1D Heat equation, numerical solution with ONLY one heat source

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SUMMARY

The discussion focuses on numerically solving the 1D heat equation for a metal bar of length L using the forward time, centered space (FTCS) method. The user encounters a challenge in calculating the temperature at the end of the bar (L-deltaX) due to the presence of only one heat source at one end. The solution requires the implementation of an additional boundary condition, such as a fixed temperature, convection coefficient, or heat flux, to accurately compute the temperature at the bar's end.

PREREQUISITES
  • Understanding of the 1D heat equation
  • Familiarity with numerical methods, specifically the FTCS method
  • Knowledge of boundary conditions in heat transfer problems
  • Basic concepts of thermal conduction and heat sources
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Students and professionals in thermal engineering, applied mathematics, and computational physics who are working on heat transfer simulations and numerical methods for solving differential equations.

gifuboy
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Hi,

I have the following problem.
I am tried to numerically solve the 1D heat equation for a metal bar of length L.

Using the forward time, centered space equation

a(t+1) = a(t)+(alpha*deltaA/(deltaX)^2)*(a(x+1,t)-2*a(x,t)+a(x-1,t))

The problem is that I only have ONE heat source at one end of the bar(0), there is nothing at the end of the bar. How do I calculate a(t+1) at L-deltaX? (end of the bar). The above equation is dependent on a(x+1,t), how do I calculate a(t+1,L-deltaX)?

Thanks.
 
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Hi gifuboy, welcome to PF. You need another boundary condition at the end of the bar (e.g., a certain temperature, a certain convection coefficient, a certain heat flux, etc.).
 

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