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Applied and Environmental Microbiology, March 2002, p. 1458-1463, Vol. 68, No. 3
0099-2240/02/$04.00+0 DOI: 10.1128/AEM.68.3.1458-1463.2002
Copyright © 2002, American Society for Microbiology. All Rights Reserved.
Rupture of the Cell Envelope by Decompression of the Deep-Sea Methanogen Methanococcus jannaschii
Chan Beum Park and Douglas S. Clark*
Department of Chemical Engineering, University of California, Berkeley, California 94720
Received 15 August 2001/
Accepted 4 December 2001

ABSTRACT
The effect of decompression on the structure of
Methanococcus jannaschii, an extremely thermophilic deep-sea methanogen, was
studied in a novel high-pressure, high-temperature bioreactor.
The cell envelope of
M. jannaschii appeared to rupture upon
rapid decompression (ca. 1 s) from 260 atm of hyperbaric pressure.
When decompression from 260 atm was performed over 5 min, the
proportion of ruptured cells decreased significantly. In contrast
to the effect produced by decompression from hyperbaric pressure,
decompression from a hydrostatic pressure of 260 atm did not
induce cell lysis.

INTRODUCTION
The deep sea below 1,000 m accounts for 89% of the earth's total
ocean and is believed to harbor a rich variety of undiscovered
organisms exhibiting genetic and metabolic diversity (
5,
14,
18). Even though decompression is nearly unavoidable at some
point during research on deep-sea microorganisms, data on microbial
survival upon decompression are rare due to limitations in the
techniques and facilities suitable for high-pressure cultivation
(
19,
20). The only report of bacterial death upon decompression
concerned gas vacuolate bacteria (
7). In contrast, bacteria
without gas vacuoles, such as
Escherichia coli and
Corynebacterium xerosis, were reported to survive rapid decompression from extreme
gas supersaturation at 300 atm (
6,
7). Likewise, the deep-sea
heterotrophic isolate MT-41 obtained from 10,476 m did not exhibit
any morphological changes upon decompression from hydrostatic
pressure but did undergo ultrastructural alterations with increasing
time at atmospheric pressure (
3).
Hyperbaric bioreactor systems containing both liquid and gas phases offer advantages for the cultivation of autotrophic microorganisms at high pressures, most notably, better control of gaseous substrates and products (2, 10, 12, 13, 16). Considering the fact that many deep-sea extremophiles isolated to date grow on a gaseous substrate and produce a gaseous product(s) (8), hyperbaric pressurization should be an effective tool for efficient cultivation.
In the present work, we developed a high-pressure, high-temperature culturing system featuring both hyperbaric and hydrostatic bioreactors. Preliminary growth studies were performed with Methanococcus jannaschii, an extremely thermophilic methanogen originally isolated from a depth of 2,600 m (9). Scanning electron microscopy (SEM) revealed that the cell envelope of M. jannaschii ruptured upon decompression from 260 atm of hyperbaric pressure, with the degree of the disruption depending on the rate of decompression. These results have important implications for the collection and retrieval of microorganisms from deep-sea habitats containing high concentrations of dissolved gases and for the sampling of organisms from high-pressure laboratory reactors.
M. jannaschii was grown in serum bottles (125 ml) by strict anaerobic techniques, as described by Balch and Wolfe (1). The composition of the growth medium was the same as that described previously (17). Before starting the cultivation at 80°C in a shaking incubator, the gas atmosphere was anaerobically adjusted to 30 lb/in2 with a gas mixture of H2-CO2 (4:1). Exponentially growing cells were used as the inoculum. The inoculum sizes in the hyperbaric and hydrostatic bioreactors were 10 and 30% of the working volumes, respectively.
A schematic diagram of the high-pressure reactor system is shown in Fig. 1. All tubing and connectors used were obtained from High Pressure Equipment Co. (Erie, Pa.) and were designed to endure pressures up to 1,360 atm. A confined gasket-closure reactor (model GC-17; High Pressure Equipment Co.) was used as the hyperbaric bioreactor and was capable of operation at up to 200°C and 590 atm. The bioreactor had a total volume of 1.15 liters. A thermocouple (OMEGA Inc., Stamford, Conn.) inserted into a stainless steel 316 well extending three-fourths of the way into the bioreactor provided the signal to a proportional-integral-derivative controller (OMEGA Inc.) for precise control of the temperature through a heating belt (OMEGA Inc.). A diaphragm compressor (Newport Scientific Inc., Jessup, Md.) was used to supply H2, CO2, and He at high pressures. An oxygen trap (Alltech Inc., Deerfield, Ill.) was installed between the diaphragm compressor and the gas cylinder. The gas atmosphere in the hyperbaric bioreactor was H2-CO2 (4:1) up to 7.8 atm, and He was used for pressurization over 7.8 atm. The pressure of the hyperbaric bioreactor was precisely controlled with an air-actuated back-pressure regulator (Tescom, Elk River, Minn.) placed in the exit line of the gas loop.
After 1 h of startup operation, gas flow was switched to the
recycle mode in order to minimize the loss of gaseous substrates.
Liquid medium and inoculum were supplied anaerobically via a
liquid pump combined with a pressure module (Prostar 210 SDM;
Varian, Santa Clara, Calif.). Culture samples were taken periodically
from a liquid outlet line with a microcontrol metering valve
(High Pressure Equipment Co.), during which the maximum flow
rate was always maintained below 10 ml/min. Culture harvest
was obtained through a port in the bottom of the bioreactor
after gradual ventilation of gases to equilibrate the bioreactor
at atmospheric pressure. A tubular reactor (model MS-18; High
Pressure Equipment Co.) was used as the hydrostatic bioreactor
and had a volume of 65 ml. The hydrostatic bioreactor was first
pressurized with H
2-CO
2 (4:1) to 7.8 atm, and its pressure was
increased to 260 atm hydrostatically by pumping in cells and
growth medium with the liquid pump. Growth medium (45 ml) was
anaerobically inoculated in a serum bottle with 20 ml of exponentially
growing
M. jannaschii culture, followed by transfer into the
hydrostatic reactor through the liquid pump until the internal
pressure reached 260 atm. Temperature control was achieved by
incubating the pressurized hydrostatic bioreactor in an oven
after it was disconnected, as indicated in Fig.
1. The reactor
was reconnected to the system and repressurized to 260 atm every
2 h throughout the incubation period, during which time the
pressure decreased by no more than 10%. After 10 h of cultivation,
the hydrostatic bioreactor was depressurized in 1 s and the
culture was withdrawn for further analysis. This experiment
was performed twice with cultures of different initial cell
densities.
Protein concentrations in each sample were measured by the Bio-Rad microassay technique (11). The turbidity of each culture sample was measured by the optical density at 660 nm (OD660). M. jannaschii cells were fixed with a solution of 1% (vol/vol) glutaraldehyde and 0.1% (vol/vol) osmium tetroxide for analysis by SEM. The fixed cells were deposited onto polycarbonate membrane filters (0.2-µm pore size; Millipore Corp., Bedford, Mass.) with a 10-ml syringe, followed by rinsing with 0.1 M sodium cacodylate buffer (pH 7.2) and dehydration with ethanol. SEM of the fixed M. jannaschii cells was performed on a model S-5000 scanning electron microscope (Hitachi, Tokyo, Japan) after critical point drying and sputter coating.
Growth of M. jannaschii in the hyperbaric bioreactor at 7.8 and 260 atm was analyzed by determining the OD660 (Fig. 2A) and the total protein content (Fig. 2B), for which culture samples were withdrawn through a microcontrol metering valve with a low flow rate (<10 ml/min) but a rapid decompression time (<1 s). M. jannaschii exhibited barophilic growth according to the change in protein content, consistent with the results reported by Miller et al. (11). However, there was no substantial increase in the OD660 of the culture grown at 260 atm, which remained below 0.1. Similar results were obtained in repeated experiments carried out under hyperbaric conditions at 260 atm. After the same 260-atm culture was harvested with a longer decompression time (5 min), the OD660 had increased more than sixfold (Fig. 2A). However, assuming that the protein measurements shown in Fig. 2B reflect the true growth curves, the OD660 value from the 260-atm harvest was still low due to the artifact of cell rupture.
In order to investigate the effect of decompression on cell
morphology,
M. jannaschii grown at different pressures was analyzed
by SEM. As shown in Fig.
3A and
B,
M. jannaschii grown at 7.8
atm maintained the same morphology as that previously reported
(
9). In contrast, the culture grown at 260 atm and decompressed
in 1 s contained ruptured cells, widespread clusters of flagella,
and debris that appeared to be from the cell envelopes (Fig.
3C through
F).
The SEM photographs of
M. jannaschii harvested via slow decompression
for 5 min revealed that most cells maintained their normal morphology,
although some ruptured cells were still evident (Fig.
4A and
B). Moreover, the amounts of cellular debris and clustered flagella
were much smaller than they were after rapid decompression (Fig.
3C). We also examined the morphology of
M. jannaschii after
incubation for 24 h at 1 atm following a slow harvest from 260
atm. As shown in Fig.
4C and
D, there was no significant change
in the morphology of
M. jannaschii after the 24-h incubation.
This result is in contrast to the previously observed behavior
of MT-41, a deep-sea heterotrophic bacterium isolated from 10,476
m, which did exhibit aberrations in morphology after a 24-h
incubation at 1 atm (
3).
From these observations it became evident that decompression
from the hyperbaric gas system led to the rupture of
M. jannaschii and that decompression time is an important determinant of cell
damage. Thus, the low OD
660 observed after rapid decompression
from 260 atm can be ascribed to the smaller absorptivity of
cellular debris compared to that in intact cells. The higher
absorbance of whole cells is to be expected, given that the
absorptivity coefficient in the Beer-Lambert law is dependent
on the cross-sectional area of the analyte (
15).
The effect of decompression from high hydrostatic pressure was investigated by cultivating M. jannaschii in the hydrostatic bioreactor at 260 atm without using He. In this experiment, decompression was completed in 1 s after cultivation. As shown in Fig. 5, M. jannaschii exhibited a lower growth rate at 260 atm in the hydrostatic bioreactor, but, unlike the results seen with the hyperbaric bioreactor, the OD660 remained above 0.09. Furthermore, the correlation between the OD660 and the protein content was close to that of the 7.8-atm culture in the hyperbaric bioreactor, implying that decompression from hydrostatic pressure did not cause cell lysis.
The observed rupture by rapid decompression may have been promoted
by the increased intracellular solubility of He at high pressures,
in which cellular disruption was induced by the rapid expansion
of concentrated He in the cytoplasm through the cell envelope
during decompression of the sample. In this regard, it is noteworthy
that the solubility of He in water increases ca. 31-fold from
7.8 to 260 atm (
4). In contrast, a damaging effect caused by
high shear during sampling could be ruled out for the following
reasons: (1) the culture harvest remaining in the bioreactor
following decompression also contained many ruptured cells,
(2) the flow rate used for sampling from the 260 atm hyperbaric
culture was fairly low (<10 ml/min), and (3) in some ruptured
cells, only a small section of the cell envelope was missing,
consistent with the presence of a blowout mechanism induced
by rapid expansion.
In summary, the present work illustrates that rapid decompression from a hyperbaric environment can lead to cell rupture in deep-sea microorganisms regardless of whether a membrane-enclosed vacuole is present. This result should be borne in mind in laboratory studies of microbial growth at high pressures and in the sampling of deep-sea habitats containing high concentrations of dissolved gases.

ACKNOWLEDGMENTS
This research was supported by the National Science Foundation
(BES-9816490) and the Schlumberger Fellowship of D.S.C.
We thank Eric Grunland at the UC Berkeley Chemistry Machine Shop and Tracy Hsiao for their help in the design of the high-pressure, high-temperature bioreactor system.

FOOTNOTES
* Corresponding author. Mailing address: Department of Chemical Engineering, University of California, Berkeley, CA 94720-1462. Phone: (510) 642-2408. Fax: (510) 643-1228. E-mail:
clark{at}cchem.berkeley.edu.


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Applied and Environmental Microbiology, March 2002, p. 1458-1463, Vol. 68, No. 3
0099-2240/02/$04.00+0 DOI: 10.1128/AEM.68.3.1458-1463.2002
Copyright © 2002, American Society for Microbiology. All Rights Reserved.