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2D Axisymmetric Heat Transfer Problem with uniform Neumann BCs

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Statement of the Problem

This test corresponds to a 2D axisymmetric simulation of heat transfer in a solid. The domain Ω\Omega is an axisymmetric domain [0,1]×[0,1][0,1]\times[0,1]. The axis of symmetry is located at r=0r=0.

ρCpTt=kT+S(r,z,t) in Ω \begin{align} \rho C_p\frac{\partial T}{\partial t}&=\nabla \cdot k \nabla T + S(r,z,t)\text{ in }\Omega \end{align}

In equation (1), S(r,z,t)S(r,z,t) is the source term allowing the exact solution:

T(r,z,t)=etcos(πr2)cos(πz)z \begin{align} T(r,z,t) &= e^{-t} cos (\pi r^2) cos(\pi z) - z \end{align}

A convergence analysis is carried out to ensure the consistency of the results.

Initial condition

The initial condition is given by:

T(r,z)=cos(πr2)cos(πz)z \begin{align} T(r,z) &= cos (\pi r^2) \cos(\pi z) - z \end{align}

Boundary Conditions

  • Uniform Neumann boundary conditions are prescribed on the upper and lower surfaces.

nkT=1 on ΓbottomnkT=1 on Γtop \begin{align} {\bf{n}} \cdot{} k \nabla T &= 1 \text{ on }\Gamma_{bottom} \\[6pt] {\bf{n}} \cdot{} k \nabla T &= -1 \text{ on }\Gamma_{top} \end{align}

  • Homogeneous Neumann boundary conditions are prescribed on the left and right boundaries.

nkT=0 on Γleft and Γright \begin{align} {\bf{n}} \cdot{} k \nabla T &= 0 \text{ on } \Gamma_{left} \text{ and } \Gamma_{right} \end{align}

Parameters Used for the Test

For this test, all physical parameters are equal to one.

Numerical Scheme

  • Time integration: Euler Implicit over the interval t[0,0.01]t\in[0,0.01] with a time-step δt=103\delta t=10^{-3}.
  • Spatial discretization for convergence analysis: uniform grid with N=30,60,90,120N={30, 60, 90, 120} nodes in each spatial direction, with Q1\mathcal{Q}_1

Results

Figures 1 shows the results of convergence analysis with Q1\mathcal{Q}_1.

MMS_heat
Figure 1: convergence analysis with Q1\mathcal{Q}_1 finite elements