A Two Dimensional Backward Heat Problem With Statistical Discrete Data

preprint2016arXivOpen access

Abstract

In this paper, we focus on the backward heat problem of finding the function θ(x,y)=u(x,y,0)θ(x,y)=u(x,y,0) such that \[ {l l l} u_t - a(t)(u_{xx} + u_{yy}) & = f(x,y,t), & \qquad (x,y,t) \in Ω\times (0,T), u(x,y,T) & = h(x,y), & \qquad (x,y) \in\barΩ. \] where Ω=(0,π)×(0,π)Ω= (0,π) \times (0,π) and the heat transfer coefficient a(t)a(t) is known. In our problem, the source f=f(x,y,t)f = f(x,y,t) and the final data h(x,y)h(x,y) are unknown. We only know random noise data gij(t)g_{ij}(t) and dijd_{ij} satisfying the regression models g_{ij}(t) &=& f(x_i,y_j,t) + \varthetaξ_{ij}(t), d_{ij} &=& h(x_i,y_j) + σ_{ij}ε_{ij}, where ξij(t)ξ_{ij}(t) are Brownian motions, εij∼N(0,1)ε_{ij}\sim \mathcal{N}(0,1), (xi,yj)(x_i,y_j) are grid points of ΩΩ and σij,ϑσ_{ij}, \vartheta are unknown positive constants. The noises ξij(t),εijξ_{ij}(t), ε_{ij} are mutually independent. From the known data gij(t)g_{ij}(t) and dijd_{ij}, we can recovery the initial temperature θ(x,y)θ(x,y). However, the result thus obtained is not stable and the problem is severely ill--posed. To regularize the instable solution, we use the trigonometric method in nonparametric regression associated with the truncated expansion method. In addition, convergence rate is also investigated numerically.

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