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Applied and Environmental Microbiology, May 2000, p. 2243-2247, Vol. 66, No. 5
0099-2240/00/$04.00+0
Copyright © 2000, American Society for Microbiology. All rights reserved.
Differential Damage in Bacterial Cells by Microwave
Radiation on the Basis of Cell Wall Structure
Im-Sun
Woo,1
In-Koo
Rhee,2 and
Heui-Dong
Park1,*
Department of Food Science and
Technology1 and Department of
Agricultural Chemistry,2 Kyungpook National
University, Taegu, Korea
Received 16 August 1999/Accepted 11 February 2000
 |
ABSTRACT |
Microwave radiation in Escherichia coli and
Bacillus subtilis cell suspensions resulted in a dramatic
reduction of the viable counts as well as increases in the amounts of
DNA and protein released from the cells according to the increase of
the final temperature of the cell suspensions. However, no significant
reduction of cell density was observed in either cell suspension. It is believed that this is due to the fact that most of the bacterial cells
inactivated by microwave radiation remained unlysed. Scanning electron
microscopy of the microwave-heated cells revealed severe damage on the
surface of most E. coli cells, yet there was no significant
change observed in the B. subtilis cells. Microwave-injured E. coli cells were easily lysed in the presence of sodium
dodecyl sulfate (SDS), yet B. subtilis cells were resistant
to SDS.
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TEXT |
In recent years, the use of
microwave radiation has become popular in the food industry for
thawing, drying, and baking foods, as well as for the inactivation of
microorganisms in foods (21, 31, 32). In particular,
microbial destruction by microwave radiation has great potential in the
pasteurization of foods (31). Its short heating and exposure
time is less destructive to food than longer conventional heating
(15).
There have been many studies on the use of microwaves for the reduction
of microorganisms in various foods, including turkey, beef, corn-soy
milk, chicken, frozen foods, and potatoes (1, 5, 8, 12, 14, 28,
36). All of these works have led to the conclusion that microwave
radiation extends food preservation by reducing microbial cells in
food. Microwave heating is known to inactivate many microorganisms,
such as Escherichia coli, Streptococcus faecalis,
Clostridium perfringens, Staphylococcus aureus,
Salmonella, and Listeria spp. (2, 4, 5, 9,
10, 14, 15, 19, 20, 23, 24, 30). Bacterial and mold spores, as
well as the bacteriophage PL-1, which is specific to
Lactobacillus casei, have also been reported to be sensitive
to microwave radiation (20-22).
Despite many studies on microbial destruction by microwave radiation,
the mechanism of destruction is not fully understood. It is generally
thought that the destruction of microorganisms is mainly due to a
thermal effect of microwave exposure (16, 37, 38). However,
another argument has also been proposed to explain microbial
inactivation by microwaves. Several researchers have attempted to
ascertain if such radiation has a nonthermal effect on microorganisms
(7, 10, 27, 34). The destruction of microorganisms by
microwave at temperatures lower than the thermal destruction point has
been observed (11, 13, 22, 24, 27). In particular,
microwave-stressed cells of S. aureus exhibited a greater
metabolic imbalance than conventionally heated cells (27).
Morozov and Petin found that hypertonic solutions (1.0%) of sodium
chloride were less effective in protecting cells against heat damage
during microwave heating than during thermal heating (29).
This study examined the mechanism of microbial cell inactivation by
microwave heating along with the differences in the effects on
gram-positive and -negative bacteria.
Bacterial culture and microwave treatment.
E. coli
wild-type strain K-12 (3) was obtained from the Korean
Collection for Type Cultures, and Bacillus subtilis KM107 (24) was obtained from the stock culture in our laboratory. E. coli was grown in Luria broth (1% Bacto Tryptone, 0.5%
yeast extract, 1% NaCl) (33), and B. subtilis
was grown in nutrient medium (0.3% Bacto beef extract, 0.5% Bacto
Peptone) (35). The bacteria were cultured in 500 ml of the
liquid medium at 37°C for 15 h on a rotary shaker (150 rpm).
Cells were harvested by centrifugation and washed twice with a sterile
0.9% NaCl solution. The cell pellets were resuspended in a 0.9% NaCl
solution at a cell concentration of 109 to 1010
CFU/ml, which was used for the microwave radiation.
For the microwave heating, a 2,450-MHz microwave oven (MR301M; LG
Electronics, Inc., Changwoon, Korea) was used. The cell suspensions
were divided into 500-ml plastic beakers and maintained at 20°C. The
plastic beakers with the cell suspensions were placed individually in
the center of the oven and exposed to microwaves at full power (600 W).
The temperature changes in the suspensions were monitored with a
fluoroptic thermometer (950 channels; Luxtron Co., Santa Clara,
Calif.). After microwave radiation, the suspensions were stored at
4°C for the following experiments. Figure
1 shows the correlation between the
microwave radiation time and the temperature changes in the bacterial
cell suspensions. A linear increase in the temperature relative to
exposure time was observed, which was consistent when the microwave
radiation was repeated.

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FIG. 1.
Changes in the temperature of bacterial cell suspensions
relative to microwave exposure time. A bacterial cell suspension in
0.9% NaCl was exposed to microwave radiation at 600 W, and its
temperature changes were monitored.
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Measurements of viable cell counts and nucleic acid and protein
amounts.
The microwave-radiated cell suspensions were serially
diluted with a sterile 0.9% NaCl solution and spread on Luria-Bertani agar (E. coli) or nutrient agar (B. subtilis)
plates. The plates were incubated at 37°C for 24 h, and cells
were enumerated. Cell density was measured at 600 nm using a
spectrophotometer (CE393; Cecil Instruments, Cambridge, United
Kingdom). The amount of protein released from the microwave-treated
cells was measured at 595 nm by the method of Bradford (6).
Bovine serum albumin was used as the standard protein. The nucleic acid
content of the supernatants was directly measured at 260 nm using a UV
spectrophotometer (U200; Hitachi Co., Tokyo, Japan). All the
experiments were carried out in triplicate.
Electron microscopy.
After the cells were treated by microwave
radiation, the shape of the cells was examined by electron microscopy.
The cells were fixed at 24°C for 60 min with 2.5% glutaraldehyde in
0.1 M sodium cacodylate buffer (pH 7.2) (Sigma-Aldrich Chemie Gmbh, Steinheim, Germany), dehydrated with a serial concentration of ethanol,
and then dried on a critical point dryer (HCP-2; Hitachi Co.). The
dried cell samples were coated with gold (26), and examined
using a scanning electron microscope (S-4100; Hitachi Co.). For
transmission electron microscopy, dehydrated cells were embedded in a
medium type LR white resin (Sigma Chemical Co., St. Louis, Mo.), which
was polymerized at 60°C for 24 h (26). The
polymerized samples were sliced with an ultramicrotome and observed
using a transmission electron microscope (Hitachi Co.).
Inactivation of bacterial cells by microwave radiation.
The
inactivation patterns of the microwave-radiated cells were investigated
using cell suspensions (109 to 1010 CFU/ml) of
E. coli, a gram-negative bacterial strain, and B. subtilis, a gram-positive strain (Fig.
2). The viable counts in both cell
suspensions were found to dramatically diminish relative to an increase
in the microwave heating temperatures. Treatment up to 80°C resulted
in an approximate 5-log reduction of the viable count in both strains
compared to the initial counts. The highest reduction ratio in the
viable counts was observed when the temperature was increased from 50 to 60°C, which was a ca. 3-log reduction in E. coli
organisms (from 1.1 × 108 to 2.5 × 105 CFU/ml) and a ca. 2-log reduction in B. subtilis organisms (from 3.3 × 106 to 1.6 × 104 CFU/ml). When the microwave heating temperature
exceeded 60°C, the amount by which viable counts were reduced
dramatically decreased. When the temperature was increased from to 60 to 80°C, the viable counts were reduced only by factors of 10 in the
E. coli and 3 in the B. subtilis cell
suspensions. Therefore, it is assumed that microwave heating for
microbial inactivation is highly efficient up to a temperature of
60°C, yet not as effective at higher temperatures.

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FIG. 2.
Changes in viable count and cell density in E. coli (left panel) and B. subtilis (right panel) cell
suspensions relative to the temperature produced by microwave
radiation. The temperature of 20°C shown on the x axis
represents the temperature of cell suspensions before microwave
treatment. , viable cell count; , cell density.
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Although E. coli cells were slightly more sensitive to
microwave radiation than B. subtilis cells when the
temperature was increased from 50 to 60°C, B. subtilis
cells were more sensitive than E. coli cells when the
temperature was increased from 40 to 50°C. A temperature increase
from 40 to 60°C resulted in a ca. 3.23-log reduction in the E. coli and a ca. 3.66-log reduction in the B. subtilis
viable cell counts, indicating that B. subtilis cells are
more inactivated by microwave heating than E. coli in this
temperature shift. Because the cell wall of gram-positive bacteria is
generally much thicker and stronger than that of gram-negative bacteria, it was expected that B. subtilis would be more
resistant to microwave radiation than E. coli. However,
B. subtilis was found to be more sensitive than E. coli when the temperature was increased from 40 to 60°C.
Interestingly, it was observed that cell density in both cell
suspensions did not decrease in spite of a significant reduction in the
viable counts. This may be due to the fact that the microwave-treated cells were not completely lysed even when they were inactivated by
microwave radiation, and thus the cell density did not decrease.
Leakage of cell materials caused by microwave processing.
Another general indication of heat damage to microorganisms is the
leakage of nucleic acid and protein from cells. Microwave-injured cells
have often been reported to release ninhydrin-positive material, purines, and pyrimidines into a suspension (23). Nucleic
acid and its related compounds, such as pyrimidines and purines, are well known to absorb UV light at a wavelength of 260 nm. The presence of these materials in a suspension indicates damage to the cell at the
membrane level. Furthermore, similarly injured cells are also known to
release intracellular proteins into a suspension.
The amount of nucleic acid released into the cell suspension was
analyzed by measuring the absorbance at 260 nm (Fig.
3A). The two bacterial strains showed
similar patterns in their release of nucleic acid. The amount of leaked
nucleic acid from the cells grew relative to an increase in the
microwave-heated temperature of the cell suspension. However, the
leakage of nucleic acid from B. subtilis was higher than
that from E. coli. This result would seem to imply that
B. subtilis suffered greater membrane damage than E. coli. The amount of protein released into the cell suspension was
also analyzed in both strains (Fig. 3B). Microwave heating up to 40°C
resulted in no significant differences in the amount of protein leaked
from the cells. However, when the treatment temperature exceeded
40°C, substantial differences in the amount of leaked protein were
observed. These results indicate that most of the microwave-heated
cells were ghost cells from which intracellular materials were released
into the cell suspension. The protein release pattern of the two
bacterial strains was the reverse of the nucleic acid release pattern;
the amount of leaked protein in B. subtilis was found to be
much lower than that in E. coli. In particular, a low level
of protein leakage was observed when B. subtilis cells were
heated to 60°C, a temperature observed to be sufficient for a 5-log
reduction in the viable count. The reason for this is still unknown.

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FIG. 3.
Nucleic acid and protein amounts released into the cell
suspension from microwave-radiated bacterial cells relative to the
temperature produced by microwave radiation. After the E. coli ( ) and B. subtilis ( ) cell suspensions were
heated to the temperature shown on the x axis, the amounts
of nucleic acid and protein in the supernatant of the cell suspension
were measured.
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Effect of microwave radiation on the surface structure of bacterial
cells.
The opposite release patterns for the release of nucleic
acid and protein in two bacterial strains prompted us to examine the
surface structure of microwave-radiated cells (Fig.
4). The untreated cells and cells heated
up to 70°C were examined using a scanning electron microscope, and
the shapes of their surface structures were compared. It was found that
untreated E. coli cells had a smooth surface, while most of
the microwave-radiated cells exhibited severe destruction. The surfaces
of the microwave-heated cells were damaged and had become rough and
swollen. However, all the B. subtilis cells exhibited the
same smooth surface. Whether the cells were microwave heated or not, no
damage to their surface structures was observed. This result suggests
that the microwave-radiated cells remained unlysed in suspension,
although they were inactivated by the radiation. Furthermore, the
damage to the surface structure of E. coli cells may not,
therefore, be the main reason for inactivation by microwave heating.

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FIG. 4.
Scanning electron microphotograph of untreated and
microwave-radiated (up to 70°C) bacterial cells.
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Sensitivity of microwave-heated cells to SDS.
In order to
investigate the sensitivity of microwave-injured cells to lysis by
sodium dodecyl sulfate (SDS), microwave-heated cells in 0.9% NaCl were
incubated at 37°C with shaking (150 rpm) in the presence of 0.1%
SDS, and the cell density was monitored at 600 nm (Fig.
5). For E. coli, the density
of the microwave-heated cell suspension was dramatically reduced within
an hour of incubation in the presence of SDS, but it did not decrease
significantly in the absence of SDS. In the case of the untreated cell
suspension, no significant reduction in the cell density was observed
during 4 h of incubation, regardless of the presence of SDS. These
results support the conclusion that most of the cells inactivated by
microwave radiation remain unlysed in a cell suspension in the absence
of SDS. In addition, they are also highly sensitive to lysis by SDS.

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FIG. 5.
Sensitivity of untreated and microwave-radiated
bacterial cells to SDS. E. coli and B. subtilis
cell suspensions in 0.9% NaCl, both untreated and microwave heated up
to 70°C, were incubated at 37°C with shaking (150 rpm). Changes in
cell densities were then monitored at 600 nm, both with and without the
presence of 0.1% SDS. , untreated cells in the absence of SDS; ,
untreated cells in the presence of SDS; , microwave-radiated cells
in the absence of SDS; , microwave-radiated cells in the presence of
SDS.
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When the experiment was repeated using microwave-heated B. subtilis cells, different results were obtained. In the absence of
SDS, the cell density in both the untreated and microwave-heated cell
suspensions slightly decreased in a similar pattern. Unexpectedly, however, the cell density in both cell suspensions slightly increased in the presence of SDS. Why cell density increased is still unknown. Although ambiguous results were obtained for the reaction of B. subtilis cells to SDS, it was obvious that microwave-heated
B. subtilis cells were not affected by SDS. It was predicted
that microwave-injured E. coli cells would be sensitive to
SDS and that untreated cells would be resistant. However, in the case of B. subtilis, both untreated and microwave-heated cells
were unexpectedly resistant to SDS. This may be due to the fact that the cells of B. subtilis, a gram-positive bacterium, were
not lysed even in the presence of SDS because of their thick and rigid cell wall structure.
Effect of microwave radiation on the intracellular components of
cells.
To investigate the effect of microwave heating on
intracellular components, cells that were microwave heated up to 70°C
were examined using a transmission electron microscope (Fig.
6). When microwave heated, both types of
bacteria showed several dark spots in their cytoplasm. However, no dark
spots were observed in the untreated cells, suggesting that the dark
spots were the result of microwave heating. Heat treatment has been
known to cause protein denaturation and aggregation in cytoplasm as
well as to induce heat shock proteins (39, 40). Therefore,
the dark spots are thought to be aggregated proteins caused by
microwave heating. The two bacterial strains showed similar results for
protein aggregation regardless of their cell wall structure, which
suggests that protein aggregation may participate somehow in microbial
inactivation caused by microwave heating. Further studies on the
induction of heat shock proteins are in progress to elucidate whether
microwave heating induces heat shock proteins in bacterial cells.

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FIG. 6.
Transmission electron microphotograph of untreated and
microwave-radiated (up to 70°C) bacterial cells.
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ACKNOWLEDGMENTS |
This work was supported by a research grant from the Living System
Laboratory, LG Electronics Inc. We are highly grateful for this support.
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FOOTNOTES |
*
Corresponding author. Mailing address: Department of
Food Science and Technology, Kyungpook National University, 1370 Sankyuk, Taegu 702-701, Korea. Phone: 82-(53)-950-5774. Fax:
82-(53)-950-6772. E-mail: hpark{at}knu.ac.kr.
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Applied and Environmental Microbiology, May 2000, p. 2243-2247, Vol. 66, No. 5
0099-2240/00/$04.00+0
Copyright © 2000, American Society for Microbiology. All rights reserved.
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