WO1992006634A1 - A device for measurement of electrical impedance of organic and biological materials - Google Patents
A device for measurement of electrical impedance of organic and biological materials Download PDFInfo
- Publication number
- WO1992006634A1 WO1992006634A1 PCT/SE1991/000703 SE9100703W WO9206634A1 WO 1992006634 A1 WO1992006634 A1 WO 1992006634A1 SE 9100703 W SE9100703 W SE 9100703W WO 9206634 A1 WO9206634 A1 WO 9206634A1
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- WO
- WIPO (PCT)
- Prior art keywords
- measuring
- electrodes
- electrode
- control electrode
- impedance
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Classifications
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B5/00—Measuring for diagnostic purposes; Identification of persons
- A61B5/05—Detecting, measuring or recording for diagnosis by means of electric currents or magnetic fields; Measuring using microwaves or radio waves
- A61B5/053—Measuring electrical impedance or conductance of a portion of the body
- A61B5/0531—Measuring skin impedance
-
- A—HUMAN NECESSITIES
- A61—MEDICAL OR VETERINARY SCIENCE; HYGIENE
- A61B—DIAGNOSIS; SURGERY; IDENTIFICATION
- A61B3/00—Apparatus for testing the eyes; Instruments for examining the eyes
- A61B3/10—Objective types, i.e. instruments for examining the eyes independent of the patients' perceptions or reactions
- A61B3/16—Objective types, i.e. instruments for examining the eyes independent of the patients' perceptions or reactions for measuring intraocular pressure, e.g. tonometers
Definitions
- the present invention relates to a device for non-invasive depth-selective detection and characterization of surface phenomena in organic and biological systems such as tissues by surface measurement of the electrical impedance of said mate ⁇ rial with said device as well as a method for said surface characterization.
- Electrical impedance is a very sensitive indicator of minute changes in organic and biological material and especially tissues such as mucous membranes, skin and integuments of organs, including changes due to irritation caused by diffe ⁇ rent reactions, and scientists all over the world have worked hard to find a convenient way to measure variations and alte ⁇ rations in different kinds of organic and biological material to be able to establish the occurrence of such alterations which are due to different states, characteristic of irrita ⁇ tions from e.g. diseases.
- Characteristic features of these systems are that they are intended for use with specimens mounted in appropriate elec ⁇ trochemical cells.
- U.S.P. 4,038,975 (Aug. 2,1977) to Vrana et al. relates to an electrically instrumented method of diagnosing the presence of a neoplast in mucuos membrane samples wherein the electrical impedance of the sample has resistive and capacitive compo- nents and wherein the relative values of said components are indicative of the presence or absence of said neoplast by associating the sample with the terminals of a series circuit including in succession a grounded, amplitude-modulated high- frequency generator and first and second equal-valued resis ⁇ tors wherein the impedance of the generator and the resistance of both resistors are low relative to the impedance of the sample.
- EP 0 315 854 (Appln. No. 88118083.0) to Honna is previously known a method and a system for measuring moisture content in skin by passing "weak" low frequency electric current through the keratinous layer between two electrodes abutted upon the skin, amplifying the electric voltage appearing on the layer, rectifying and taking out signals of the amplified output, and measuring the amplitude of the signal, which is characterized in that the voltage appearing on the keratinous layer is the voltage appearing between either one of said two electrodes whichever is closer to another electrode which is abutted upon said skin at a location outside said two electrodes.
- the system comprises a measuring electrode structure of triple concentric circles including a central electrode, an inter ⁇ mediate electrode and an outer electrode all of which can be abutted on the skin, a generator which uses one of said elec ⁇ trodes as a common electrode and supplies low frequency signal between this common electrode and another of said three elec ⁇ trodes; an amplifier which converts the resulting current into a voltage appearing between said common electrode and yet another of said three electrodes, and a means to display the output voltage of the amplifier which is characterized in that a circuit means is provided for switching between a first cir ⁇ cuit using said intermediate electrode as common electrode and a second circuit which uses the outer electrode as a common electrode.
- Characteristic of existing technology in this field is that either: a) a biopsy would have to be excised in order to well define the actual tissue under test, i.e. not suit ⁇ able for in vivo measurements; or
- electrodes are applied to the skin at separate sites, directing the electric test current right through the skin and regarding the inner part of the skin and deeper lying tissue as an almost ideal short cir* * * it between the contact sites, i.e. no discrimi ⁇ nation between the layers of the rather complicated anatomy of the skin.
- depth selectivity is achie ⁇ ved by controlling the extension of the electric field in the vicinity of the measuring electrodes by means of a control electrode between the measuring electrodes, the control electrode being actively driven with the same frequency as the measuring electrodes to a signal level, taken from one of the measuring electrodes but also multiplied by a complex number, in which the real and imaginary parts are optimized for each application depending upon the desired depth penetra ⁇ tion.
- the function of the controlling field is analogous to that of a field effect transistor, well known from solid state physics. In biological tissue or "wet state", conduction mechanisms are complicated involving a number of ions, polari ⁇ zation effects, charged or polarizable organelles, etc. How ⁇ ever, no reconstruction algorithms are needed to achieve depth selectivity, although consecutive measurements at different depths must be recorded in order to obtain a profile.
- the principle is basically frequency independent, and works from DC to several MHz. Simple impedance measurements at one or a few frequencies, as well as impedance spectroscopy in this range can thus be done depth selective on e.g. skin.
- Fig. 1 is a block diagram illustrating the principle of measu ⁇ rement employed in an embodiment of the present invention
- Fig. 2a is a plane topview of the tip of a probe with two measuring electrodes separated by a control electrode;
- Fig. 2b is a cross-sectional view along plane S - S of Fig. 2a;
- Fig. 3a is a cross-sectional view of a probe with linear, iterated structure
- Fig. 3b is a perspective view of the tip of the probe with a linear, iterated structure, electrically equvivalent to Fig. 3a;
- Fig. 3c is a perspective view of the tip of a simplified structure of a similar arrangement, sufficient in some appli ⁇ cations.
- Fig. 4a is an illustration of a normal tissue with closed packed cells
- Fig. 4b is an illustration of an irritated tissue showing increased intercellular space
- Fig. 5 is a plot showing mean values in % obtained with prior technique in measurement of irritation on oral mucosa for NaCl, H 3 P0 4 , SLS;
- Fig. 6 is a plot showing values in % for one person obtained with the technique according to the invention in the measure ⁇ ment of irritation on oral mucosa;
- Fig. 7 is a plot showing irritation index results of measure ⁇ ment of irritation on skin with the technique according to the invention for one person with 20 hours of exposure of material and additionally 24 hours;
- Fig. 8 is a plot showing absolute value of electrical impedan ⁇ ce at 20 kHz measured on intact surface of rat kidney at consecutive values of blood pressure by stepwise choking and releasing supporting artery in vivo;
- Fig. 9a is a plane topview of a generalized probe switchable into different configurations
- Fig. 9b is a cross-sectional view along plane S - S of Fig. 9a showing also switchable electrical pathways.
- the essential features of the invention are a probe with two measuring electrodes separated by a control electrode, sui ⁇ table equipment for measuring the electric impedance in the desired frequency range, and an amplifier with adjustable amplification capable of maintaining the chosen control sig ⁇ nal, derived from the potential of one of the measuring elec ⁇ trodes at the control electrode without loading said measuring electrode, i.e. the amplifier must have high input impedance and low output impedance in the frequency range used.
- the control electrode is following the potential of one of the measuring electrodes by multiplying the signal of the ampli ⁇ bomb with a complex number in which the real and imaginary parts are optimized for each application. With the amplifica ⁇ tion factor set to zero, the system assumes the special case of signal ground at the control electrode.
- the system behaviour is similar to the system in the prime case of Fig. 1 described in the EP Publication No. 0315 854 (Application No. 88118083.0), where one electrode is always connected to signal ground.
- the intermediate electrode of said system is not actively driven by an amplifier as in the present invention but is galvanically connected to signal ground.
- any control signal different from zero the amplitude may be less than, equal to, or larger than the amplitude supplied to the measuring electrodes
- the present amplifier of course can also be set to signal ground whereby the function signalwise corresponds to the previously known apparatus.
- the electrodes may be configured in concentric, linear, iterated linear or any topological way compatible with the essential features. Additional electrodes carrying guard, signal ground, driven guard, etc. may be required to optimize operation depending on the application. Cabling and shielding must be in accordance with established engineering practice in order to minimize electromagnetic interference. For use on humans, design may have to conform to local safety regula ⁇ tions.
- the amplitude supplied to the electrodes should be no more than a few tens of millivolts, preferably below 50 millivolts and more preferably about 25 millivolt. Higher amplitudes produce unreliable results.
- Working on wet mucous membranes does not require any special preparations. If deeper layers of the skin (stratum corneum and down) are to be investigated, the dry surface of the skin is preferably inundated with a salt solu ⁇ tion of physiological concentration.
- control electrode to vary depth penetration is, as stated above, limited by the shapes, sizes and distances of the electrodes as well as the properties of the tissue under test. For a large range of depths a variety of probes of different sizes may thus seem necessary. However, a generalized probe can be achieved by adding a number of electrodes which are switched into different functions according to Fig. 9b.
- the dominating factor determining depth penetration is distances between electrodes; the basic theory has been expanded by Roy et al (Roy, A. & Apparao, A.: Depth of investigation in direct current methods. Geophysics, Vol. 36, No. 5, 1971, pp 943-959; Roy, K.K. & Rao, K.P. : Limiting depth of detection in line electrode systems. Geophysical Prospecting, 25 . . 1977, pp 758-767) for a number of electrode configurations.
- the path of the measured test current is kept from the immediate surface of the probe by driving the virtual control electrode according to the present invention.
- all (minimum one) electrodes in between are connected together to form the virtual control electrode.
- Distances between electrodes may be the same or vary in a non-linear way to achieve e.g. stepwise increase of penetration with a fixed factor.
- the switches may be mechanical or electronic and may be manually operated or under computer control.
- the best mode is thus to use the center electrode and outermost ring as measurement electrodes and using the rings in between, connected together, as a control electrode, and driving this virtual control electrode with a potential derived from the potential of one of the measurement electrodes in the same way as described above.
- Fig. 1 is shown a block diagram illustrating the principle of measurement employed in a preferred embodiment of the present invention.
- Two measuring electrodes A and C are separated by a third electrode, the control electrode B.
- Said control electrode B will be actively held at a given potential by a controllable amplifier F, said amplifier F also receiving an input reference signal from electrode A using a high impedance input terminal and supplying said control electrode B via a low impedance output terminal so that said control electrode B will track said electrode A but with a signal level ensueing from the transfer function of the amplifier F.
- Said measuring electrodes A and C are connected to a standard instrument for impedance measurement IM.
- FIG. 2b illustrates a preferred embodiment of the tip end of a measurement probe for studies of irritation on i.e. oral mucosa and skin.
- Said probe consists of the electrodes A, B and C, each electrically isolated from the other, in a coaxial arrangement and presents as depicted in Fig 2a. a plane surface containing respective electrodes A, B and C and the isolating material 1.
- Fig. 3b and Fig. 3c are showing the respective embodiments of an open linear, iterated structure which can be used according to the invention.
- the structure of Fig. 3c involves a simpli ⁇ fied feature, within the scope of the invention sufficient in some applications.
- the invention relates to a device for depth-selective, non- invasive, local measurement of electric impedance in tissues such as preferably skin, mucous membranes and integuments of organs in or from humans or animals in vivo or in vitro comprising a probe with concentric electrodes, the size of which is depending upon desired maximum depth penetration.
- the electrodes comprise a central electrode being one of two measuring electrodes, and the central electrode being sur ⁇ rounded by a control electrode which is following the poten ⁇ tial of the central electrode by multiplying the signal of one of the measuring electrodes by a complex number in which the real and imaginary parts are optimized for each applica ⁇ tion.
- the control electrode is surrounded by a second measuring electrode.
- the essential part of the probe except for the contact surface, is surrounded by conductive material at signal ground or following the potential at the central electrode by a factor of one. All conductive parts are separated by stable isolating material and all electrodes and isolating material on the contact surface arranged in one plane, concave or convex surface to fit the surface of the test site with minimum liquid wedge.
- the device is further provided with suitable equipment for measuring impedance at a limited number of frequencies, these frequencies determined in pretests for a certain application by a wide scan of frequen ⁇ cies and plotting of Nyquist or Bode graphs.
- the signal of the control electrode is optimized when the real part is a number between 0.01 - 10 and the imaginary part as close to zero as possible for the transfer function of the amplifier F in the used frequency range .
- Fig. 4a shows normal tissue with close packed cells.
- Fig. 4b shows irritated tissue with increased intercellular space.
- High frequency (HF) is coupled capacitively through cell membrane to cell interior.
- LF Low frequency
- Conductivity is essentially the same in intra- och extracellu ⁇ lar liquid.
- the graph shows result from 30 minutes exposure (-30 to 0 in graph) to sodium lauryl sulphate, with a pause of approximately 15 seconds half way (at -15 in graph) to measure that point. After 12 hours irritation index is back at normal levels. Maximum irritation of this substance on this test person was reached 15 minutes after cessation of exposure.
- the device according to the invention it is possible to measure non-invasibly from the surface of any mucous membrane which can be reached from one side.
- any mucous membrane which can be reached from one side.
- artifacts from skin or muscular tissue are eliminated, and it is possible to follow irritation processes on single per ⁇ sons with high accuracy.
- Absolute value of electrical impedance at 20 kHz was measured on the intact surface of a rat kidney, still in function. At the same time arterial pressure was measured with a sensor implanted in the supporting vessel. Consecutive blood pres ⁇ sures were induced by choking and releasing the supporting artery. Impedance correlated well with pressure, with a delay of approximately 15 seconds. Graph shows sequence of events. Autoregulatory mechanisms of the kidney are not demonstrated explicitly with this type of plot.
- the device according to the invention has been tried for measurement of electric impedance on intact kidney of rat in vivo, the kidney being exposed to changes in blood circulation and pressure. There is significant correlation between pressu ⁇ re and value of measured impedance, the correlation being higher at 20 kHz (FIG 8) than at 100 kHz. Thus, the device according to the invention may be useful to detect ischemic states during e.g. transplantational surgery.
- the invention may be useful for diagnosis of glauco ⁇ ma.
Abstract
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Priority Applications (9)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US08/039,361 US5353802A (en) | 1990-10-18 | 1991-10-18 | Device for measurement of electrical impedance of organic and biological materials |
DK91918393T DK0553187T3 (en) | 1990-10-18 | 1991-10-18 | Measurement of electrical impedance in organic and biological material |
AU88499/91A AU659111B2 (en) | 1990-10-18 | 1991-10-18 | A device for measurement of electrical impedance of organic and biological materials |
EP91918393A EP0553187B1 (en) | 1990-10-18 | 1991-10-18 | A device for measurement of electrical impedance of organic and biological materials |
DE69129698T DE69129698T2 (en) | 1990-10-18 | 1991-10-18 | DEVICE FOR MEASURING THE ELECTRICAL IMPEDANCE OF ORGANIC AND BIOLOGICAL SUBSTANCES |
JP51777291A JP3320413B2 (en) | 1990-10-18 | 1991-10-18 | Measurement device for electrical impedance of organic or biological materials |
CA002093922A CA2093922C (en) | 1990-10-18 | 1991-10-18 | A device for measurement of electrical impedance of organic and biological materials |
FI931730A FI110304B (en) | 1990-10-18 | 1993-04-16 | Apparatus and method for measuring the electrical impedance of organic and biological substances |
NO931415A NO307863B1 (en) | 1990-10-18 | 1993-04-16 | Apparatus for measuring electrical impedance in organic and biological materials |
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
SE9003336A SE466987B (en) | 1990-10-18 | 1990-10-18 | DEVICE FOR DEEP-SELECTIVE NON-INVASIVE, LOCAL SEATING OF ELECTRICAL IMPEDANCE IN ORGANIC AND BIOLOGICAL MATERIALS AND PROBE FOR SEATING ELECTRICAL IMPEDANCE |
SE9003336-6 | 1990-10-18 |
Publications (1)
Publication Number | Publication Date |
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WO1992006634A1 true WO1992006634A1 (en) | 1992-04-30 |
Family
ID=20380684
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
PCT/SE1991/000703 WO1992006634A1 (en) | 1990-10-18 | 1991-10-18 | A device for measurement of electrical impedance of organic and biological materials |
Country Status (15)
Country | Link |
---|---|
US (1) | US5353802A (en) |
EP (1) | EP0553187B1 (en) |
JP (1) | JP3320413B2 (en) |
KR (1) | KR100201178B1 (en) |
AT (1) | ATE167794T1 (en) |
AU (1) | AU659111B2 (en) |
CA (1) | CA2093922C (en) |
DE (1) | DE69129698T2 (en) |
DK (1) | DK0553187T3 (en) |
ES (1) | ES2120419T3 (en) |
FI (1) | FI110304B (en) |
HU (1) | HU216496B (en) |
NO (1) | NO307863B1 (en) |
SE (1) | SE466987B (en) |
WO (1) | WO1992006634A1 (en) |
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WO2010085969A1 (en) | 2009-01-27 | 2010-08-05 | Scibase Ab | Switch probe for multiple electrode measurement of impedance |
US8948838B2 (en) | 2009-01-27 | 2015-02-03 | Scibase Ab | Switch probe for multiple electrode measurement of impedance |
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WO2019223874A1 (en) | 2018-05-24 | 2019-11-28 | Scibase Ab | Impedance measurement device |
Also Published As
Publication number | Publication date |
---|---|
ES2120419T3 (en) | 1998-11-01 |
NO307863B1 (en) | 2000-06-13 |
CA2093922C (en) | 2001-07-31 |
JPH06502323A (en) | 1994-03-17 |
AU8849991A (en) | 1992-05-20 |
AU659111B2 (en) | 1995-05-11 |
EP0553187A1 (en) | 1993-08-04 |
SE9003336A (en) | 1992-04-19 |
JP3320413B2 (en) | 2002-09-03 |
US5353802A (en) | 1994-10-11 |
KR100201178B1 (en) | 1999-06-15 |
FI931730A (en) | 1993-04-16 |
EP0553187B1 (en) | 1998-07-01 |
NO931415D0 (en) | 1993-04-16 |
HU216496B (en) | 1999-07-28 |
DK0553187T3 (en) | 1999-06-28 |
NO931415L (en) | 1993-05-13 |
HUT66173A (en) | 1994-09-28 |
DE69129698D1 (en) | 1998-08-06 |
SE466987B (en) | 1992-05-11 |
ATE167794T1 (en) | 1998-07-15 |
CA2093922A1 (en) | 1992-04-19 |
FI931730A0 (en) | 1993-04-16 |
SE9003336D0 (en) | 1990-10-18 |
DE69129698T2 (en) | 1999-03-11 |
HU9301109D0 (en) | 1993-08-30 |
FI110304B (en) | 2002-12-31 |
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