“…Let us consider a 2D EIT problem where Ω is the cross section of a human thorax probed by V electrodes displaced along its external perimeter (Figure ). EIT data are collected with the adjacent‐electrode‐pair strategy by successively applying a low‐frequency ( f < 100kHz) current to a pair of adjacent electrodes and measuring the arising impedance values on all remaining pairs of neighboring electrodes, the total number of independent measurements being M = V ( V − 3)/2. The DUT Ω is characterized by a real (purely resistive) conductivity distribution σ ( r ) piecewise constant within Q = 5 subregions {Γ q , q = 1, …, Q }, Ω = ∪ Γ q , modeling fat ( σ ( r ) = σ F ,∀ r ∈ Γ 1 ‐ Figure ), muscle ( σ ( r ) = σ M ,∀ r ∈ Γ 2 ‐ Figure 1), hearth ( σ ( r ) = σ H ,∀ r ∈ Γ 3 ‐ Figure 1) and left/right lungs ( σ ( r ) = σ L / R ,∀ r ∈ Γ 4/5 ‐ Figure 1), respectively.…”