Biopotential: An electric potential that is measured between points in living cells, tissues, and organisms, and which accompanies all biochemical processes.
Also describes the transfer of information between and within cells
This book focuses strictly on the measurement of potentials
Mechanism behind biopotentials 1/2
Concentration of potassium (K + ) ions is 30-50 times higher inside as compared to outside
Sodium ion (Na + ) concentration is 10 times higher outside the membrane than inside
In resting state the member is permeable only for potassium ions
Potassium flows outwards leaving an equal number of negative ions inside
Electrostatic attraction pulls potassium and chloride ions close to the membrane
Electric field directed inward forms
Electrostatic force vs. diffusional force
Nernst equation:
Goldman-Hodgkin-Katz equation:
Mechanism behind biopotentials 2/2
When membrane stimulation exceeds a threshold level of about 20 mV, so called action potential occurs:
Sodium and potassium ionic permeabilities of the membrane change
Sodium ion permeability increases very rapidly at first, allowing sodium ions to flow from outside to inside, making the inside more positive
The more slowly increasing potassium ion permeability allows potassium ions to flow from inside to outside, thus returning membrane potential to its resting value
While at rest, the Na-K pump restores the ion concentrations to their original values
The number of ions flowing through an open channel >10 6 /sec
Body is an inhomogeneous volume conductor and these ion fluxes create measurable potentials on body surface
Electrocardiography (ECG)
Measures galvanically the electric activity of the heart
Well known and traditional, first measurements by Augustus Waller using capillary electrometer (year 1887)
Instead of displaying the scalar amplitude (ECG curve) the electric activation front is measured and displayed as a vector (dipole model, remember?)
It has amplitude and direction
Diagnosis is based on the curve that the point of this vector draws in 2 or 3 dimensions
The information content of the VCG signal is roughly the same as 12-lead ECG system. The advantage comes from the way how this information is displayed
A normal, scalar ECG curve can be formed from this vectro representation, although (for practical reasons) transformation can be quite complicated
Plenty of different types of VCG systems are in use
No legacy problem as such
The biopotential amplifier
Small amplitudes, low frequencies, environmental and biological sources of interference etc.
Essential requirements for measurement equipment:
High amplification
High differential gain, low common mode gain high CMRR
High input impedance
Low Noise
Stability against temperature and voltage fluctuations
Electrical safety, isolation and defibrillation protection
The Instrumentation Amplifier
Potentially combines the best features desirable for biopotential measurements
High differential gain, low common mode gain, high CMRR, high input resistance
A key design component to almost all biopotential measurements!
Simple and cheap, although high-quality OpAmps with high CMRR should be used
CMRR fine tuning
Application-specific requirements
ECG amplifier
Lower corner frequency 0.05 Hz, upper 100Hz
Safety and protection: leakage current below safety standard limit of 10 uA
Electrical isolation from the power line and the earth ground
Protection against high defibrillation voltages
EEG amplifier
Gain must deal with microvolt or lower levels of signals
Components must have low thermal and electronic noise @ the front end
Otherwise similar to ECG
EMG amplifier
Slightly enhanced amplifier BW suffices
Post-processing circuits are almost always needed (e.g. rectifier + integrator)
EOG amplifier
High gain with very good low frequency (or even DC) response
DC-drifting electrodes should be selected with great care
Often active DC or drift cancellation or correction circuit may be necessary
Electrical Interference Reduction
Power line interference (50 or 60 Hz) is always around us
Connects capacitively and causes common mode interference
The common mode interference would be completely rejected by the instrumentation amplifier if the matching would be ideal
Often a clever “driven right leg circuit” is used to further enhance CMRR
Average of the V CM is inverted and driven back to the body via reference electrode
Filtering
Filtering should be included in the front end of the InstrAmp
Transmitters, motors etc. cause also RF interference
Small inductors or ferrite beads in the lead wires block HF frequency EM interference RF filtering with small capacitors High-pass filter to reject DC drifting Low-pass filtering at several stages is recommended to attenuate residual RF interference
50 or 60 Hz notch filter
Sometimes it may be desirable to remove the power line interference
Overlaps with the measurement bandwidth
May distort the measurement result and have an affect on the diagnosis!
Option often available with EEG & EOG measuring instruments
Twin T notch filter Determines notch frequency Notch tuning
Artifact reduction
Electrode-skin interface is a major source of artifact
Changes in the junction potential causes slow changes in the baseline
Movement artifacts cause more sudden changes and artifacts
Drifting in the baseline can be detected by discharging the high-pass capacitor in the amplifier to restore the baseline
Electrical isolation
Electrical isolation limits the possibility of passage of any leakage current from the instrument in use to the patient
Such passage would be harmful if not fatal!
Transformer
Transformers are inherently high frequency AC devices
Modulation and demodulation needed
Optical isolation
Optical signal is modulated in proportion to the electric signal and transmitted to the detector
Typically pulse code modulated to circumvent the inherent nonlinearity of the LED-phototransistor combination
Defibrillation Protection
Measuring instruments can encounter very high voltages
E.g. 1500…5000V shocks from defibrillator
Front-end must be designed to withstand these high voltages
1. Resistors in the input leads limit the current 3. Protection against much higher voltages is achieved with low-pressure gas discharge tubes (e.g. neon lamps) (note: even isolation components such as transformers and optical isolators need these spark gaps) Discharge @ ~100V 2. Diodes or Zener diodes protect against high voltages Discharge @ 0.7-15V
Electrodes – Basics
High-quality biopotential measurements require
Good amplifier design
Use of good electrodes and their proper placement on the patient
Good laboratory and clinical practices
Electrodes should be chosen according to the application
Basic electrode structure includes:
The body and casing
Electrode made of high-conductivity material
Wire connector
Cavity or similar for electrolytic gel
Adhesive rim
The complexity of electrode design often neglected
Electrodes - Basics
Skin preparation by abrasion or cleansing
Placement close to the source being measured
Placement above bony structures where there is less muscle mass
Distinguishing features of different electrodes:
How secure? The structure and the use of strong but less irritant adhesives
How conductive? Use of noble metals vs. cheaper materials
How prone to artifact? Use of low-junction-potential materials such as Ag-AgCl
If electrolytic gel is used, how is it applied? High conductivity gels can help reduce the junction potentials and resistance but tend to be more allergenic or irritating
Baseline drift due to the changes in junction potential or motion artifacts Choice of electrodes Muscle signal interference Placement Electromagnetic interference Shielding
Ag-AgCl, Silver-Silver Chloride Electrodes
The most commonly used electrode type
Silver is interfaced with its salt silver-chloride
Choice of materials helps to reduce junction potentials
Junction potentials are the result of the dissimilar electrolytic interfaces
Electrolytic gel enhances conductivity and also reduces junction potentials
Typically based on sodium or potassium chloride, concentration in the order of 0.1 M weak enough to not irritate the skin
The gel is typically soaked into a foam pad or applied directly in a pocket produced by electrode housing
Relatively low-cost and general purpose electrode
Particularly suited for ambulatory or long term use
Gold Electrodes
Very high conductivity suitable for low-noise meas.
Inertness suitable for reusable electrodes
Body forms cavity which is filled with electrolytic gel
Compared to Ag-AgCL: greater expense, higher junction potentials and motion artifacts
Often used in EEG, sometimes in EMG
Conductive polymer electrodes
Made out of material that is simultaneously conductive and adhesive
Polymer is made conductive by adding monovalent metallic ions
Aluminum foil allows contact to external instrumentation
No need for gel or other adhesive substance
High resistivity makes unsuitable for low-noise meas.
Not as good connection as with traditional electrodes
Metal or carbon electrodes
Other metals are seldom used as high-quality noble metal electrodes or low-cost carbon or polymeric electrodes are so readily available
Historical value. Bulky and awkward to use
Carbon electrodes have high resistivity and are noisier but they are also flexibleand reusable
Applications in electrical stimulation and impedance plethysmography
Needle electrodes
Obviously invasive electrodes
Used when measurements have to be taken from the organ itself
Small signals such as motor unit potentials can be measured
Needle is often a steel wire with hooked tip
That’s it, Now for Q&A SQUID = Superconducting Quantum Interference Device
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