Determination of unknown shear force in transverse dynamic force microscopy from measured final data

Author:

Baysal Onur1,Hasanov Alemdar2,Kumarasamy Sakthivel3

Affiliation:

1. Department of Mathematics , University of Malta , Msida , Malta

2. Department of Mathematics , Kocaeli University , Izmit - Kocaeli ; and Şehit Ekrem Dsitrict, Altunşehir Str., Ayazma Villalari, No: 22. Bahčecik - Başiskele, Kocaeli, 41030 Türkiye

3. Department of Mathematics , Indian Institute of Space Science and Technology (IIST) , Trivandrum , India

Abstract

Abstract In this paper, we present a new methodology, based on the inverse problem approach, for the determination of an unknown shear force acting on the inaccessible tip of the microcantilever, which is a key component of transverse dynamic force microscopy (TDFM). The mathematical modelling of this phenomenon leads to the inverse problem of determining the shear force g ( t ) {g(t)} acting on the inaccessible boundary x = {x=\ell} in a system governed by the variable coefficient Euler–Bernoulli equation ρ A ( x ) u t t + μ ( x ) u t + ( r ( x ) u x x + κ ( x ) u x x t ) x x = 0 , ( x , t ) ( 0 , ) × ( 0 , T ) , \rho_{A}(x)u_{tt}+\mu(x)u_{t}+(r(x)u_{xx}+\kappa(x)u_{xxt})_{xx}=0,\quad(x,t)% \in(0,\ell)\times(0,T), subject to the homogeneous initial conditions and the boundary conditions u ( 0 , t ) = u 0 ( t ) , u x ( 0 , t ) = 0 , ( u x x ( x , t ) + κ ( x ) u x x t ) x = = 0 , ( - ( r ( x ) u x x + κ ( x ) u x x t ) x ) x = = g ( t ) , u(0,t)=u_{0}(t),\quad u_{x}(0,t)=0,\quad(u_{xx}(x,t)+\kappa(x)u_{xxt})_{x=\ell% }=0,\quad\bigl{(}-(r(x)u_{xx}+\kappa(x)u_{xxt})_{x}\bigr{)}_{x=\ell}=g(t), from the final time measured output (displacement) u T ( x ) := u ( x , T ) {u_{T}(x):=u(x,T)} . We introduce the input-output map ( Φ g ) ( x ) := u ( x , T ; g ) {(\Phi g)(x):=u(x,T;g)} , g 𝒢 {g\in\mathcal{G}} , and prove that it is a compact and Lipschitz continuous linear operator. Then we introduce the Tikhonov functional J ( F ) = 1 2 Φ g - u T L 2 ( 0 , ) 2 J(F)=\frac{1}{2}\lVert\Phi g-u_{T}\rVert_{L^{2}(0,\ell)}^{2} and prove the existence of a quasi-solution of the inverse problem. We derive a gradient formula for the Fréchet gradient of the Tikhonov functional through the corresponding adjoint problem solution and prove that it is a Lipschitz continuous functional. The results of the numerical experiments clearly illustrate the effectiveness and feasibility of the proposed approach.

Funder

National Board for Higher Mathematics

Publisher

Walter de Gruyter GmbH

Subject

Applied Mathematics

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