The Heat Equation: Our Test Case
We'll demonstrate inverse problems using 1D steady-state heat conduction:
\[ -k \frac{d^2T}{dx^2} = f(x), \quad x \in [0,1] \]
with boundary conditions: \( T(0) = T_0 \), \( T(1) = T_1 \)
Physical meaning:
- \( T(x) \) = temperature distribution
- \( k \) = thermal diffusivity (unknown parameter we want to find)
- \( f(x) \) = heat source term (known)
- Boundary conditions specify temperatures at the ends
Why This Problem?
- Physical relevance: Material property identification is crucial in engineering
- Mathematical simplicity: 1D steady-state allows clear visualization
- Exact solution available: We can verify our parameter recovery
- Well-studied: Benchmark for inverse methods
The Challenge
Scenario: You're an engineer testing a new material. You can:
- Apply known heat sources \( f(x) \)
- Control boundary temperatures
- Measure temperature at a few points
- Cannot directly measure thermal diffusivity \( k \)
Goal: Determine \( k \) from sparse, noisy temperature measurements
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Cornell University
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Center for Advanced Computing
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Copyright Statement
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Access Statement
CVW material development is supported by NSF OAC awards 1854828, 2321040, 2323116 (UT Austin) and 2005506 (Indiana University)
CVW material development is supported by NSF OAC awards 1854828, 2321040, 2323116 (UT Austin) and 2005506 (Indiana University)