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?

  1. Physical relevance: Material property identification is crucial in engineering
  2. Mathematical simplicity: 1D steady-state allows clear visualization
  3. Exact solution available: We can verify our parameter recovery
  4. 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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CVW material development is supported by NSF OAC awards 1854828, 2321040, 2323116 (UT Austin) and 2005506 (Indiana University)