young’s modulus\documentclass[12pt]{minimal}
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				\begin{document}$$E$$\end{document}E, elastic\documentclass[12pt]{minimal}
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				\begin{document}$${\Delta h}_{dfrm}$$\end{document}Δhdfrmand plastic\documentclass[12pt]{minimal}
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				\begin{document}$${\Delta h}_{stiff}$$\end{document}Δhstiffdeformations) and adhesive properties (work\documentclass[12pt]{minimal}
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				\begin{document}$$A$$\end{document}Aof adhesive forces\documentclass[12pt]{minimal}
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				\begin{document}$${F}_{adh}={F}_{adh}(x;y)$$\end{document}Fadh=Fadh(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\documentclass[12pt]{minimal}
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				\begin{document}$${D}_{f}$$\end{document}Df< 2.56 and irregularities < 500 nm vertically and < 2 μm horizontally. Its response to elastic (≤ 6nN), active (6–21 nN), or passive (> 21 nN) stimulation (\documentclass[12pt]{minimal}
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				\begin{document}$${F}_{const}$$\end{document}Fconst) is a non-trivial selective process and exhibits a correspondingly elastic (\documentclass[12pt]{minimal}
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				\begin{document}$$K=$$\end{document}K=67.4 N/m), active (\documentclass[12pt]{minimal}
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				\begin{document}$$K=$$\end{document}K=80.2 N/m) and passive (\documentclass[12pt]{minimal}
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				\begin{document}$$K=$$\end{document}K=84.5 N/m) responses.\documentclass[12pt]{minimal}
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				\begin{document}$$K=K({F}_{const})$$\end{document}K=K(Fconst)and\documentclass[12pt]{minimal}
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				\begin{document}$$E=E({F}_{const})$$\end{document}E=E(Fconst)depend on\documentclass[12pt]{minimal}
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				\begin{document}$${F}_{const}$$\end{document}Fconst. Having undergone slight plastic deformations\documentclass[12pt]{minimal}
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				\begin{document}$${\Delta h}_{stiff}$$\end{document}Δhstiff< 300 nm, the membrane is capable of restoring its shape. We mapped (\documentclass[12pt]{minimal}
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				\begin{document}$$E=E(x;y)$$\end{document}E=E(x;y),\documentclass[12pt]{minimal}
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				\begin{document}$${D}_{f}$$\end{document}Df= 2.56;\documentclass[12pt]{minimal}
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				\begin{document}$${\Delta h}_{dfrm}={\Delta h}_{dfrm}(x;y)$$\end{document}Δhdfrm=Δhdfrm(x;y),\documentclass[12pt]{minimal}
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				\begin{document}$${D}_{f}$$\end{document}Df= 2.68;\documentclass[12pt]{minimal}
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				\begin{document}$${\Delta h}_{stiff}={\Delta h}_{stiff}(x;y)$$\end{document}Δhstiff=Δhstiff(x;y),\documentclass[12pt]{minimal}
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				\begin{document}$${D}_{f }$$\end{document}Df= 2.42,\documentclass[12pt]{minimal}
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				\begin{document}$$A=A\left(x;y\right)$$\end{document}A=Ax;yand\documentclass[12pt]{minimal}
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				\begin{document}$${F}_{adh}={F}_{adh}(x;y)$$\end{document}Fadh=Fadh(x;y)) indicating its complex cavernous structure.