Lecture on Cell Potential

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This study allows for students in biomedical engineering to view the mechanisms of cells and how they respond to electrical stimuli in the body. The student is to read the document and then use this to broaden their understanding of how cells interact in a chemical-electrical environment.

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  • BME 313 Bioinstrumentation Instructor: Wei Lin

    BiopotentialBiopotentials are the results of electrochemical activities of excitable cells, which are the components of nervous, muscular or glandular tissue.

    Na+: 10 times higher outside than insideK+: 40 times greater inside than outsideCl-: 30 times higher outside than inside

  • Biopotential

    BME 313 Bioinstrumentation Instructor: Wei Lin

    Cell membrane potential is the difference between intercellular potential and extracellular potential.

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Biopotential

    i

    ok K

    KnFRTE

    ][][

    ln

    Nernst Equation:

    Goldman Equation:

    oCliNaik

    iCloNaok

    ClPNaPkPClPNaPkP

    FRTE

    ][][][][][][

    ln

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    State of Excitable Cell

    There are two states of the excitable cell:

    Images from http://www.gregalo.com/action_potential.jpg

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Propagation of Action Potential

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Propagation of Action Potential

    Myelinated transduction

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Volume Conductor

    http://www.cvphysiology.com/Arrhythmias/A014.htm

    The three dimensional conducting medium composed of tissue is referred as volume conductor. The source of electrical signals are the excitable cells serving the current sources.

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Electrocardiogram (ECG)

    Sinoatrial node (SA)

    Atrioventrical Node (AV)

    Bundle of His

    Rest of the heart

    Common Bundle

    Purkinje fiber

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Electrocardiogram (ECG)

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Electroencephalogram (EEG)

    EEG is the electrical activity of the brain. EEG can be recorded using three

    different types of electrodes Scalp electrodes Cortical electrodes (electrocorticogram) Depth electrodes

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Types of EEG (Alpha waves)

    Alpha waves are rhythmic waves in the frequency range of 8-12 Hz arising from synchronous and coherent (in phase / constructive) electrical activity of large groups of neurons in the human brain. They are found in EEGs when a normal person is in a quiet, resting state and are most intense in the occipital area.

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Types of EEG (beta waves)

    Beta waves normally occur in the frequency range of 14 to 30 Hz and could be as high as 50Hz during intense mental activity.

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Types of EEG (theta waves)

    Theta waves have frequency range of 4 to 7 Hz. They mainly occur in the parietal and temporal regions in children. They can also occur in adults during emotional stress.

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Types of EEG (delta waves)Delta waves include all the waves in EEG below 3.5 Hz. They occur in deep sleep, in infancy and in serious organic brain disease.

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Other Biopotentials

    Electromyogram (EMG): electrical activities of skeletal muscle.

    Electroretinogram (ERG): electrical activities of retina stimulated with light.

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Biopotential Electrode

    Electrode/Electrolyte interface Half cell potential Polarization of electrode Electrode circuit model.

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Biopotential Electrodes

    The electrode consists of metallic atoms C. The electrolyte is an aqueous solution containing cations of the electrode metal C+ and anions A-.

    C

    CC A-

    A-C+

    C+

    e-

    e-

    Electrode Electrolyte

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Electrode Electrolyte Interface

    Assuming the electrode has same material as cation in the electrolyte, the electrode material becomes oxidized to form a cation and one or more electrons. The electrons remain as the charge carrier in the electrode. The anion can also be oxidized at the electrode to form a neutral atom and release one or two electrons to the electrode. The reverse of the above reaction is reduction. It controls the movement of electrons in the opposite direction.

    C Cn+ + ne-

    Am- A + me-

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Half-cell Potential

    When the electrode is inserted into the electrolyte, the concentration of cations and anions at the interface changes. As the result, there is an electric potential difference between the electrolyte surrounding the electrode and the electrolyte in other places. The difference is called half-cell potential, which cannot be measured.

    +

    +

    +

    +

    +

    +

    +

    Electrode

    Electrolyte

    Half-cell potential

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Polarization

    When current passes through the electrode-electrolyte interface, it changes the half-cell potential. The change is called overpotential and it has three components

    Ohmic overpotential

    Concentration overpotential

    Activation overpotential

    + Total overpotential

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Nernst Equation

    BA

    DC

    aaaa

    nFRTEE ln0

    When two aqueous ionic solutions of different concentration are separated by an ion-selective semi-permeable membrane, an electric potential exists across the membrane and is given by Nernst equation.

    For the general oxidation-reduction reaction: neDCBA

    Where E : Half Cell PotentialE0 : Standard Half Cell Potential a : activity of cationsn : Number of electrons

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Polarizable and Non-Polarizable Electrodes

    Perfectly Polarizable Electrodes No actual charge crosses the electrode-electrolyte

    interface when a current is applied. The current across the interface is a displacement current and the electrode behaves like a capacitor.

    Perfectly Nonpolarizable Electrode Current passes freely across the electrode-

    electrolyte interface, requiring no energy to make the transition. These electrodes see no overpotentials.

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Silver/Silver Chloride Electrode

    eAgAg AgClClAg

    Cl

    sAg a

    KnFRTEE ln0

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Equivalent Circuit Model for Electrode

    Ehc

    Rd

    Cd

    Rs

    Ehc: half cell potentialRd and Cd: the impedance associated with the electrode-electrolyte interfaceRs: the series resistance associated with interface effects and the resistance in the electorlyte.

  • BME 313 Bioinstrumentation Instructor: Wei Lin

    Electrode Skin Interface and Motion Artifact

  • Surface electrode

    BME 313 Bioinstrumentation Instructor: Wei Lin

  • Micro electrode

    BME 313 Bioinstrumentation Instructor: Wei Lin

  • Electrode Arrays

    BME 313 Bioinstrumentation Instructor: Wei Lin

  • Electric stimulation of Tissue

    BME 313 Bioinstrumentation Instructor: Wei Lin