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Biopotential electrodes A complex interface Summer School Timisoara 2002R. Hinz
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1 the interface I To sense a signal a current I must flow !
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2 the interface problem I To sense a signal a current I must flow ! But no electron e - is passing the interface!
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3 metal cation No current What’s going on? leaving into the electrolyte
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4 metal cation No current One atom M out of the metal is oxidized to form one cation M + and giving off one free electron e - to the metal. leaving into the electrolyte
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5 metal cation What’s going on? No current joining the metal
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6 metal cation One cation M + out of the electrolyte becomes one neutral atom M taking off one free electron from the metal. No current joining the metal
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7 half-cell voltage No current
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8 half-cell voltage No current metal: Li Al Fe Pb H Ag/AgCl Cu Ag Pt Au V h / Volt -3,0 negativ 0 0,223 positiv 1,68
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9 electrode double layer No current ? ??
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10 electrode double layer No current ? ?
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11 electrode double layer No current ?
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12 electrode double layer No current
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13 current influence n withcurrent n with current flowing the half-cell voltage changes n n
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14 current influence n withcurrent n with current flowing the half-cell voltage changes overpotentialpolarization: n this voltage change is called overpotential or polarization: n
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15 current influence n withcurrent n with current flowing the half-cell voltage changes overpotentialpolarization: n this voltage change is called overpotential or polarization: n V p = V r + V c + V a activation, depends on direction of reaction concentration (change in double layer) ohmic (voltage drop)
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16 polarizable electrode displacement capacitor n “perfectly” polarizable electrode: - only displacement current, electrode behave like a capacitor n
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17 polarizable electrode displacement capacitor n “perfectly” polarizable electrode: - only displacement current, electrode behave like a capacitor n example: noble metals like platinum Pt
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18 nonpolarizable electrode overpotential n “perfectly” nonpolarizable electrode: -current passes freely across interface, -no overpotential n
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19 nonpolarizable electrode overpotential n “perfectly” nonpolarizable electrode: -current passes freely across interface, -no overpotential n examples: -silver/silver chloride (Ag/AgCl), -mercury/mercurous chloride (Hg/Hg 2 Cl 2 ) (calomel)
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20 Question! n How is the current doing this to “pass freely”? Electrons can’t live in liquids! Can they?
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21 chemical reactions silver / silver chloride
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22 electrical behaviour equivalent circuit
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23 electrical behaviour equivalent circuit ??
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24 electrical behaviour equivalent circuit ?
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25 electrical behaviour equivalent circuit
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26 equivalent circuit electrode-electrolyte
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27 body-surface electrode anatomy
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28 again el. behaviour additional the skin: an additional interface! ??
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29 again el. behaviour additional the skin: an additional interface! ?
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30 again el. behaviour additional the skin: an additional interface!
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31 again el. behaviour additional the skin: an additional interface!
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32 expanded equiv. circuit dominating parts highlighted
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33 total equivalent circuit simplified
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34 results n high impedance Z E n high impedance Z E :... n changing half-cell voltage V h* n changing half-cell voltage V h* :...
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35 high impedance n interference with main power-lines (!!) n n c
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36 high impedance n interference with main power-lines (!!) n potential devider with R input n c
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37 high impedance n interference with main power-lines (!!) n potential devider with R input n frequency dependant. c
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38 changing half-cell voltage n influenced by local concentration n
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39 changing half-cell voltage n influenced by local concentration n saturation of amplifier n
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40 changing half-cell voltage n influenced by local concentration n saturation of amplifier n motion artefacts by changing the the gel-skin potential (V ep ). simulation:
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41 body-surface electrode half-cell voltage drift simulated
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42 body-surface electrode impedance locus diagram
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