Author Adler A. Institution Sch. of Inf. Technol. & Eng., Ottawa Univ., Ont., Canada. Title Accounting for missing electrode data in electrical impedance tomography Source Conference Information 4th Conference on Biomedical Applications of Electrical Impedance Tomography UMIST, Manchester April 23-25 2003. Abstract An unfortunate, but not unusual, occurrence in experimental measurements with Electrical Impedance Tomography, is electrodes which become detached or poorly connected, such that the measured data cannot be used. We propose an image reconstruction methodology which allows use of the remaining good measurements. A finite element model of the EIT dynamic imaging forward problem is linearized as z=Hx, where z is the vector change in measurements and x the vector of change in finite element log conductivities. Image reconstruction is represented in terms of a Maximum a Posteriori (MAP) estimate as x=inv(H'*inv(Rn)*H + inv(Rx))*H'*inv(Rn)*z, where (') represents the transpose operator, and Rx and Rn represent the a priori estimates of image and measurement noise cross correlations, respectively. Using this formulation, missing electrode data can be naturally modelled as infinite noise on all measurements using the corresponding electrodes. Simulations were conducted of a small contrasting target at different radial positions as a function of the position of the problem electrode. Contrast position error, point spread function, and total image amplitude were calculated. All values are close (±10%) to those calculated without missing electrode data as long as the target was further from the problem electrode than 10% of the medium diameter. When the target was closer than this limit, all error values increased significantly, but the reconstructed image still represented a reasonable "best effort". Application of this technique to experimental data shows similar results. In comparison, simulations were made of the simple approach of setting measurements from problem electrodes to zero. Results show significant errors for targets 25% of the medium diameter from the electrode. The increase in point spread function size above the value for no electrode errors was three times greater for this simple approach than for the MAP estimate.