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Published byRandell Dalton Modified over 9 years ago
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Presenter : Yu-Chun Hua Presenter : Yu-Chun Hua Adviser : Dr. Ji-Jer Huang Adviser : Dr. Ji-Jer Huang Date : 99.12.09 Date : 99.12.09
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D. Boundary Potentials Measurements A 1 mA, 50 kHz constant current signal is injected to the phantom boundary The surface potentials developed are measured using neighboring method of electrode switching protocol Boundary data measurement with practical biological phantom
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D. Boundary Potentials Measurements Boundary potentials are also measured for a phantom with and without extra water column above and below the electrode array level. The measured potential data are compared with the calculated potential data. Boundary data measurement with a phantom having extra water column above and below the electrode array level.
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Paper review(2) results The differential potential is calculated using our forward solver with the phantom specifications provided by Ider et al Vds Curve Compared with Ider et al Data
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Paper review(2) results Vds: surface potential Vdm: measured data = differential potential CME: Common Mode Electrode CGE : Central Ground Electrode Vdm data with and with CGE after Calibration
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Materials and Methods System Block diagram
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Future works Paper review Build a hardware howland circuit Modified EIT system (digital control)
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References [1] R. A. Stiz, P. Bertemes-Filho, A. Ramos, V. C. Vincence. “Wide Band Howland Bipolar Current Source using AGC Amplifier “IEEE LATIN AMERICA TRANSACTIONS, VOL. 7, NO. 5, SEPTEMBER 2009 [2] From: Tushar Kanti Bera and J. Nagaraju ﹐ ” A Simple Instrumentation Calibration Technique for Electrical Impedance Tomography (EIT) Using A 16- Electrode Phantom ” 5th Annual IEEE Conference on Automation Science and Engineering Bangalore, India, August 22-25, 200
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