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Published byVirgil Sanders Modified over 9 years ago
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Creed Reilly, Sophomore, Engineering Advisor: Professor Anna Mazzucato Graduate Student: Yajie Zhang
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Diffusion coefficient c jumps at x=1/2 (the interface). Impose transmission conditions at interface. Solve equation in [0,1]. Impose Dirichlet boundary conditions at x=0,1. Initial condition is sin(πx). General Heat Equation in 1 Dimension with Transmission Condition
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Model Composite Materials:
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This is the simplest (explicit) first-order finite difference method to solve the heat equation. First order Taylor expansion was used for the time derivative (U t ) The center-difference method was used for the second space derivative (U xx ) Because this is an explicit method, a convergence condition had to be observed:
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C L =1C R =2Δx=0.1C L =1C R =2Δx=0.025
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ΔxL2(1)Linf(1)L2(2)Linf(2)LogE 0.13.03E-094.51E-094.05E-096.02E-09-0.42206 0.054.05E-096.02E-093.29E-094.89E-090.302807 0.0253.29E-094.89E-092.09E-093.10E-090.65612 0.01252.09E-093.10E-091.17E-091.74E-090.829307 0.006251.17E-091.74E-096.23E-109.24E-100.915078 0.0031256.23E-109.24E-10No Mem N/A Table 1: L2 and L∞ error for various displacement steps Graph 1: Diffusion of energy when the left half has a C=1 and the right has a C=2. Graph 2: Diffusion of energy when the left half has a C=1 and the right has a C=100.
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