Cylindrical Domain

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Berikbol T Torebek - One of the best experts on this subject based on the ideXlab platform.

Jorge Ferreira - One of the best experts on this subject based on the ideXlab platform.

  • a reaction diffusion model for a class of nonlinear parabolic equations with moving boundaries existence uniqueness exponential decay and simulation
    Applied Mathematical Modelling, 2014
    Co-Authors: Rui Robalo, Rui M P Almeida, Maria Do Carmo Coimbra, Jorge Ferreira
    Abstract:

    Abstract The aim of this paper is to establish the existence, uniqueness and asymptotic behaviour of a strong regular solution for a class of nonlinear equations of reaction–diffusion nonlocal type with moving boundaries: u t - a ∫ Ω t u ( x , t ) dx u xx = f ( x , t ) , ( x , t ) ∈ Q t , u ( α ( t ) , t ) = u ( β ( t ) , t ) = 0 , t > 0 , u ( x , 0 ) = u 0 ( x ) , x ∈ Ω 0 = ] α ( 0 ) , β ( 0 ) [ , where Q t is a bounded non-Cylindrical Domain defined by Q t = ( x , t ) ∈ R 2 : α ( t ) x β ( t ) , for all 0 t T . Moreover, we study the properties of the solution and implement a numerical algorithm based on the Moving Finite Element Method (MFEM) with polynomial approximations of any degree, to solve this class of problems. Some numerical tests are investigated to evaluate the performance of our Matlab code based on the MFEM and illustrate the exponential decay of the solution.

Tomasz Piasecki - One of the best experts on this subject based on the ideXlab platform.

  • on an inhomogeneous slip inflow boundary value problem for a steady flow of a viscous compressible fluid in a Cylindrical Domain
    Journal of Differential Equations, 2010
    Co-Authors: Tomasz Piasecki
    Abstract:

    Abstract We investigate a steady flow of a viscous compressible fluid with inflow boundary condition on the density and inhomogeneous slip boundary conditions on the velocity in a Cylindrical Domain Ω = Ω 0 × ( 0 , L ) ∈ R 3 . We show existence of a solution ( v , ρ ) ∈ W p 2 ( Ω ) × W p 1 ( Ω ) , p > 3 , where v is the velocity of the fluid and ρ is the density, that is a small perturbation of a constant flow ( v ¯ ≡ [ 1 , 0 , 0 ] , ρ ¯ ≡ 1 ). We also show that this solution is unique in a class of small perturbations of ( v ¯ , ρ ¯ ) . The term u ⋅ ∇ w in the continuity equation makes it impossible to show the existence applying directly a fixed point method. Thus in order to show existence of the solution we construct a sequence ( v n , ρ n ) that is bounded in W p 2 ( Ω ) × W p 1 ( Ω ) and satisfies the Cauchy condition in a larger space L ∞ ( 0 , L ; L 2 ( Ω 0 ) ) what enables us to deduce that the weak limit of a subsequence of ( v n , ρ n ) is in fact a strong solution to our problem.

  • on an inhomogeneous slip inflow boundary value problem for a steady flow of a viscous compressible fluid in a Cylindrical Domain
    arXiv: Mathematical Physics, 2009
    Co-Authors: Tomasz Piasecki
    Abstract:

    We investigate a steady flow of a viscous compressible fluid with inflow boundary condition on the density and inhomogeneous slip boundary conditions on the velocity in a Cylindrical Domain $\Omega = \Omega_0 \times (0,L) \in \mathbb{R}^3$. We show existence of a solution $(v,\rho) \in W^2_p(\Omega) \times W^1_p(\Omega)$, where $v$ is the velocity of the fluid and $\rho$ is the density, that is a small perturbation of a constant flow $(\bar v \equiv [1,0,0], \bar \rho \equiv 1)$. We also show that this solution is unique in a class of small perturbations of $(\bar v,\bar \rho)$. The term $u \cdot \nabla w$ in the continuity equation makes it impossible to show the existence applying directly a fixed point method. Thus in order to show existence of the solution we construct a sequence $(v^n,\rho^n)$ that is bounded in $W^2_p(\Omega) \times W^1_p(\Omega)$ and satisfies the Cauchy condition in a larger space $L_{\infty}(0,L;L_2(\Omega_0))$ what enables us to deduce that the weak limit of a subsequence of $(v^n,\rho^n)$ is in fact a strong solution to our problem.

Danillo Silva De ,oliveira - One of the best experts on this subject based on the ideXlab platform.

  • Heat conduction equation solution in the presence of a change of state in a bounded axisymmetric Cylindrical Domain
    'Universidade de Sao Paulo Agencia USP de Gestao da Informacao Academica (AGUIA)', 2019
    Co-Authors: Danillo Silva De ,oliveira
    Abstract:

    O problema da condução de calor, envolvendo mudança de fase, foi resolvido para o caso de uma cavidade limitada por duas superfícies cilíndricas indefinidamente longas. As condições de contorno impostas consistem em manter a temperatura da superfície interna fixa e abaixo da temperatura de fusão do material que preenche a cavidade, enquanto que a temperatura da superfície externa é mantida fixa e acima da temperatura de fusão. Como condição inicial se fixou a temperatura de todo o material que preenche a cavidade no valor da temperatura da superfície externa. A solução obtida consiste em duas soluções da equação de condução de calor, uma escrita para o material solidificado e outra escrita para o material em estado líquido. As duas soluções são formalmente escritas em termos da posição da frente de mudança de fase, que é representada por uma superfície cilíndrica com raio em expansão dentro da cavidade. A posição dessa superfície é, a princípio, desconhecida e é calculada impondo o balanço de energia através da frente da mudança de fase. O balanço de energia é expresso por uma equação diferencial de primeira ordem, cuja solução numérica fornece a posição da frente como função do tempo. A substituição da posição da frente de mudança de fase em um instante particular, nas soluções da equação de condução de calor, fornece a temperatura nas duas fases naquele instante. A solução obtida é ilustrada através de exemplos numéricos.The heat conduction problem, in the presence of a change of state, was solved for the case of an indefinitely long Cylindrical layer cavity. As boundary conditions it is imposed that the internal surface of the cavity is maintained below the fusion temperature of the infilling substance and the external surface is kept above it. The solution, obtained in non-dimensional variables, consists in two closed form heat conduction equation solutions for the solidified and liquid regions, which formally depend of the, at first, unknown position of the phase change front. The energy balance through the phase change front furnishes the equation for time dependence of the front position, which is numerically solved. Substitution of the front position for a particular instant in the heat conduction equation solutions gives the temperature distribution inside the cavity at that moment. The solution is illustrated with numerical examples

  • heat conduction equation solution in the presence of a change of state in a bounded axisymmetric Cylindrical Domain
    Journal of Heat Transfer-transactions of The Asme, 2011
    Co-Authors: Danillo Silva De ,oliveira, Fernando Brenha Ribeiro
    Abstract:

    The heat conduction problem, in the presence of a change of state, was solved for the case of an indefinitely long Cylindrical layer cavity. As boundary conditions, it is imposed that the internal surface of the cavity is maintained below the fusion temperature of the infilling substance and the external surface is kept above it. The solution, obtained in nondimensional variables, consists in two closed form heat conduction equation solutions for the solidified and liquid regions, which formally depend of the, at first, unknown position of the phase change front. The energy balance through the phase change front furnishes the equation for time dependence of the front position, which is numerically solved. Substitution of the front position for a particular instant in the heat conduction equation solutions gives the temperature distribution inside the cavity at that moment. The solution is illustrated with numerical examples.

Enrico Valdinoci - One of the best experts on this subject based on the ideXlab platform.