University of Houston University of Houston-Clear Lake ISSO Annual Report Y2002pp. 91-96
Dielectric Responses of Living Organisms
John H. Miller, Jr. (UH) and James R. Claycomb (UH)
Abstract
We have developed and tested several highly sensitive approaches for measuring
the linear and nonlinear dielectric responses of live cell suspensions at low
frequencies. We observe enormous linear dielectric constants at very low
frequencies (with relative dielectric constants of over a hundred million at 10
Hz) attributed to the high polarizability of live cells resulting from their
finite membrane potential. In addition, we find that nonlinear dielectric
responses are affected by the metabolic states of the cells, such as their
response to glucose. The tools reported here are powerful noninvasive methods
with numerous potential applications in pharmacology, medicine, and biology.
THE ELECTRIC CHARGES IN LIVE CELLS INTERACT WITH OR produce electric fields, which results in enormous dielectric responses, flexoelectricity, and related phenomena. The electromagnetic properties of live organisms are of considerable fundamental interest and also hold the potential for numerous practical applications. For example, dielectric spectroscopy can potentially be used to detect biological warfare agents without requiring direct contact with the organisms. Additional applications include monitoring human cells grown in NASA bioreactors for microgravity studies, noninvasive glucose sensors, and detection of cancer cells.
Conventional methods of performing dielectric spectroscopy at very low frequencies require large electric field amplitudes, which can induce electrorotation, electroflexion, and other strongly perturbative influences. The reason is that previous techniques lack sufficient sensitivity to attain the nonperturbative weak field limit at low frequencies. Thus, there is a need for developing methods of measuring low-frequency dielectric response with greatly improved sensitivity.
Technical Plan and Equipment
We have developed several approaches for measuring both the linear and the nonlinear dielectric responses of live cell
suspensions at low frequencies. One method is to use sensitive
superconducting quantum interference devices (SQUIDs) to measure the tiny magnetic fields produced by the small displacement
currents flowing through the cell suspension. The SQUID sensor is coupled to flux locked loop electronics, the output of which is
fed into a lock-in amplifier. The suspension is placed between the
two electrodes of a parallel plate capacitor, across which an ac
voltage is applied at the frequency of interest.
Another approach is to employ a similar parallel plate capacitor and to use a bridge circuit to measure the alternating current (both magnitude and phase relative to the applied ac voltage); this information is utilized to compute the complex dielectric response as a function of frequency. The full complex dielectric spectrum from 10 Hz to 100 kHz is thereby acquired with an FFT spectrum analyzer. In order to measure nonlinear dielectric response, a signal at a fixed fundamental frequency is applied and the induced harmonics are measured with the FFT spectrum analyzer. We have also developed a SQUID-based approach to improve the sensitivity of nonlinear dielectric response measurements.
Experimental Activity
Experiments carried out in this project are designed to probe
the dielectric properties of live cells. Interiors of living cells
are electrically negative with respect to their environment,1 and this
charge separation is utilized for a variety of cellular
properties, from energy production to cell-to-cell communication. The charges that create the membrane potential can be polarized by
an electric field, leading to a net dipole moment, as illustrated
in Fig. 1(a). The linear dielectric response, which measures the ability
of the charges to respond to an alternating field, decreases with
frequency. Most importantly, its frequency-dependence depends on the type of organism and also helps differentiate between living
organisms and nonliving materials.
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Figure 1. (a) Field-induced polarization of the charges in a cell or organism. The magnitude of the induced dipole moment strongly depends on the membrane potential and other properties of the organism. (b) Setup for measuring the dielectric response of living organisms. The network analyzer measures the conduction and displacement currents induced by the time-varying potential between the two plates of the capacitor.
One of the set-ups we use to measure linear dielectric response2,3 is illustrated in Fig. 1(b). An ac voltage applied to the electrodes produces both a conduction current and a displacement current through the specimen. The real and imaginary parts of the transfer function V2(w)/V1(w) are proportional to the conductivity and the dielectric constant , respectively. This method demonstrates the lowest noise levels thus far at low amplitudes and frequencies4-8 and, unlike electrorotation methods,9 is weakly perturbative.
Discussion
Figure 2 shows dielectric spectra of suspensions of Schizosaccharomyces pombe
(yeast-108 cells/ml), Escherichia
coli (109 cells/ml),
and particles of the inert compound Y2O3 in aqueous
solutions. The dielectric responses of the living cell
suspensions are seen to be enormous at low frequencies and to decrease with frequency. We find that these data are consistent with
theoretical predictions10 and
that the low-frequency dielectric constant decreases if the cells die. One can see that strong frequency
dependence is a unique property of living organisms, by
comparing it to the flat responses of water, ethylene glycol, and inert powder suspensions (Fig. 2).

Figure 2. Measured relative dielectric constant vs. frequency, r(f), for suspensions of S. pombe (yeast-108 cells/ml), E. coli bacteria (109cells/ml), and the inert inorganic compound Y2O3, and for water and ethylene glycol, obtained using the setup shown in Fig. 1(b)
Results
More recently, we have developed a powerful tool to probe the nonlinear dielectric responses of live cells to a singe
frequency excitation. We have measured nonlinear dielectric properties of live cell suspensions using both a conventional electrode
technique and a novel set-up employing a high-Tc superconducting quantum interference device (SQUID), as illustrated in Fig. 3.
For example, we have measured the nonlinear dielectric properties of Saccharomyces cerevisiae
(bakers
yeast) cells,11 as
shown in Figs. 4 and 5. Woodward and Kell12-14 have demonstrated that nonlinear
dielectric spectroscopy is a powerful tool for characterizing biological cell suspensions and their metabolic states. Enzymes
embedded in the cell membrane are not free to rotate in the
presence of an ac electric field but, instead, change shape or
conformation.15 These
conformational changes, which depend on the metabolic state, result in a distortion of the excitation
waveform that is detected as a superposition of harmonics of the
fundamental excitation frequency.

Figure 3. Setups used to measure nonlinear dielectric properties of biological agents: using both a conventional electrode technique (left) and a novel set-up employing a high-Tc SQUID (right).

Figure 4. Harmonics of the 1 kHz driving frequency recorded with an FFT spectrum analyzer using a four-electrode probe (Fig. 3) immersed in: (a) water, (b) a suspension of yeast (Saccharomyces cerevisiae) cells, and (c) a suspension of yeast cells after the addition of 5 grams of glucose. The first large peak is attributed to the 1-kHz excitation.

Figure 5. (a) Harmonic response of bakers yeast cells to a low frequency, 17-Hz excitation using the SQUID-based setup (Fig. 3). (b) Variation of the third harmonic response with excitation field amplitude (17-Hz excitation frequency). (c) Third harmonic response vs. excitation frequency for a 1-V/cm fundamental field amplitude
To measure higher harmonics with the electrode technique, the four-electrode probe is suspended vertically in the cell suspension. An ac voltage is supplied across the outer electrodes, and the cell response across the inner pair is measured with an FFT spectrum analyzer. Nonlinear dielectric spectroscopy is an extremely sensitive probe in which the spectra depend on the type of organism and its metabolic state. For example, enzyme conformation changes result in harmonics that can be monitored with a fast-Fourier transform (FFT) spectrum analyzer. Figure 4 shows the voltage power spectra recorded on the FFT spectrum analyzer using a four-electrode probe immersed in (a) water, (b) a yeast (S. cerevisiae) cell suspension, and (c) a yeast suspension with glucose. Alarge peak is observed at the driving frequency (1 kHz) in each medium. A small third harmonic is observed in the water medium, probably due to residual polarization effects. More pronounced second and third harmonics are observed in the cell suspension, with less pronounced fourth and fifth harmonics. An enhanced second harmonic is observed in the cell suspension after the addition of glucose. This type of behavior has been attributed to changes in the metabolic state of the yeast cells.15
SQUIDs are extremely sensitive magnetic sensors that can measure the magnetic fields generated by displacement currents flowing in the cell suspension. The SQUID-based configuration, shown in Fig. 3 (right), provides greatly enhanced sensitivity at low frequencies and eliminates spurious harmonics resulting from polarization effects at the electrode surfaces. Figure 5(a) shows the harmonic response to a 17 Hz excitation frequency at a fixed amplitude, while Figs. 5(b) and 5(c) show the field amplitude-dependence and frequency-dependence, respectively, of the third harmonic response.
The sensitive linear and nonlinear dielectric spectroscopy methods reported here are powerful noninvasive tools with numerous potential applications in pharmacology, medicine, and biology.
Acknowledgments
The investigators gratefully acknowledge support by the
Institute for Space Systems Operations (ISSO), the Texas Center for Superconductivity and Advanced Materials
(TcSAM), and the Robert A. Welch Foundation (E-1221).
References
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2C. Prodan, J. R. Claycomb, E. Prodan, and J. H. Miller, Jr. "High-Tc
SQUID-Based Impedance
Spectroscopy of Living Cell Suspensions," Physica
C 341-348 (2000): 2693-94.
3C. Prodan, F.
Mayo, J. R. Claycomb, J. H. Miller, Jr., and M. J. Benedik. "Low-Frequency, Low-Field Dielectric Spectroscopy
of Living Cell Suspensions," J. Appl. Phys. (Submitted.)
4J. Gimsa and D. Wachne r. "A Unified Resistor-Capacitor Model for Impedance,
Dielectrophoresis, Electrorotation, and Induced Transmembrane Potential," Biophys.
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1419
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(CTAB) Surfactant Upon the Dielectric Properties of Yeast Cells," Biochimica
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8K. Asami, E. Gheorghiu, and T. Yonezawa. "Dielectric Behavior of Budding Yeast in Cell Separation,"
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9R. Georgieva, B. Neu, V. M. Shilov, E. Knippel, A. Budde, R. Latza, E.
Donath, H. Kiesewetter, and H. Bäumle. "Low Frequency Electrorotation of Fixed Red Blood Cells,"
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10C. Prodan and E. Prodan. "The Dielectric Behavior of Living Cell Suspensions,"
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Phys. D: Appl. Phys. 32 (1999):
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11J. R. Claycomb,
C. Prodan, D. Nawarathna, and J. H. Miller, J r. "Nonlinear Dielectric Spectroscopy of Living Cell
Suspensions," 2nd Joint Meeting of the IEEE Engineering in Medicine & Biology Society and the Biomedical Engineering
Society, Houston, TX, Oct. 23-26, 2002. (In
press.)
12A. M. Woodward
and D. B. Kell. "On the Nonlinear Dielectric Properties of Biological Systems:
Saccharomyces
cerevisiae," Bioelectrochem. & Bioenergetics 24
(1990): 83-100.
13A. M. Woodward
and D. B. Kell. "Dual-Frequency Excitation: A Novel Method for Probing the Nonlinear Dielectric Properties of
Biological Systems, and its Application to Suspensions of S.
cerevisiae," Bioelectrochem.
& Bioenergetics 25 (1991):
395-413.
14A. M. Woodward
and D. B. Kell. "On the Relationship between the Nonlinear Dielectric Properties and Respiratory
Activity of the Obligately Aerobic Bacterium Micrococcus luteus," Bioelectrochem.
& Bioenergetics 26 (1991):
423-39.
15A. Jones.
"Computational Aspects of Nonlinear Biological Dielectric Spectroscopy," Ph.D. Thesis, Dept. of Computer
Science, University of Whales, Aberystwyth, 2001.
Publications
Claycomb, J. R. and J. H. Miller, Jr. "Superconducting
Shields for SQUID Applications," Review
of Scientific Instruments 70 (1999): 4562-68.
Claycomb, J. R., N. Tralshawala, and J. H. Miller, Jr.
"Theoretical Investigation of Eddy-Current Induction for Nondestructive Evaluation by Superconducting Quantum Interference
Devices," IEEE Trans.
Magn. 36 (2000): 292-98.
Claycomb, J. R., M. Nersesyan, D. Luss, and J. H. Miller, Jr. "SQUID Detection of Magnetic Fields Produced by Chemical
Reactions," IEEE
Trans. on Applied Superconductivity 11.1 (2001): 863-66.
Claycomb, J. R., C. Prodan, D. Nawarathna, and J. H. Miller, Jr. "Nonlinear Dielectric Spectroscopy of Living Cell
Suspensions," IEEE Trans.
Engineering in Medicine and Biology Transactions,
2003. (In press.)
Claycomb, J. R., K. E. Bassler, J. H. Miller, Jr., M. Nersesyan,
and D. Luss. "Avalanche Behavior in the Dynamics of Chemical Reactions,"
Physical
Review Letters 87 (2001):
178303-1-4.
Claycomb, J. R., A. Brazdeikis, R. A. Yarbrough, G. Gogoshin, and J. H. Miller, Jr. "Nondestructive Testing of PEM Fuel
Cells," IEEE Trans. Appl. Supercond., 2003. (In
press.)
Claycomb, J. R., M. Nersesyan, W. LeGrand, J. T. Ritchie, D. Luss, and J. H. Miller, Jr. "Chemomagnetic Characterization
of Chemical Reactions using High-Tc SQUIDs," Physica
C 341-348 (2000): 2641-44.
Fang, H., J. R. Claycomb, Y. X. Zhou, P. T. Putman, S. Padmanabhan, J. H. Miller, Jr., K.
Ravi-Chandar, and K. Salam. "Melt-Textured YBCO Superconducting Tube for Magnetic
Shielding," IEEE Trans. Appl. Supercond., 2003. (In
press.)
Lobera-Serrano, J. A., J. R. Claycomb, J. H. Miller, Jr. and K. Salama. "Hybrid Double-D
Sheet-Inducer for SQUID-Based NDT," IEEE Trans.
on Applied Superconductivity 11.1
(2001): 1283-86.
Martirosyan, K. S., J. R. Claycomb, G. Gogoshin, R. A. Yarbrough, J. H. Miller, Jr., and D.
Luss. "Spontaneous Magnetization Generated by Spin, Pulsating and Planar Combustion Synthesis,"
J.
of Appl. Phys. (Submitted.)
McCarten, J. P., T. C. Jones, X. Wu, J. H. Miller, Jr., I. Pirtle, X. Xu, J. R.
Claycomb, J.-R. Liu, and W.-K. Chu. "Phase Slip Scaling Relationship for the 59 K and 143 K Charge-Density
Waves in NbSe3," Journal de Physique IV (France)
9 (1999): 129-32.
Nersesyan, M. D., J. R. Claycomb, J. T. Ritchie, J. H. Miller,
Jr., and D. Luss. "Magnetic Fields Produced by the Combustion of Metals in Oxygen,"
Combustion
Science and Technology 169 (2001): 89-106.
Nersesyan, M. D., J. R. Claycomb, Q. Ming, J. H. Miller, Jr., J.
T. Richardson, and D. Luss. "Chemomagnetic Fields Produced by Solid Combustion Reactions,"
Applied
Physics Letters 75 (1999): 1170-72.
Nersesyan, M. D., J. R. Claycomb, J. T. Ritchie, J. H. Miller,
Jr., J. T. Richardson, and Dan Luss. "Electric and Magnetic
Fields Generated by SHS," J.
Materials Synthesis and Processing 9 (2001): 63-72.
Prodan, C., J. R. Claycomb, E. Prodan, and J. H. Miller, Jr.
"High-Tc SQUID-Based
Impedance Spectroscopy of Living Cell Suspensions," Physica
C 341-348 (2000): 2693-94.
Prodan, C., F. Mayo, J. R. Claycomb, J. H. Miller, Jr., and M.
J. Benedik. "Low-Frequency, Low-Field Dielectric Spectroscopy of Living Cell Suspensions,"
J. Appl. Phys. (Submitted.)
Presentations
Claycomb, J. R., C. Prodan, D. Nawarathna, and J. H. Miller, Jr. "Nonlinear Dielectric Spectroscopy of Living Cell
Suspensions," 2nd Joint Meeting of the IEEE Engineering in Medicine & Biology Society and the Biomedical Engineering
Society, Houston, TX, Oct. 23-26, 2002.
Claycomb, J. R., D. Nawarathna, K. E. Bassler, C. Prodan, and J. H. Miller Jr. "Is Electro-Chemical Noise a SOC
Phenomenon," March Meeting of the American Physical Society, Austin, TX, March 3-7, 2003.
Claycomb, J. R., R. A. Yarbrough, G. Gogoshin, K. E. Bassler, and J. H. Miller, Jr. "Self Organized Criticality in
Electrochemical Reactions," March Meeting of the American Physical Society, Indianapolis, IN, March 18-22, 2002.
Claycomb, J. R, A. Brazdeikis, R. A. Yarbrough, G. Gogoshin, J. H. Miller, Jr., and M. Le. "Nondestructive Testing of PEM
Fuel Cells," Applied Superconductivity Conference, Houston, TX, Aug. 4-9, 2002.
Fang, H., J. R. Claycomb, Y. X. Zhou, P. T. Putman, S. Padmanabhan, J. H. Miller, Jr., K.
Ravi-Chandar, and K. Salama. "Melt-Textured YBCO Superconducting Tube for Magnetic Shielding," Applied Superconductivity Conference,
Houston, TX, Aug. 4-9, 2002.
Nawarathna, D. "Nonlinear Dielectric Spectroscopy of Living Cell Suspensions," 24th Semiannual TcSAM Student
Symposium, Houston, TX, Dec. 17, 2002.
Nawarathna, D., J. R. Claycomb, C. Prodan, and J. H. Miller, Jr. "Non-Linear Dielectric Spectroscopy of Living Cell
Suspensions using SQUIDs," March Meeting of the American Physical Society, Austin, TX, March 3-7, 2003.
Prodan, C., F. Mayo, J. R. Claycomb, and J. H. Miller, Jr. "Dielectric Spectroscopy of Living Cell Suspensions,"
March Meeting of the American Physical Society, Indianapolis, IN, March 18-22, 2002.
Prodan, C., F. Mayo, J.R. Claycomb, D. Nawarathna, and J. H. Miller, Jr. "Techniques of Measuring the Membrane Potential
of Biological Cells: Measurements and Modeling," March Meeting of the American Physical Society, Austin, TX, March
3-7, 2003.
Sanabria, H., G. Cardenas, X. Yang, J. H. Miller, Jr., L. T. Wood, and M. J.
Benedik. "Optical Projection Microscopy of Live Cells," March Meeting of the American Physical Society,
Austin, TX, March 3-7, 2003.
Vajrala, V., D. Nawarathna, J. R. Claycomb, C. Prodan, and J. H. Miller, Jr. "Impedance Magnetocardiography using High-Tc
SQUIDs," March Meeting of the American Physical Society, Austin, TX, March 3-7, 2003.
Funding and proposals
"Dielectric Spectroscopy of Biological Agents," Naval
Surface Warfare Center, requested for two years, $757,726 (submitted).
"Novel Applications of High-Tc Superconducting Sensors." Robert A. Welch Foundation, June 1, 2001-May 31, 2004,
$150,000.
"Novel Live Cell Imaging and Monitoring Technologies." NASA, Office of
Biological and Physical Research, requested for four years, $813,468 (submitted).
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Investigative Team UH PI: John H. Miller, Jr.,. Ph.D., Associate Professor UH PDAF: James R. Claycomb, Ph.D. |
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Institute for Space Systems Operations - Y2002
Annual Report
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