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Published byRussell Briggs Modified over 8 years ago
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BRAIN TISSUE IMPEDANCE ESTIMATION
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Improve the Brain’s Evoked Potential’s source Temporal and Spatial Inverse Problem Improve the Brain Tissue Impedance value ranges
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ASSUMPTION S Linearity of the System All channels have the same frequency The input current signal is sinusoidal
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ASSUMPTIONS (cont.) The systems noise is a white noise at a maximum SNR of 10[dB] The tissue impedance can be characterized by a RC filter
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ASSUMPTIONS (cont.) The tissue impedance is complex The tissue conductivity is anisotropy
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ASSUMPTIONS (cont.) The tissue conductivity remains the same through out the experiment. The passing time and the heat, caused as a result of the current flow through the tissue, do not effect the conductivity.
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I(t) Impedance = Noise Perpendicular Conductivity V(t) System Identification Optimization Tissue Simulation Tissue Simulation
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I(t)V(t) Tissue Simulation Tissue Simulation Generating current - the system input Calculating voltage - the measured output Based on the mathematical model:
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Mathematical Model
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Input & Output Signals SignalNoise - SNR 10 [dB] Channel 1 Channel 2 Channel 3 InputsOutputs
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I(t) Impedance = Noise V(t) System Identification Black box deciphering
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A good abstract model, which can describe the system, is: UY e
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Impedance Amplitude Channel 1 Channel 2 Channel 3 Impedance Phase Simulated valueEstimated valueUpper ToleranceLower Tolerance Impedance Estimation
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Impedance = Perpendicular Conductivity Optimization The optimization concerns finding a parameters that minimize the mathematical model function
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Optimization Sensitivity Points Unless the function is continuous and has one minimum only, there is no guarantee that the minimum achieved is the global minimum. Starting points dispersal
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Estimated Parameters Simulated ValueEstimated Value Parameter AmplitudeParameter Phase
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Perpendicular Conductivity Optimization I(t)V(t) Tissue Simulation Tissue Simulation Impedance = Noise System Identification
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NOISE TIME HEAT HARDWARE
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Sampling Noise I(t) Impedance = Perpendicular Conductivity V(t) System Identification Optimization Experimental System Experimental System
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R1R1 R2R2 R3R3 AmplitudePhase Short Results
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Parameter AmplitudeParameter Phase Short impedance estimation
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Impedance AmplitudeImpedance Phase R3 R1 R2
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Parameter AmplitudeParameter Phase Tissue impedance estimation
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Conclusions and Future Improvements : There is a problem some where along the estimation process. The problem could be at any of the stages of signal collection or signal analysis. Future option: replacing the input sinusoidal signal with a white noise signal. The Optimization is the weakest link in the estimation chain. The estimation time and complexity may be reduced with a different algorithm.
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