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Biopotential electrodes A complex interface Summer School Timisoara 2002R. Hinz.

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Presentation on theme: "Biopotential electrodes A complex interface Summer School Timisoara 2002R. Hinz."— Presentation transcript:

1 Biopotential electrodes A complex interface Summer School Timisoara 2002R. Hinz

2 1 the interface I To sense a signal a current I must flow !

3 2 the interface problem I To sense a signal a current I must flow ! But no electron e - is passing the interface!

4 3 metal cation No current What’s going on? leaving into the electrolyte

5 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

6 5 metal cation What’s going on? No current joining the metal

7 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

8 7 half-cell voltage No current

9 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

10 9 electrode double layer No current ? ??

11 10 electrode double layer No current ? ?

12 11 electrode double layer No current ?

13 12 electrode double layer No current

14 13 current influence n withcurrent n with current flowing the half-cell voltage changes n n

15 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

16 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)

17 16 polarizable electrode displacement capacitor n “perfectly” polarizable electrode: - only displacement current, electrode behave like a capacitor n

18 17 polarizable electrode displacement capacitor n “perfectly” polarizable electrode: - only displacement current, electrode behave like a capacitor n example: noble metals like platinum Pt

19 18 nonpolarizable electrode overpotential n “perfectly” nonpolarizable electrode: -current passes freely across interface, -no overpotential n

20 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)

21 20 Question! n How is the current doing this to “pass freely”? Electrons can’t live in liquids! Can they?

22 21 chemical reactions silver / silver chloride

23 22 electrical behaviour equivalent circuit

24 23 electrical behaviour equivalent circuit ??

25 24 electrical behaviour equivalent circuit ?

26 25 electrical behaviour equivalent circuit

27 26 equivalent circuit electrode-electrolyte

28 27 body-surface electrode anatomy

29 28 again el. behaviour additional the skin: an additional interface! ??

30 29 again el. behaviour additional the skin: an additional interface! ?

31 30 again el. behaviour additional the skin: an additional interface!

32 31 again el. behaviour additional the skin: an additional interface!

33 32 expanded equiv. circuit dominating parts highlighted

34 33 total equivalent circuit simplified

35 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* :...

36 35 high impedance n interference with main power-lines (!!) n n c

37 36 high impedance n interference with main power-lines (!!) n potential devider with R input n c

38 37 high impedance n interference with main power-lines (!!) n potential devider with R input n frequency dependant. c

39 38 changing half-cell voltage n influenced by local concentration n

40 39 changing half-cell voltage n influenced by local concentration n saturation of amplifier n

41 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:

42 41 body-surface electrode half-cell voltage drift simulated

43 42 body-surface electrode impedance locus diagram


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