University of Houston University of Houston-Clear Lake ISSO Annual Report Y2004 73-76
Low-Frequency Dielectric Spectroscopy of Martian Soil Samples
Abstract--Martian soil simulants and live cell suspensions are under study using low-frequency dielectric spectroscopy (DS) and related techniques, such as nonlinear harmonic response. Such methods hold tremendous potential to develop sensors that can test for subsurface microbial life on Mars and for numerous additional applications. For example, the low-frequency alpha-dispersion, unique to live organisms, leads to enormous dielectric responses that enable a clear distinction between living and inanimate materials. UH researchers measured the low-frequency dielectric properties of soil samples known to be Mars analogues, as well as known live cell suspensions. In this initial study, they tested common soil and JSC Mars-1, a volcanic ash from Hawaii developed for use as a Mars regolith simulant. Biologically active, JSC Mars-1 contains microorganisms and biomolecules equivalent to 106-107 cells/gram, less than common soils. Finally, the UH research team recently discovered resonant-like behavior in the frequency-dependent harmonic responses of live cells. Preliminary evidence suggests that this behavior may result from active molecular motor complexes unique to live organisms. DS may prove to be a life detection tool.
The issue of whether or not life once existed on Mars, or perhaps still exists today,1 has profound scientific implications for the evolution of life on Earth and the distribution of life in the cosmos. The Viking program made the first serious attempt to detect the presence of living or fossilized organisms in Martian soil and yielded ambiguous results.2 However, recent studies of the Martian meteorite Allan Hills 84001 (ALH84001) suggest that microbial life existed on Mars about four billion years ago.3 Perhaps the most compelling evidence is the existence of magnetite (Fe3O4) crystals found within carbonate globules and their associated rims in the meteorite.4 About one fourth of these tens-of-nanometer sized magnetites are nearly identical to those produced by magnetotactic bacteria on Earth and are not known or expected to be produced by abiotic means. Researchers have argued that these Martian magnetite crystals are in fact magnetofossils, which, if true, would constitute evidence of the oldest life forms known.5
Further evidence suggests that subsurface Martian life could potentially survive even
today.6 There is abundant geological evidence that ice was once deposited in
the regolith, where it should still be present above mid-latitudes.
Goals of the Project
The goals of this project are to study dielectric spectroscopy12,13 and related
methods, such as nonlinear harmonic response,14 as possible techniques for the
detection and characterization of live organisms. One objective is to characterize Martian
soil simulants using dielectric spectroscopy. A challenge for astrobiological
investigation of Mars and other extraterrestrial bodies is to develop in situ
instruments capable of distinguishing environmental samples or extracts containing life
forms from those that do not. At the same time, the life-detection technology must not be
geocentric; that is, it must not be targeted to characteristics that, although specific to
life, may be limited to those life forms native to Earth. We are thus investigating
dielectric spectroscopy (DS) as a life detection tool, because life throughout the Cosmos,
regardless of its biochemistry and the nature of its genetic material, must utilize a
variety of complex, charged macromolecules.15
Results
A material's dielectric constant e(w) represents its linear response to
an applied ac electric field at a frequency w. This property is determined by the
motion of free charges inside the live cells, as well as by the way macromolecules
polarize in response to the applied field. In our experiments, we employ a parallel plate
capacitor configuration for linear response measurements and a four-probe method to
measure any nonlinear harmonics produced by changes in the conformational states of
macromolecular enzyme complexes. Our setup for linear dielectric response uses a liquid
capacitor cell coupled to a Solartron Analytical Model 1260 Impedance Analyzer. This setup
enables us to obtain the complex dielectric response, with both the real and imaginary
parts, where the imaginary part of the dielectric response is proportional to the
conductivity divided by the frequency.
Several dispersions (or relaxations), termed a-, b-, and g- dispersions, can be measure in the linear dielectric responses of biological cell suspensions and tissues over the frequency range 1 Hz-10 GHz. The a-dispersion, which appears below several kHz, is unique to living organisms and has been found to correlate with the cellular membrane potential.16 The b-dispersion, typically observed at MHz frequencies, is due to interfacial polarization, and is mainly attributed to the insulating plasma membrane surrounding each cell. The g-dispersion, which lies above 1 GHz,17 results from reorientation of water and biological macromolecules. This project primarily focuses on the low-frequency a- and b- responses. In addition, we employ related methods, such as nonlinear harmonic response, to probe signals produced by active molecular motors that are unique to live organisms, using a Stanford Research SR 780 Vector Signal Analyzer.
We tested common soil and JSC Mars-1, a volcanic ash from Hawaii, developed for use as a Mars regolith simulant.18 Biologically active, JSC Mars-1 contains microorganisms and biomolecules equivalent to 106-107 cells/gram,19 less than common soils (which can contain quantities of up to 109 cells/gram). Portions of each environmental sample were left untreated, while other portions were sterilized: autoclaved for 60 minutes at 121°C, at 2 atm, then heated in an oven at 220°C for 3 hours followed by exposure to ultraviolet light for 16 hours. Water extractions were then performed on sterilized and untreated soil and JSC Mars-1 samples. Extracts of untreated soil and JSC Mars-1 yielded multiple microbial strains when incubated on Luria-Bertani (LB) agar for 24 hours at three temperatures: 23°C, 30°C, and 37°C. Extracts of sterilized soil and JSC Mars-1 showed no growth at any of these temperatures, indicating that the sterilization protocol had indeed destroyed all living forms within the environmental samples.
When DS was conducted on extracts, the dielectric constant and conductivity were found to be higher for sterilized samples as compared with untreated samples. We hypothesize that the sterilization protocol results in increased dielectric constant and conductivity due to lysis of cells and the consequent release of charged molecules. However, the values obtained for unsterilized samples may be attributed not only to the presence of charged molecules, but also to membrane potentials of living cells. Samples containing living cells may thus be distinguishable from those containing only macromolecules by performing DS at variable temperatures.
Thus at two temperatures, 4°C and 37°C, we tested a suspension of the bacterium, E. coli (2.5 × 109 cells/ml, see Fig. 1), as well as three examples of large, charged biomolecules: deoxyribonucleic acid (DNA), hemoglobin (Hb), and bovine serum albumin (BSA). At 10 Hz, dielectric constant for E. coli suspension increased by 70% at 37°C as compared to 4°C, while dielectric constants for DNA, Hb, and BSA increased by 28%, 17%, and 49% respectively. However, the DNA, Hb, and BSA used in this preliminary study were then found to be contaminated with microorganisms. As in the case of E. coli, the effects of temperature on life may be the reason the dielectric differences measured for these compounds. We therefore used fetal bovine serum (FBS) (containing proteins, cell wall lipids, and other compounds), specially treated to eliminate all known or suspected life forms, including the controversial entities known as nanobacteria.20,21 Results showed that at 10 Hz the dielectric constant for sterile FBS increases by only approximately 6.5% for the FBS at 37°C vs. 4°C (see Fig. 1).

Figure 1. Relative dielectric constants (top, real part) and conductivities (bottom) of a suspension of E. coli (2.5 × 109 cells/ml) at 4°C and 37°C.
More recently, we have discovered resonant-like peaks in the frequency-dependent nonlinear harmonic responses of live cells. Preliminary evidence suggests that this behavior may result from active molecular motor complexes unique to live organisms, thus providing another tool for detecting life forms and for fundamental research in biophysics. Nonlinear response is currently probed by measuring induced higher harmonics using a four-electrode probe suspended in the cell suspension, as shown in Fig. 2, in order to study the intrinsic response of the medium and reduce electrode polarization effects. A sinusoidal voltage is applied to the outer electrodes, and the cell response across the inner pair of electrodes is measured as a function of frequency, showing plots of the induced harmonics, using the SR780 signal analyzer. Nonlinear dielectric spectroscopy is an extremely sensitive technique by which the spectra are influenced by the type of organism, its metabolic state, and changes in the conformational states of proteins.

Figure 2. Setup used to measure the nonlinear harmonic response of a live cell suspension using a four-electrode technique, with a 1-cm spacing between the outer two electrodes.
Figure 3 shows the magnitudes of the induced harmonics (across the inner two
electrodes) vs. applied fundamental frequency, for an applied voltage amplitude of 5 V
across the outer two electrodes. Note that two peaks, centered around 5 kHz and 12 kHz,
appear to "grow- out of the background as the cell concentration is increased. In
addition, we find that potassium cyanide suppresses the observed peaks. Potassium cyanide
(KCN) is a known respiratory inhibitor that binds to the cytochrome c oxidase complex.
This enzyme is the fourth complex of the electron transport chain, which pumps protons (H+
ions) across the mitochondrial inner membrane against the concentration gradient. As it
does so, it oxidizes the electron carrier cytochrome c, and is responsible for 90 percent
of the oxygen consumption by all living organisms on the planet. Importantly, yeast cells
are not necessarily killed by cyanide, and they remain capable of fermentation.
The large H+ concentration gradient across the membrane results in a transmembrane
potential that can be as high as 250 mV and drives a remarkable molecular turbine, known
as ATP-synthase. Since the proton gradient and transmembrane potential are suppressed when
cyanide blocks the cytochrome c oxidase complex, the operation of ATP-synthase is also,
indirectly, inhibited by cyanide. More recent experiments on naked uncoupled mitochondria
suggest that the observed lower frequency peak in Fig. 3 may be produced by the cytochrome
c oxidase complex and/or other components of the mitochondrial electron transport chain,
or, perhaps, molecular motors in the cytoplasm that rely on ATP for their operation.

Figure 3. Induced 3rd harmonic amplitude vs. applied fundamental frequency (5-V applied amplitude) for three different concentrations of S. cerevisiae (budding yeast). Note that two peaks, centered around 5 kHz and 12 kHz, appear to "grow- out of the background as cell concentration is increased.
Ongoing and planned studies will employ a variety of inhibitors that bind to different enzymes, to determine the precise origins of the observed features. Additional results in our lab suggest that the higher frequency peak may either result from a remarkable molecular turbine—the F0 unit of ATP synthase—or from molecular motors in the cytoplasm driven by ATP.
Recently, Elston et al.22 have proposed a model of energy transduction by the F0 unit of ATP-synthase. A proton on the high concentration side of the mitochondrial inner membrane enters through a channel onto the F0 rotor, and is then deflected through electrostatic repulsion by the positively charged arg1 unit on the "stator," thus providing a torque on the rotor. The number of discrete rotational steps of the F0 rotor depends on the number of subunits, many eucaryotic mitochondria having F0 rotors with 12 subunits, but the number being smaller in many bacteria. Eventually, after passing through nearly one complete revolution, the proton leaves through another channel on the low concentration side of the membrane. The Brownian ratchet has become a paradigm for representing a wide variety of molecular motors, both rotary and linear, and can be modeled as a particle in an asymmetric saw tooth potential undergoing random thermal excitations. The stochastic excitation of the particle out of each well, together with the asymmetry, results in a net Brownian motion with an average dc component along a preferred direction. Alternatively, an ac excitation at a specific frequency can also induce motion along the preferred direction, especially when the applied frequency correlates with the washboard frequency. This effect has thus come to be called the "correlated ratchet.-
Our results indicate that dielectric spectroscopy, at variable temperatures, and nonlinear harmonic response may be useful both for in situ astrobiology studies on the surface of Mars and for study of the liquid ocean beneath the ice of Europa.
References
1B. M. Jakosky and E. L. Shock, "The Biological Potential of Mars, the
Early Earth, and Europa," J. Geophys. Res. 103 (1998): 19,359-64.
2L. Margulis, P. Mazur, E. S. Barghoorn, H. O. Halvorson, T. H. Jukes, and I.
R. Kaplan, "The Viking Mission: Implications for life on Mars," J. Mol. Evol.
14 (1979): 223-32.
3D. S. McKay, E. K. Gibson Jr., K. L. Thomas-Keprta, H. Vali, C. S. Romanek, S.
J. Clemett, X. D. F. Chillier, C. R. Maechling, and R. N. Zare, "Search for Past Life
on Mars: Possible Relic Biogenic Activity in Martian Meteorite ALH84001," Science
273 (1996): 924-930.
4K. L. Thomas-Keprta, S. J. Clemett, D. A. Bazylinksi, J. L. Kirschvink, D. S.
McKay, S. J. Wentworth, H. Vali, E. K. Gibson, Jr., M. F. McKay, and C. S. Romanek,
"Truncated Hexa-Octahedral Magnetite Crystals in ALH84001: Presumptive
Biosignatures," Proc., Nat. Acad. Sci. USA 98 (2001): 2164-69.
5K. L. Thomas-Keprta, S. J. Clemett, D. A. Bazylinksi, J. L. Kirschvink, D. S.
McKay, S. J. Wentworth, H. Vali, E. K. Gibson, Jr., and C. S. Romanek,
"Magnetofossils from Ancient Mars: A Robust Biosignature in the Martian Meteorite
ALH84001," Applied & Environmental Microbiology 68 (2002): 3663-72.
6B. P. Weiss, Y. L. Yung, and K. H. Nealson, "Atmospheric Energy for
Subsurface Life on Mars?- Proc., Nat. Acad. Sci. USA 97 (2000): 1395-99.
7M. T. Mellon and B. M. Jakosky, "Geographic Variations in the Thermal and
Diffusive Stability of Ground Ice on Mars," J. Geophys. Res. 98 (1993):
3345-64.
8M. H. Carr, Water on Mars. New York: Oxford Univ. Press, 1996.
9W. B. Whitman, D. C. Coleman, and W. J. Wiebe, "Prokaryotes: The Unseen
Majority," Proc., Nat. Acad. Sci. USA 95 (1998): 6578-83.
10K. H. Nealson, "The Limits of Life on Earth and Searching for Life on
Mars," J. Geophys. Res. 102 (1997): 23,675-86.
11J. C. Priscu, C. H. Fritsen, E. E. Adams, S. J. Giovannoni, H. W. Paerl, C.
P. McKay, P. T. Doran, D. A. Gordon, B. D. Lanoil, and J. L. Pinckney, "Perennial
Antarctic Lake Ice: An Oasis for Life in a Polar Desert," Science 280
(1998): 2095-98.
12H. P. Schwan, "Electrical properties of tissue and cell
suspensions," in Advances in Biological and Medical Physics. Vol 5. Eds. J.
H. Lawrence and C. A. Tobias. New York: Academic Press, 1957. 147-209.
13K. Asami, "Characterization of Biological Cells by Dielectric
Spectroscopy," J. Non-crystaline Solids 305 (2002): 268-77.
14D. Nawarathna, J. R. Claycomb, J. H. Miller, Jr., and M. J. Benedik,
"Nonlinear Dielectric Spectroscopy of Live Cells Using Superconducting Quantum
Interference Devices," Appl. Phys. Lett. 86 (2004): 023902-1-3.
15C. Prodan, "Dielectric Properties of Live Cell Suspensions," Ph.D.
Dissertation, University of Houston, 2003.
16C. 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. 95 (2004): 3754-56.
17J. B. Hasted, Aqueous Dielectrics. London: Chapman and Hall, 1973.
18C. C. Allen, R. V. Morris, K. M Jager, D. C. Golden, D. J. Lindstrom, M. M.
Lindstrom, and J. P. Lockwood, "Martian Regolith Simulant JSC Mars-1," 29th
Annual Lunar and Planetary Science Conference, NASA Johnson Space Center, Houston, TX,
March 16-20, 1998.
19C. C. Allen, C. Griffin, A. Steele, N. Wainwright, and E. Stansbery,
"Microbial Life in Martian Regolith Simulant JSC Mars-1," 31st Lunar and
Planetary Science Conference, Johnson Space Center, Houston, TX, March 13-17, 2000.
20E. O. Kajander, N. Ciftcioglu, K. Aho, and E. Garcia-Cuerpo,
"Characteristics of Nanobacteria and Their Possible Role in Stone Formation," Urol.
Res. 2 (2003): 47-54.
21A. P. Sommer, H. I. Hassinen, and E. O. Kajander, "Light-Induced
Replication of Nanobacteria: A Preliminary Report," J. Clin. Laser Med. Surg.
5 (2002): 241-44.
22T. Elston, H. Wang, and G. Oster, "Energy Transduction in ATP
Synthase," Nature 391 (1998): 510-13.
Publications
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.
of App. Physics 95.7 (2004): 3754-56.
PDF (261KB)
Table of Contents
Institute for Space Systems Operations - Y2004 Annual
Report
Copyright © 2005