2010
DOI: 10.1109/titb.2009.2036010
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Absolute Electrical Impedance Tomography (aEIT) Guided Ventilation Therapy in Critical Care Patients: Simulations and Future Trends

Abstract: ReuseUnless indicated otherwise, fulltext items are protected by copyright with all rights reserved. The copyright exception in section 29 of the Copyright, Designs and Patents Act 1988 allows the making of a single copy solely for the purpose of non-commercial research or private study within the limits of fair dealing. The publisher or other rights-holder may allow further reproduction and re-use of this version -refer to the White Rose Research Online record for this item. Where records identify the publish… Show more

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Cited by 32 publications
(27 citation statements)
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“…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.…”
Section: Forward Eit Problemmentioning
confidence: 99%
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“…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.…”
Section: Forward Eit Problemmentioning
confidence: 99%
“…To numerically solve the forward problem (ie, the computation of the electrodes impedances), the finite‐element method (FEM) is used by partitioning Ω into N triangular mesh cells. Moreover, under the low‐frequency approximation, the potential distribution produced by the injected currents and affected by the conductivity distribution of the DUT is computed with the Poisson equation and the electrodes impedances, trueZ¯={};,,Zmm=1..M, are determined as. trueZ¯=normalΨ()σfalse¯ where trueσ¯={};,,σ()boldrnn=1N and Ψ(. ) is the forward EIT‐FEM operator.…”
Section: Forward Eit Problemmentioning
confidence: 99%
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“…One step further, information on regional distribution of ventilation might be fused with other relevant parameters such as blood gas values and thus being the basis for a computerized advisory system facilitating the application of the least injurious ventilation [7 ].…”
Section: Open Questions and Future Developments Of Electrical Impedanmentioning
confidence: 99%