2017
DOI: 10.1088/1361-6420/aa648c
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Parameter identification in a semilinear hyperbolic system

Abstract: We consider the identification of a nonlinear friction law in a one-dimensional damped wave equation from additional boundary measurements. Well-posedness of the governing semilinear hyperbolic system is established via semigroup theory and contraction arguments. We then investigte the inverse problem of recovering the unknown nonlinear damping law from additional boundary measurements of the pressure drop along the pipe. This coefficient inverse problem is shown to be ill-posed and a variational regularizatio… Show more

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Cited by 9 publications
(8 citation statements)
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“…For the well-posedness and the regularity of the solution of the system (5)-(6), we refer to [9]. More advanced numerical schemes for hyperbolic PDEs, such as the total variation diminishing (TVD) method [40], or the discontinuous Galerkin method (DG) [24], could be implemented at the next step of our research to investigate more complicated dynamics of the gas networks.…”
Section: 2mentioning
confidence: 99%
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“…For the well-posedness and the regularity of the solution of the system (5)-(6), we refer to [9]. More advanced numerical schemes for hyperbolic PDEs, such as the total variation diminishing (TVD) method [40], or the discontinuous Galerkin method (DG) [24], could be implemented at the next step of our research to investigate more complicated dynamics of the gas networks.…”
Section: 2mentioning
confidence: 99%
“…Note that the nonlinear term q|q| p which describes the damping law of gas networks is still differentiable with respect to the change of the flow direction. For details of the regularity of the solution (p, q) of the PDE (5), we refer to Theorem 3.2 given in [9]. It is also pointed out by Theorem 4.3 in [9] that the forward PDE operator of (5) is Fréchet differentiable with Lipschitz continuous derivative.…”
Section: 2mentioning
confidence: 99%
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“…We are concerned with the construction of special series solutions of a classical one dimensional semilinear wave equation defined by {arrayutt=uxx+au+λu20xπandt>0.arrayux(0,t)=ux(π,t)=0arrayu(x,0)=f(x)arrayut(x,0)=g(x) Equation models the damping vibration of a string and also the propagation of pressure waves in a gas pipeline, where λ u 2 accounts for the friction against the pipe walls. The nonlinearity is known to cause finite time blowup, for example ufalse(x,tfalse)=1()0.1emt0.1emT2 is such a solution in case a =0 and λ = 6.…”
Section: Introductionmentioning
confidence: 99%
“…(1) Equation 1 models the damping vibration of a string and also the propagation of pressure waves in a gas pipeline, 1 where u 2 accounts for the friction against the pipe walls. The nonlinearity is known to cause finite time blowup, for example u(x, t) = 1 ( t− T) 2 is such a solution in case a = 0 and = 6.…”
Section: Introductionmentioning
confidence: 99%