Dormant bacterial spores are able to survive long periods of time without nutrients, withstand harsh environmental conditions, and germinate into metabolically active bacteria when conditions are favorable. Numerous factors influence this hardiness, including the spore structure and the presence of compounds to protect DNA from damage. It is known that the water content of the spore core plays a role in resistance to degradation, but the exact state of water inside the core is a subject of discussion. Two main theories present themselves: either the water in the spore core is mostly immobile and the core and its components are in a glassy state, or the core is a gel with mobile water around components which themselves have limited mobility. Using deuterium solid-state NMR experiments, we examine the nature of the water in the spore core. Our data show the presence of unbound water, bound water, and deuterated biomolecules that also contain labile deuterons. Deuterium-hydrogen exchange experiments show that most of these deuterons are inaccessible by external water. We believe that these unreachable deuterons are in a chemical bonding state that prevents exchange. Variable-temperature NMR results suggest that the spore core is more rigid than would be expected for a gel-like state. However, our rigid core interpretation may only apply to dried spores whereas a gel core may exist in aqueous suspension. Nonetheless, the gel core, if present, is inaccessible to external water.
Dormant bacterial spores are able to survive long periods of time without nutrients, withstand harsh environmental conditions, and germinate into metabolically active bacteria when conditions are favorable. Numerous factors influence this hardiness, including the spore structure and the presence of compounds to protect DNA from damage. It is known that the water content of the spore core plays a role in resistance to degradation, but the exact state of water inside the core is a subject of discussion. Two main theories present themselves: either the water in the spore core is mostly immobile and the core and its components are in a glassy state, or the core is a gel with mobile water around components which themselves have limited mobility. Using deuterium solid-state NMR experiments, we examine the nature of the water in the spore core. Our data show the presence of unbound water, bound water, and deuterated biomolecules that also contain labile deuterons. Deuterium-hydrogen exchange experiments show that most of these deuterons are inaccessible by external water. We believe that these unreachable deuterons are in a chemical bonding state that prevents exchange. Variable-temperature NMR results suggest that the spore core is more rigid than would be expected for a gel-like state. However, our rigid core interpretation may only apply to dried spores whereas a gel core may exist in aqueous suspension. Nonetheless, the gel core, if present, is inaccessible to external water.
Gram-positive bacteria,
particularly of the Bacillus and Clostridium genera, have a sporulation mechanism
by which they can protect their DNA and become dormant under harsh
conditions that would otherwise kill them.[1] This survival mechanism allows for the bacteria to survive in a
metabolically inactive state for long periods of time until conditions,
such as temperature or nutrient content, allow for germination and
outgrowth. Some spores have been recovered and cultured after storage
in amber for millions of years.[2] The structure
of the spore is well-understood, separated into distinct regions:
an outer spore coat which is laminar and serves as a protective barrier;[3−7] the cortex, composed of cross-linked peptidoglycan distinct from
that found in the germinated bacterial cell wall and implicated in
the heat resistance of spores;[8−11] and the core, containing the bacterial DNA as well
as protective molecules such as small acid-soluble proteins (SASPs)[12−14] and an aquo-coordination complex between Ca2+ and dipicolinic
acid (pyridine-2,6-dicarboxylic acid).[15−18] The spore core has a lowered
water content compared to that of vegetative cells, which is thought
to be a major factor in spore heat resistance.[19−21]The exact
nature of the water in the spore core is not well understood.
Two main paradigms have formed around this question. One theory is
that the core water is in an amorphous (glassy) state. This was suggested
by Sapru and Labuza in 1993[22] by predicting
glass transition temperatures for spores based on inactivation kinetics
and finding that more heat-resistant spores had higher predicted glass
transition temperatures. Ablett in 1999[23] used differential scanning calorimetry to identify features of B. subtilis spores that were indicative of low moisture
content even in an excess water environment and using 13C NMR on calcium dipicolinate concluded it was likely in an amorphous
solid state indicative of a core with low water content consistent
with a glassy state. Amorphous calcium dipicolinate was also seen
using Raman spectroscopy of B. cereus spores.[24,25] The other theory is that the core water is in a gel-like state.
This hypothesis was put forward initially by Black and Gerhardt[26] as a means of explaining their results on water
uptake in spores using tritium-labeled H2O; they proposed
that the spore core is an insoluble gel whose components are cross-linked
but water-permeable. More recently, some[27,28] have argued for the gel-like core theory based on deuterium relaxation
times recorded from D2O-exchanged spores. Proponents of
the gel core theory assert that the gel provides thermal heat resistance
during dormancy by protecting proteins against thermal denaturation,
assisted by the lower water content of the core.[27] Sunde et al.[27] asserted that,
were the core in a glassy state, there would be a broad signal apparent
in a 2H NMR spectrum of the spore; however, such a signal
would be undetectable using the magnetic relaxation dispersion experiments
as performed. Kaieda et al.[28] analyzed
a quadrupolar-echo spectrum of hydrated spores and concluded that
its line shape represents mobile water and labile deuterons from proteins,
nucleic acids, and peptidoglycan. Thus, no immobilized water could
be detected in the 2H NMR spectrum of fully hydrated spores.[28]Here, we report 2H NMR spectra
of deuterated spores
of a wild-type Bacillus subtilis (ATCC 6051) and
the chloramphenicol-resistant strain Bacillus subtilis 1A578.[29] Deuterium–hydrogen exchange
experiments were conducted to examine the permeability of water into
the spore and to compare them against calcium dipicolinate trihydrate
(a known spore core component) and bovine serum albumin (as a spore
protein analogue). In addition, variable-temperature (VT) NMR experiments
were performed to determine how the deuteron mobility varies as the
spores are heated and cooled. Our results suggest that there is immobile
water in the spore core that can be detected using quadrupolar echo
deuterium NMR. Variable-temperature NMR data does not show a gradual
increase in molecular mobility proportional to temperature as would
be expected for a spore core containing a gel of highly mobile water.
Instead, our VT NMR data indicate that deuterated biomolecules and
deuterated water retain their anisotropic motion properties at 50
°C. Heating to 100 °C does not affect viability, and the
NMR spectra show that the proteins remain immobile at this temperature.
However, 100 °C causes a transition of some deuterons from anisotropic
to isotropic motion which we attribute to immobile water associated
with protein hydration. These observations support the glassy-state
core theory for our samples of dried spore powders. Nonetheless, we
also observe mobile water in the core as recently reported[27,28] and it remains possible that an aqueous spore suspension could have
a gel-like core.
Materials and Methods
Spore Preparation
Bacillus subtilis 1A578, a chloramphenicol-resistant
strain,[29] was obtained from Bacillus Genetic
Stock Center (BGSC, Department
of Chemistry at the Ohio State University). Spores were prepared from
stock Bacillus subtilisATCC 6051 and 1A578. Frozen
stock was inoculated overnight in 20 mL aliquots of LB medium, which
was used to inoculate 200 mL of LB mediumat 1% in a 1 L Erlenmeyer
flask. The culture was allowed to grow (200 rpm @ 37 °C) for
24 h, after which it was centrifuged at 10000g at
4 °C for 20 min, the supernatant decanted, and the pellet resuspended
in a separate 1 L flask with 200 mL of chemically defined sporulation
medium (CDSM, composition included in the Supporting
Information)[30] and allowed to grow
(200 rpm @ 37 °C) until the culture exhibited at least 80% spores
via phase contrast microscopy (between 3 and 10 days). For partially
deuterated spores, cultures were inoculated into 25% D2OLB medium and resuspended in 25% D2OCDSM for sporulation.
Once the sample had sufficient spores, the culture was spun down,
washed 1× with sterile Milli-Q water, spun down, and resuspended
in a centrifuge tube in 20 mL of sterile 50% v/v EtOH:H2O. The resuspended spores were shaken at 200 rpm at 25 °C for
2 h to kill any remaining vegetative cells. The spores were then centrifuged
3X (10000g, 4 °C, 20 min); the supernatant was
decanted and the spores were washed 3X with 20 mL aliquots of sterile
Milli-Q water between each centrifugation. After washing, the spores
were resuspended in a fresh 20 mL aliquot of sterile water and stored
overnight at 4 °C; the following morning the culture was spun
down and resuspended in fresh sterile water. The final step of purification
involved delivery of the spores into a sterile centrifuge tube via
syringe filtration using 3.1 and 1.2 μm glass fiber filters
connected in series. The purified spores were centrifuged (10000g, 4 °C, 20 min), the supernatant was decanted, and
the pellet was resuspended and transferred to a glass vial with 99%
D2O (total volume 8 mL). The spore suspension was frozen
with liquid nitrogen and lyophilized for 2 days to form a fluffy,
charged white or off-white powder, which was stored at −20
°C until use. Spores were packed into 5 mm ceramic magic-angle-spinning
rotors and sealed with O-ring caps for NMR experiments.For
deuterium–hydrogen exchange experiments, the lyophilized
deuterated spores were transferred to a sterile 15 mL Falcon tube
and resuspended in sterile Milli-Q water. The tube was sealed with
a plastic cap, covered in parafilm, and stored at 4 °C with occasional
shaking for 1 week. The exchanged spores were transferred to a centrifuge
tube and spun at 10000g (4 °C, 20 min). Water
was decanted, and the wet spores were resuspended with sterile Milli-Q
water to aid their transfer into a glass vial prior to lyophilization
as described above. Spores for hydrogen–deuterium exchange
experiments were prepared in a similar manner. Lyophilized spores
grown in protonated media were suspended in sterile D2O
for 1 week before drying.
Synthesis of Amorphous and Crystalline Calcium
Dipicolinate
(CaDP) and Deuteration of BSA
Deuterated amorphous calcium
dipicolinate trihydrate was prepared by modifying the procedure of
Johnson et al.[31] to use 99% D2O. After dissolving the dipicolinic acid and adding calcium hydroxide
to a pH between 9 and 10, the heated solution was allowed to cool
to room temperature and then stored in a desiccator for 4 days. Subsequently,
the solution was further dried via lyophilization for 24 h. The resulting
powder was packed into an NMR rotor to collect 2H NMR data.Crystalline deuterated CaDP was prepared using a modification of
the procedure by Bailey et al.,[32] replacing
deionized water with 99% D2O. Slight heating was necessary
to dissolve the dipicolinic acid. After addition of Ca(OH)2, the solution was transferred into several 13 mm OD test tubes and
stored in a desiccator for ∼1 month. Needle-shaped crystals
began to form within 1–2 weeks. The crystal structure was determined
by X-ray crystallography and found to have the same space group and
similar dimensions as previously reported data.[33] Details of the X-ray crystallography procedures and results
are provided as Supporting Information.Bovine serum albumin (BSA, Sigma-Aldrich, Inc.) was dissolved in
99% D2O (100 mg/8.0 mL), stirred for 24 h at 4 °C,
and lyophilized for 5 days before packing in a 5 mm rotor and collecting
a deuterium solid-state echo (SSECHO) spectrum. A second sample was
prepared by dissolving 100 mg of BSA in 8 mL of D2O, mixing
for 24 h, and drying via lyophilization for 19 days.
NMR Experiments
Quadrupolar echo 2H NMR
experiments were collected by placing the filled ceramic rotor into
a Varian 5 mm wide-line NMR probe and inserting the probe into an
Oxford 400 MHz (9.4 T) magnet (2H frequency = 61.424 MHz).
Data was collected using a Varian Unityplus console
and VNMR 6.1C software on a Sun workstation. The pulse sequence (SSECHO,
90–τ1–90–τ2–acquire)
used a pulse width of 6 μs, recycle delay of 120 s, τ1 of 60 μs, and τ2 of 50 μs. The
acquisition time was 40 ms. Deuterium NMR calibrations were performed
with malonic acid-d4 and pure D2O samples to optimize the 90° pulse width and verify the appropriate
spectral appearance of our calibration standards. The spore samples
were studied at room temperature. The 2H T1 for immobilized water was found to be 24 s using a sample
of frozen D2O (−40 °C) cooled by a stream of
nitrogen gas chilled by a XRII FTS refrigeration unit. Data analysis
was accomplished using VNMR 6.1C provided by Varian Inc.Variable-temperature 2H NMR experiments were performed by delivering heated dry
air to the sample. The sample was held at the desired temperature
for 15 min prior to data acquisition. Data was collected with the
SSECHO pulse sequence using a delay time of 120 s for each of the
2000 transients (66 h data collection time). An initial spectrum was
collected at 21 °C followed by heating to 50 °C. A spectrum
collected at this temperature was compared to the 21 °C spectrum,
and the sample was then cooled back to 21 °C. Another spectrum
was collected to see whether changes that occurred, if any, at 50
°C were reversible. Subsequent spectra were also collected at
100 and 21 °C, respectively.
Results
Deuterium–Hydrogen
Exchange
The deuterium quadrupolar
echo NMR spectrum of partially deuterated B. subtilisATCC 6051 spores is shown in Figure 1A. There
are three distinct features that are present in this spectrum: feature
I, a sharp singlet peak at 0 Hz referenced to a liquid D2O standard; feature II, a Pake doublet with a separation of approximately
32 kHz; and feature III, another Pake doublet with a 120 kHz separation.
A second deuterium NMR spectrum was collected after the B.
subtilis ATCC 6051 spores were soaked in H2O (Figure 1B). Here, signals for features I, II, and III are
present, although the intensity is lower due to either replacing labile
deuterons with protons or sample loss after repacking the postexchange
spores. After correcting for the latter through scaling of the spectrum
by the same proportion as sample lost, an overlay of the pre- and
postexchange spectra (Figure 1C) shows a diminution
of features I and II while feature III is unchanged.
Figure 1
2H solid-state
NMR spectrum of 25% D2O-labeled B. subtilis ATCC 6051 spores (A); of the same sample after
one-week’s exchange with H2O (B); A and B overlaid
on the same axis and scaled for sample loss (C). Three main features
(I, II, III) are apparent in the spectra, with feature I decreasing
most after exchange. Spectra were collected at room temperature over
10,000 scans with a delay time of 120 s.
2H solid-state
NMR spectrum of 25% D2O-labeled B. subtilisATCC 6051 spores (A); of the same sample after
one-week’s exchange with H2O (B); A and B overlaid
on the same axis and scaled for sample loss (C). Three main features
(I, II, III) are apparent in the spectra, with feature I decreasing
most after exchange. Spectra were collected at room temperature over
10,000 scans with a delay time of 120 s.Using the same methodology, spores of B. subtilis 1A578 were also studied using deuterium–hydrogen exchange
via quadrupolar 2H NMR. Figure 2 shows the spectra for spores of B. subtilis 1A578
grown in 25% deuterated media before (A) and after (B) a one-week
exchange with H2O, and a comparison of the two spectra
on the same axis (C) corrected for mass loss during sample preparation.
The 1A578 spores appear to have sharper features II and III than those
of ATCC 6051. Likewise, the comparison in Figure 2C shows that feature III is not affected by soaking in H2O whereas features I and II become smaller.
Figure 2
Deuterium quadrupolar
echo NMR spectra of B. subtilis 1A578 spores: grown
in 25% D2O media (A); same sample
after one-week exchange with H2O (B); A and B shown on
the same axis and scaled for mass (C). Three main features (I, II,
III) are apparent indicating signals arising from different deuterons
in the spore; feature I exhibits the largest decrease after exchange.
Spectra were collected at room temperature over 10,000 scans with
a delay time of 120 s.
Deuterium quadrupolar
echo NMR spectra of B. subtilis 1A578 spores: grown
in 25% D2O media (A); same sample
after one-week exchange with H2O (B); A and B shown on
the same axis and scaled for mass (C). Three main features (I, II,
III) are apparent indicating signals arising from different deuterons
in the spore; feature I exhibits the largest decrease after exchange.
Spectra were collected at room temperature over 10,000 scans with
a delay time of 120 s.
Hydrogen—Exchange Deuterium NMR of Spores
Spores
of both strains of B. subtilis, ATCC 6051 and 1A578,
grown in protonated media, were soaked in 99% D2O for 1
week and lyophilized, and quadrupolar echo 2H NMR spectra
were collected. These spectra are shown as Figures 3 and 4, respectively. The spectrum
of wild-type (ATCC 6051) spores shows a strong central feature I,
an area of intermediate line broadening, and significant broadening
at the baseline while features II and III are not observed. The chloramphenicol-resistant
(1A578) spores produce a deuterium spectrum that is dominated by feature
I and does not have features II and III, and broadening of the baseline
is present but less intense.
Figure 3
Deuterium solid-state spectrum of B.
subtilis ATCC
6051 spores grown in protonated medium and soaked in D2O for one week’s exchange (room temperature, 120 s delay,
10,000 transients). Features II and III are not apparent, leaving
only feature I and a broad signal.
Figure 4
Deuterium solid-state NMR spectrum of spores of B. subtilis 1A578; this strain exhibits a different line shape after H-to-D
exchange than B. subtilis ATCC 6051. Although the
same overall changes (no features II or III and broad signal) are
observed, the broad feature is much less intense. The spectrum was
collected at room temperature with a 120 s delay time and a total
of 7178 transients.
Deuterium solid-state spectrum of B.
subtilis ATCC
6051 spores grown in protonated medium and soaked in D2O for one week’s exchange (room temperature, 120 s delay,
10,000 transients). Features II and III are not apparent, leaving
only feature I and a broad signal.Deuterium solid-state NMR spectrum of spores of B. subtilis 1A578; this strain exhibits a different line shape after H-to-D
exchange than B. subtilisATCC 6051. Although the
same overall changes (no features II or III and broad signal) are
observed, the broad feature is much less intense. The spectrum was
collected at room temperature with a 120 s delay time and a total
of 7178 transients.
Bovine Serum Albumin Spectra
The spectra of BSA lyophilized
for 5 days and for 19 days are shown in Figures 5B and 5C, respectively. The mobile D2O peak is reduced in the 19-day spectrum versus the 5-day spectrum,
with little to no difference in the broader signal. These spectra
are identical to previously reported spectra of a deuterated enzyme,
subtilisin.[34] However, we previously published
a spectrum of deuterated BSA prepared under different conditions.[35] This spectrum is shown in Figure 5A and shows a Pake doublet with a large separation, similar
in width to feature III in Figures 1 and 2. For this sample, the protein:water ratio (500
mg:10 mL) and drying (1 day) were insufficient to achieve complete
deuterium exchange and removal of excess water. Hence, Figure 5A has a lower SNR and the additional set of Pake
doublets are not seen in the samples with extended drying (Figure 5B and 5C).
Figure 5
A comparison of one sample
of deuterated lyophilized bovine serum
albumin lyophilized 1 day (A) with a second sample (BSA) dried for
5 days (B) and 19 days (C). The Pake doublet observed in A is attributed
to bound water that vanishes when the sample is dried for longer periods
of time (B, C). Spectra were collected at room temperature with a
delay time of 120 s over 4364 transients (A) or 10,000 transients
(B, C).
A comparison of one sample
of deuterated lyophilized bovine serum
albumin lyophilized 1 day (A) with a second sample (BSA) dried for
5 days (B) and 19 days (C). The Pake doublet observed in A is attributed
to bound water that vanishes when the sample is dried for longer periods
of time (B, C). Spectra were collected at room temperature with a
delay time of 120 s over 4364 transients (A) or 10,000 transients
(B, C).
Deuterium NMR Spectra of
Calcium Dipicolinate
Figure 6 shows
the quadrupolar echo deuterium NMR spectra
of the amorphous and crystalline forms of calcium dipicolinate (CaDP)
respectively. The amorphous sample presents itself as having a Pake
doublet with a peak splitting of 116 kHz, with a central peak that
is broader than that observed in the B. subtilis spores
(Figure 6A). When a smaller sample of the amorphous
CaDP is subjected to additional drying (Figure 6B), the Pake doublet disappears and the spectrum resembles that of
the deuterated BSA samples (Figures 5B and 5C). The crystal form exists as a trihydrate, and,
when isolated from deuterated water, crystalline CaDP·3D2O does not show a central peak (feature I), instead revealing
a Pake doublet with a peak splitting of 31 kHz that broadens as it
nears the baseline (Figure 6C). The crystal
structure determined using a small portion of the CaDP·3D2O NMR sample is shown in Figure 7.
Figure 6
2H NMR quadrupolar echo spectrum of amorphous deuterated
calcium dipicolinate trihydrate dried for 24 h (A), a separate amorphous
CaDP sample dried for 48 h (B), and crystalline calcium dipicolinate
trihydrate (C). A Pake doublet surrounds a broad mobile D2O peak in A, which is not evident with longer drying on the other
amorphous sample (B); crystalline CaDP shows a Pake doublet at ∼31
kHz indicative of limited motion (C). Spectrum A was collected at
room temperature with a delay time of 120 s over 7768 transients;
B over ∼2200 transients; C over 10,000 transients.
Figure 7
Crystal structure of deuterated calcium dipicolinate trihydrate
(CaDP·3D2O), as shown in a thermal ellipsoid plot,
showing that it forms a dimer as a crystal.
2H NMR quadrupolar echo spectrum of amorphous deuterated
calcium dipicolinate trihydrate dried for 24 h (A), a separate amorphous
CaDP sample dried for 48 h (B), and crystalline calcium dipicolinatetrihydrate (C). A Pake doublet surrounds a broad mobile D2O peak in A, which is not evident with longer drying on the other
amorphous sample (B); crystalline CaDP shows a Pake doublet at ∼31
kHz indicative of limited motion (C). Spectrum A was collected at
room temperature with a delay time of 120 s over 7768 transients;
B over ∼2200 transients; C over 10,000 transients.Crystal structure of deuterated calcium dipicolinate trihydrate
(CaDP·3D2O), as shown in a thermal ellipsoid plot,
showing that it forms a dimer as a crystal.
Variable-Temperature Deuterium NMR
Figure 8 shows various spectra collected during the VT NMR
experiment involving B. subtilisATCC 6051. The first
spectrum collected (top left) is similar to that of Figure 1A, with variations caused by lower signal-to-noise
ratio in these spectra collected with 2000 scans (66 h) versus 10,000
scans (333 h). When heated to 50 °C there are only minor differences
observed, mostly a slight decrease in the Pake doublet features II
and III. This change appears to reverse itself when the sample is
cooled back to 21 °C. Feature I becomes dominant and features
II and III become reduced when the sample is heated to 100 °C.
As before, the spectrum resumes its previous appearance when cooled
back to 21 °C (bottom right).
Figure 8
Spectra obtained for the variable-temperature
deuterium NMR of
25% deuterated B. subtilis ATCC 6051 spores. Very
slight changes are seen when the spores are heated to 50 °C and
cooled; larger changes to the line shape are apparent when heated
to 100 °C but appear to revert themselves when cooled to the
original temperature. These changes and their reversion to previous
line shape are suggestive of glass-like transitions inside a rigid
spore core. Spectra were collected with a delay time of 120 s and
2000 transients at the temperatures indicated.
Spectra obtained for the variable-temperature
deuterium NMR of
25% deuterated B. subtilisATCC 6051 spores. Very
slight changes are seen when the spores are heated to 50 °C and
cooled; larger changes to the line shape are apparent when heated
to 100 °C but appear to revert themselves when cooled to the
original temperature. These changes and their reversion to previous
line shape are suggestive of glass-like transitions inside a rigid
spore core. Spectra were collected with a delay time of 120 s and
2000 transients at the temperatures indicated.
Discussion
Assignment of Deuterium NMR Spectra
The distinct features
(I, III, and III) in the deuterium quadrupolar echo NMR spectrum of
partially deuterated B. subtilisATCC 6051 spores
(Figure 1A) are assigned by comparison to samples
of known composition. Feature I is attributed to deuterons with isotropic
motion, possibly from water that is mobile or very dynamic in its
environment; future experiments will examine feature I in more detail
to study the T1 of this peak. Feature
II has a Pake doublet separation (32 kHz) similar to that seen in
the crystalline calcium dipicolinate sample, whose crystal structure
shows water coordinated to the metal ion, carboxylic acids, and nearby
water molecules. However, feature II could also be due to nonlabile
deuterons incorporated in biomolecules. Using a growth medium with
25% D2O, our samples will have partial deuteration of every
molecule. Thus, methyl groups will be found as −CH2D and give a Pake pattern with a 38 kHz peak separation.[36] The Pake pattern is reduced from the typical
140–220 kHz separation found in organic compounds[37] due to free rotation. It is well-known that
−CD3 molecules in proteins and peptides present
a similar NMR spectrum.[38] Labile water
associated with the lipid bilayers, such as the spore membrane, gives
a peak separation of a few kilohertz while deuterons in the lipid
itself produce a larger separation, on the order of 30 kHz.[39,40] Feature II could also be interpreted as the result of C2 symmetry
jumps; this is common in crystalline hydrates[41] and, if applicable to calcium dipicolinate trihydrate, would tie
feature II to the spore core as well through the CaDP·3H2O.Attribution of feature III (peak separation of 120
kHz) to immobilized water molecules has been disputed and was suggested
to arise from labile deuterons in biomolecules.[28] We have prepared and studied labile deuterons in the BSA
protein sample, and the 2H NMR spectrum does not have feature
III present after extended drying (Figures 5B and 5C). Spectra similar to Figure 5B have been reported for hydrated subtilisin enzyme
isolated from a D2O solution. This sample contains labile
O–D and N–D groups along with a layer of hydration water
strongly associated with the enzyme.[34] For
a sample of BSA dried for 1 day, the spectrum shows a Pake doublet
with a separation similar to that of feature III. We attribute the
Pake doublet in Figure 5A to water molecules
(HOD) bound to the protein sample. These HOD molecules are not firmly
attached to the protein as they can be removed with vacuum drying
(Figures 5B and 5C).
The outer edges of the Pake doublet in Figure 5A are less sharp than the Pake doublet of frozen water (Figure 9C). This indicates that excess water associated
with BSA is immobilized in a heterogeneous fashion. The variation
in chemical environment can be due to localized differences in numbers
of neighboring water molecules and the hydrogen bonding network. Similar
observations are made with CaDP samples with a wide Pake doublet (Figure 6A) that is removed with further drying (Figure 6B).
Figure 9
A comparison of the Pake doublets of B. subtilis 1A578 (A) versus crystalline CaDP·3D2O (B), bulk
frozen D2O (C), and amorphous CaDP·3D2O
(D), indicating the likelihood of the spore Pake doublets arising
from immobilized core components. In this model feature III arises
from bound water similar to that of amorphous CaDP but unlike bulk
water; feature II may arise from methyl rotations or from the crystalline
CaDP·3D2O signal.
A comparison of the Pake doublets of B. subtilis 1A578 (A) versus crystalline CaDP·3D2O (B), bulk
frozen D2O (C), and amorphous CaDP·3D2O
(D), indicating the likelihood of the spore Pake doublets arising
from immobilized core components. In this model feature III arises
from bound water similar to that of amorphous CaDP but unlike bulk
water; feature II may arise from methyl rotations or from the crystalline
CaDP·3D2O signal.The shape of feature III (Figures 1 and 2) shows that these deuterons are in
an environment
of substantial homogeneity compared to water associated with amorphous
proteins or CaDP. If these deuterons are protein-associated water,
they would be very susceptible to a temperature-induced increase in
isotropic motion. These dynamics should be reversible and would not
require the protein itself to undergo isotropic motion. Such behavior
is shown after heating the spore to 100 °C and cooling it back
down to 21 °C (Figure 8). The dramatic
change of the anisotropic feature III into the isotropic signal of
feature I supports our view that these deuterons are in rigid water
associated with biomolecules, and their increased motion does not
require a diffuse liquid-like state. Within a few degrees of the D2O melting point (3.8 °C), water molecules flip between
ice crystal sites yielding a narrow isotropic peak. Wittebort et al.[42] used variable temperature 1H and 2H NMR studies to examine molecular dynamics in ice. In the
hexagonal form of ice, I, the central water molecule is bound to 2 neighboring H atoms (via
the oxygen) and 2 neighboring oxygen atoms (via the protons). These
four bonds form a tetrahedron around the central water molecule. In
Wittebort’s sample, a narrow line is seen at −6 °C
and attributed to isotropic reorientation within the ice lattice.
At −24 °C, the narrow line is very small due to a reduction
in dynamics. Our spore samples were analyzed at room temperature,
and thus bulk ice is not expected, although the water could be dynamic
within a rigid lattice; the relatively small size of the narrow line
at −6 °C in Wittebort’s sample implies that its
contribution to feature I would be negligible. Observation of immobile
water at room temperature is not without precedence. A mixture of
mobile and solid water has been reported for hydrated minerals. The
sodium-silicate kanemite has three bound water molecules which move
between tetrahedral binding sites within the mineral structure, though
some water is found in between layers of the mineral.[41,43] Rigid water in the kanemite sample produces a Pake pattern separation
>190 kHz due to Na–O–D and Si–O–D bonds
at −120 °C. At room temperature, a weak powder pattern
is observed symmetric to an isotropic peak, indicating less mobile
water undergoing jumps. Thus, water in nonbulk environments generates
Pake patterns with varying quadrupolar coupling constants. Li et al.
report that water in cornstarch samples produces Pake pattern separations
less than 144 kHz.[44] Thus, it is not unexpected
that excess water bound to proteins could give a Pake pattern splitting
of 120 kHz compared to that of 144 kHz for bulk ice.Dimers
of α-truxillic acid form with two carboxylic acid
groups arranged in a linear fashion. The result is a pair of O–H···O=C
hydrogen bonds and replacement with deuterium producing a sharp Pake
doublet with a 117 kHz splitting,[45] but
only when those carboxylic acids are in the linear arrangement. We
do not believe a homogeneous chemical environment such as that found
in α-truxillic acid, however, produces feature III in bacterial
spores. There are numerous carboxylic acid groups in the spore proteins,
but they form hydrogen bonds with amide groups. Carboxylic acid groups
in the peptidoglycan are arranged in a random disordered fashion and
would not be expected to adopt a homogeneous linear conformation.
The crystalline calcium dipicolinate unit cell shows one water bond
to a carboxylic acid group, yet we do not see feature III in Figure 6C. Most of the carboxyl groups are involved in direct
chelation of the Ca2+ ions, reducing the occurrence of
O–D···O=C hydrogen bonding.Another
possible source of feature III is nonlabile deuterons found
as rigid C–D groups.[36,46] This labeling would
be widespread among the various proteins, DNA, peptidoglycan, and
membranes found in a mature spore. These deuterons could be responsible
for the remaining portion of feature III at 100 °C not converted
to the isotropic feature I. Thus, we believe that feature III is due
to both nonlabile deuterons in biomolecules and rigid water associated
with biomolecules. Due to the complexity of the spore sample and the
heterogeneous nature of the deuterium spectrum, with many components,
we were unable to generate a satisfactory quantitative estimate of
each component in the spore. As seen with previous reports,[28] quantitative assignment would be dependent on
the level of hydration. Nonetheless, our qualitative study provides
additional insight in the spore core water environment. Future studies
will attempt quantification through line shape simulation and comparison
of simulated spectra with the spectra reported here.
Sites Accessible
to Exchange
The exchange of accessible
deuterons with H2O is demonstrated in Figure 1 using spores of B. subtilisATCC 6051. The
decrease in the mobile D2O peak (feature I) is expected;
mobile D2O would exchange freely with exogenous water.
However, a significant fraction of mobile water is unreachable by
external H2O. These deuterons can be both core and noncore
water. In the latter case, deuterons are protected from exchange by
protein conformations that trap water in a rigid matrix. Dormant spores,
even hydrated, would maintain proteins in tight conformations which
would limit access and exchange as a means of hindering chemical attack.
If water can cross the membrane, some core-associated deuterons must
be protected from exchange by protein conformations or the transport
and exchange of water is very slow compared to the 7-day exchange
period. As the exchange was carried out in a water suspension, excess
water would cause full hydration and swelling of the spore samples,
although in a state of dormancy active water transport would cease
to function. A rigid core model would protect water from exchange,
but it is also possible that a rigid core could transition into a
gel state with excess hydration. If this were the case, some mobile
deuterons in protein/DNA/CaDP environments must be inaccessible to
gel water, or the core is a mixture of gel and rigid domains restricting
access to exchange sites. Nevertheless, this analysis does not preclude
the opportunity for gel core water to be present with dynamics different
than bulk water.[28] However, experiments
targeted to study core-water dynamics after H-to-D exchange would
report only accessible water while trapped water would be invisible
and not contribute to relaxation rate analysis. From the data in Figures 1 and 2, this trapped water
has a noticeable contribution to feature I. Thus, Kaieda et al.[28] do not report all possible water in hydrated
spores.However, it is also possible that the membrane prevents
water diffusion. In this scenario, the mobile water peak observed
here and in previous work would be due to noncore water molecules
protected from exchange by protein conformations. Unfortunately, changes
to feature I after exchange cannot be used to evaluate whether the
mobile water peak is due to core or noncore water. It is not unreasonable
that the lipid bilayer would undergo significant structural and/or
biochemical changes during sporulation to protect the core from dehydration
or attack by sporicidal agents through the removal or closure of transmembrane
channels and transport proteins, or structural changes to the phospholipids
themselves creating a tighter network. Deuterium NMR is commonly used
to examine the motion of lipid membranes and dynamics within the hydrophobic
tails[47−53] as well as other relevant biomolecules such as DNA.[54] If the lipid bilayer deuteron signals could be isolated
from other components in the spore, these experiments could be used
in the future to elucidate such changes. After lyophilization, the
samples are exposed to atmospheric moisture during the 2-week time
period required to collect a deuterium NMR spectrum. The rotor, approximately
half to three-quarters full, allows for water vapor in the headspace
to penetrate the spore and continue exchange processes. We do not
detect changes in the spectrum over time or after recollection of
prior data with the same sample. Thus, atmospheric H2O
is not able to access exchangeable deuterons. Drying may cause the
spore to acquire hydrophobic properties in the coat protein layers
or membrane or change from a gel to rigid core.The inner Pake
doublet (feature II) also decreases, indicating
some of these deuterons are in an environment susceptible to exchange.
No change would be seen for nonlabile deuterons in biomolecules created
in the culture and sporulation media. If the spore core is impenetrable,
water in the calcium dipicolinate trihydrate would remain after exchange
and contribute to feature II, if the core CaDP has a structure similar
to the crystalline material produced in our laboratory. It is also
possible that some of the water associated with CaDP is subject to
exchange, perhaps on the exterior of crystallites, whereas most of
the water in CaDP is protected. Kaieda et al.[28] proposed that these signals could be due to deuterated methyl groups;
similar line shapes were seen in magic-angle-spinning (MAS) spectra
of deuterated valines inside of glycophorin A.[38]Interestingly, feature III is relatively unchanged
after soaking
in H2O. If this Pake doublet were, as suggested, due solely
to labile deuterons,[28] the expected result
of a deuterium–hydrogen exchange would be a loss of deuterium
signal in the spectrum, or at least a decrease in intensity proportional
to that seen for features I and II. Thus, these deuterons are either
nonlabile or nonaccessible to external water. As described above,
a glassy core would protect labile waterdeuterons in the core. Additionally,
if linear hydrogen bonds such as in α-truxillic acid dimers[45] are responsible for feature III, they may persist
in water if the biomolecules or peptidoglycan do not rearrange in
response to swelling from excess hydration. This seems unlikely as Bacillus spores change shape/size in response to external
water.[55] If these hydrogen bonds are susceptible
to exchange, and responsible for feature III, then they would be nonexistent
in the postexchange spectrum. Thus, the persistence of feature III
after the D-to-H exchange process supports either bound water molecules
in the spore or the partial deuteration of carbon atoms found in various
biomolecules. As described above, we believe that both species are
present.Similar behavior was observed in deuterium–hydrogen
exchange
experiments with a sample of B. subtilis 1A578 spores,
as seen in Figure 2. This indicates that changes
to features I and II, and the persistence of feature III, are not
a property confined to the ATCC 6051 strain. Nevertheless, the spores
of the chloramphenicol-resistant and wild-type strains show dramatic
differences when subjected to hydrogen-to-deuterium exchange experiments.
In these experiments, spores were produced using protonated growth
and sporulation media. Labile, and accessible, protons were replaced
with deuterium by soaking in sterile D2O.The postexchange
spectra for ATCC 6051 spores show a line shape
(Figure 3) lacking the sharp features II and
III of Figure 1A. Hydrocarbons of biomolecules
and lipid groups would not contribute to the post H-to-D exchange
spectra. The lack of a strong feature II reinforces the conclusion
that deuterons responsible for features II and III are not labile
(perhaps in C–D or CHD groups) or not easily accessible for
exchange (located in the core and/or protected by proteins). However,
the 1A578 spores produce a spectrum (Figure 4) dominated by mobile water (feature I). The broadened baseline has
a shape similar to that of the wild-type spores (Figure 3) but lower in intensity. Proteins external to the core may
have a structural conformation that protects labile protons from exchange
with deuterons. A proteomics study with the chloramphenicol-resistant
1A578 found 85 proteins already identified from Bacillus species and 69 novel proteins.[56] Thus,
unique protein structures may exist that resist exchange with deuterium,
a possibility that warrants further study. Both spore samples were
handled in a similar fashion, thus comparison of the spectra indicates
that 1A578 has a greater fraction of mobile water. This could result
from the chloramphenicol-resistant spores retaining a greater mass
of mobile water, having a mobile water fraction with greater resistance
to drying, or the labile deuterons being predominately found as mobile
water. These deuterons obviously have rapid isotropic motion, but
it is not clear if they are located in the core, noncore regions,
or both.If feature III of the spore deuterium NMR spectrum
in Figure 1A was indicative of labile deuterons,
asserted by
Kaieda et al.,[28] the spectrum observed
in Figure 3 should look identical (or nearly
so) to that seen in Figure 1A. Instead, Figure 3 shows a feature II that is practically indistinguishable
from the central mobile deuterium peak and broad shoulders instead
of the sharp Pake doublet seen in feature III of Figure 1A. Likewise, if feature III were the result of O–D···O=C
hydrogen bonds susceptible to exchange, the H-to-D experiment should
produce a sharp Pake doublet. Instead, we speculate that the broad
signals in Figures 3 and 4 are from labile deuterons of proteins. When the spectra in Figures 3 and 4 are compared to a
spectrum of BSA, the result is a nearly identical overlap for the
wild-type 6051 spores (Figure 10). However,
with its large fraction of mobile water, the resistant 1A578 spores
(Figure 11) do not overlap with the BSA spectrum
unless the protein spectrum is reduced in height. While the scaling
factor was 3.3, this number is somewhat meaningless as we are not
convinced that labile deuterons in the coat proteins of 1A578 spores
would be exchanged to a similar degree as labile deuterons in a homogeneous
solution of BSA.
Figure 10
Postexchange B. subtilis ATCC 6051 spore
spectrum
(Figure 3) to which the five-day-dried BSA
spectrum (Figure 5B) has been overlaid. BSA’s
spectrum fits very well to the spectrum of the whole spore.
Figure 11
Postexchange B. subtilis 1A578 spore spectrum
(Figure 4) overlaid on the same spectrum as
the five-day lyophilized deuterated BSA (Figure 5B). BSA’s spectrum fits well to the broad peak feature in
1A578 but less so to the mobile water peak feature. The difference
in line shape between this and Figure 10 is
attributed to structural changes in B. subtilis 1A578
resulting in higher protein conformational homogeneity and may be
responsible for the differences in line shape overall between B. subtilis 1A578 and B. subtilis ATCC
6051.
Postexchange B. subtilisATCC 6051 spore
spectrum
(Figure 3) to which the five-day-dried BSA
spectrum (Figure 5B) has been overlaid. BSA’s
spectrum fits very well to the spectrum of the whole spore.Postexchange B. subtilis 1A578 spore spectrum
(Figure 4) overlaid on the same spectrum as
the five-day lyophilized deuterated BSA (Figure 5B). BSA’s spectrum fits well to the broad peak feature in
1A578 but less so to the mobile water peak feature. The difference
in line shape between this and Figure 10 is
attributed to structural changes in B. subtilis 1A578
resulting in higher protein conformational homogeneity and may be
responsible for the differences in line shape overall between B. subtilis 1A578 and B. subtilis ATCC
6051.
Rigid Spore Core from Variable-Temperature
Deuterium Solid-State
NMR
We speculate that the spore core is more a solid than
a gel-like state, but exchange experiments alone do not provide enough
evidence to distinguish the physical state of the core. Instead, we
base our analysis on variable-temperature data collected to provide
this distinction. Figure 8 shows the results
of the VT NMR experiments with B. subtilisATCC 6051
spores. It is evident that the mobile D2O peak does not
increase perceptibly when the sample is heated from 21 to 50 °C.
However, when cooled back to 21 °C and heated to 100 °C,
the central peak intensity increases dramatically. The high temperature
causes significant portions of the spore to undergo isotropic, or
nearly isotropic, motion. Other portions of the spore retain anisotropic
behavior as evidenced by the persistence of features II and III after
heating. The lack of a dramatic change in features II and III at 50
°C suggests that components able to undergo isotropic motion
are not affected by the moderate heating. This analysis does not support
a gel-like core with a high mobile water content, which would be expected
to show gradual changes as the temperature is increased. The rigid
core analysis is similar to the predictions made by Sapru[22] indicating glass-transition temperatures in
between 50 and 100 °C for various Bacillus strains.The analysis of our VT NMR data builds upon our assignment of spectra
to different components, drying effects on the spectra, and changes
caused by H/D or D/H exchange. As discussed below, we suggest a spore
model with a rigid core where CaDP and biomolecules are rigid (features
II and III) with a smaller fraction of deuterons existing as nonrigid,
perhaps mobile, water (feature I). Data collected at 100 °C suggests
that there is a phase change between 50 and 100 °C responsible
for the large increase in the isotropic deuteron signal. The higher
fraction of mobile deuterons could arise from faster dynamics of nonlabile
deuterons in biomolecules. Nevertheless, 100 °C is insufficient
to convert every deuteron of features II and III into an isotropic
state. Deuterated peptidoglycan, contributing to feature III, is a
highly cross-linked network and not expected to have large degrees
of freedom, even with heating. Also, these deuterons may exist in
proteins that resist conformation changes at high temperature. Crystalline
CaDP may generate feature II, and work in our lab shows that crystalline
CaDP does not melt in boiling water.When the sample is cooled
back to 21 °C (from 100 °C),
NMR data show that the sample characteristics which generate the room
temperature spectra are nearly identical to those of the initial spectra
collected at 21 °C prior to heating. This suggests that changes
in the deuteron environment due to heating are reversible. Deuterated
biomolecules would return to an immobile state, but we do not know
if these biomolecules have been denatured to render the spore inert.
Previous work by the Setlow Lab has shown that the viability of B. subtilis spores is relatively unaffected by dry heating
to 100 °C.[20] The viability of these
spores also suggests that the protein denaturation is modest and would
not generate the isotropic signal at 100 °C. Thus, changes to
feature III in Figure 8 are attributed to bound
water molecules where heating increases their motion to generate an
isotropic peak, yet cooling allows them to revert to the bound state
without affecting the viability of the spore itself. From this viewpoint,
the VT NMR data suggest the presence of bound water contributing to
feature III in contrast to the assertions promoted by Kaieda et al.Proton NMR has been used to examine water in spores; however, the
combination of heterogeneous samples and narrow chemical shift dispersion
creates difficulties in assigning spectra. Nevertheless, the water
will generate a very strong signal, and its chemical environment will
influence spin relaxation rates. Bradbury et al. reported equal amounts
of water in core and cortex + coat regions. Water was found to be
both mobile and immobile. After separating the coat proteins and PG
cortex, the water in these samples was found to be immobile; thus,
mobile water was assigned to the core.[57] Using solid-state NMR spectroscopy, the characteristic 13C resonance for dipicolinic acid (DPA)[58] was detected with cross-polarization in freeze-dried and rehydrated
spores of B. subtilis.[55] CPMAS data reflect those 13C spins that maintain strong
dipolar coupling with nearby 1H nuclei, and thus indicate
limited or absent molecular motion. In contrast, single-pulse MAS
(SPMAS) signals are strongly affected by mobile species where strong
spin–lattice effects cause fast T1 relaxation. Leuschner and Lillford could not detect DPA with 13C SPMAS, demonstrating that the DPA is in a firm rigid lattice,
and rehydration of the core does not increase the molecular motion
of DPA. From these prior studies, the core-specific DPA molecules
may exist in a glassy core with water around the DPA also in an immobile
state. We have shown in Figure 9B that the
trihydrate form of crystalline CaDP produces a deuterium spectrum
with a Pake doublet similar to feature II. This does not prove that
CaDP in the core is crystalline, only that it is possible that CaDP
could adopt a structural arrangement similar to the crystal structure.
It is entirely possible that the CaDP is found as microcrystals in
a glassy matrix of water, DNA, and proteins. The D-to-H exchange experiments
show slight reduction of feature II; this reduction could be due to
exchangeable waters around the CaDP crystallites.Kaieda et
al.[28] reported a quadrupolar
echo 2H NMR spectrum of fully hydrated Mn2+ depleted B. subtilis PS533 spores and concluded that the broad ∼130
kHz feature was entirely the result of labile deuterons in immobilized
proteins and other biomolecules in the spore. Unfortunately, it is
hard to understand how Kaieda et al. could state that there was no
evidence for immobilized water in the core if their data and experimental
techniques could not detect immobile core-associated D2O. Their protocol is essentially a hydrogen-to-deuterium exchange
experiment introducing D2O after growing spores in deuterium-free
media; however, instead of lyophilization, the authors used the wet
spore pellet for their NMR analysis. The line shape observed in Figures 10 and 11 (particularly Figure 11) is similar to that shown in Kaieda et al.[28] for their quadrupolar echo 2H NMR
results. In their paper, the wet cell pellet creates a massive signal
for mobile water. The authors claim that the wet pellet spectrum demonstrates
swollen spores with a gel-like core and that their relaxation rate
measurements reflect the dynamics of water within the core region.
We do not dispute the validity of their data collection or their observation
of water fractions with bulk and nonbulk behavior. We assert that
their measurements are not representative of all water molecules in
the spore sample. The persistence of feature I after D-to-H exchange
suggests that water remains trapped, perhaps in a rigid core as suggested
by our VT NMR data. Samples of 1A578 spores generated from protonated
media and followed by deuterium exchange produce a spectrum (Figure 11) similar to that in Kaieda’s work. We believe
that our spectrum reflects the mobile water content (core and noncore)
of a dried spore sample while Kaieda’s data originates with
fully hydrated samples. Upon closer inspection, their spectrum shows
a broadened baseline similar to that seen with BSA protein reported
here, and we agree that this baseline broadening is due to labile
deuterons in biomolecules. Lastly, Sunde et al.[27] assert that, were the core in a glassy state, there would
be a broad signal apparent on a 2H NMR spectrum of the
spore; however, such a signal would not be detectable using the magnetic
relaxation dispersion experiments as performed. We have observed this
signal in different spore strains, and its width of ∼120 kHz
is consistent with excess water bound to BSA and CaDP.The reason
why the spectra reported in Kaieda et al.[28] are similar to that in Figure 11 (the B. subtilis 1A578), and why there are
differences in the line shape between B. subtilisATCC 6051 and 1A578, may have an explanation. While ATCC 6051 is
a wild-type strain, 1A578 is a variant of B. subtilis 168 that has resistance to chloramphenicol.[29] It is possible that the mechanism of resistance causes structural
changes in the vegetative cells of this strain. Such changes might
manifest themselves in subtle alterations in the spore structure resulting
in the differences in the deuterium NMR spectra of Figures 1–4. The strain used
both in Kaieda et al.’s work[28] and
in the paper by Sunde et al.[27] is B. subtilis PS533, noted as being resistant to kanamycin.[59] Thus, the similarity of the deuterium NMR spectra
reported by Kaieda et al. to B. subtilis 1A578 spectra
shown in Figure 4 may result from introducing
a resistance locus to B. subtilis. From this viewpoint,
it is possible that the data reported by Sunde et al. are also influenced
by a similar phenomenon. It is also noteworthy that features II and
III of the wild-type B. subtilisATCC 6051 spores
(Figure 1) show greater broadening and heterogeneity
compared with the sharper lines seen in Figure 2, data from chloramphenicol resistant strain. Sharper lines result
from enhanced structural homogeneity, and thus the resistance locus
appears to have caused an observable reduction in variation of proteins/biomolecule
conformation. This observation merits additional study with other
bacterial spore strains. It may be possible to apply other sophisticated
biomolecular NMR experiments to explore structural biology via 13C and 15N labeling.
Conclusions
In
this work, we studied deuterium NMR spectra of B. subtilisATCC 6051 and 1A578 with an aim of determining the state of water
inside of the spore core. This was aided by variable-temperature NMR
studies of these species and 2H NMR spectra of calcium
dipicolinate and bovine serum albumin. The overall NMR line shape
of spectra for spores of both B. subtilis strains
indicates that water is in multiple distinct states in the spore.
The wide Pake doublet and the maintenance of its signal through deuterium–hydrogen
exchange indicates that it is bound water, likely associated with
the core. This is also demonstrated through the hydrogen–deuterium
exchange spectra where the only signals that appear on the spectrum
are those similar to bulk proteins such as those seen in deuterated
bovine serum albumin. The difference between the spore spectrum shown
in Kaieda et al.[28] and that of B. subtilisATCC 6051 is postulated to be due to structural
differences perhaps attributable to different proteins or antibiotic
resistances, similar to B. subtilis 1A578. The crystalline
calcium dipicolinate spectrum, when compared to spore spectra, suggests
that the inner Pake doublet may be attributable to immobile core components.
In addition, the lack of proportional increase in the mobile deuterium
signal during the variable-temperature NMR experiments, and the return
of the signal to its original line shape upon cooling, suggest a narrow
transition along the lines predicted by Sapru[22] and Ablett[23] and thus a glassy core.The existence of bound water has come under recent scrutiny[27] from the measurement of deuterium relaxation
rates. These samples were dispersed in deuterated water, and deuterium
relaxation rates were measured with solution-state NMR methods at
different magnetic field strengths. The spin–lattice relaxation
could be explained by molecular motions on the order of 50 ps, which
implies a mobile water fraction within the core. As described by the
authors, this correlation time is too fast for water to be in a “rigid
lattice” environment that would produce a 200 kHz wide spectrum.
However, these water molecules are invisible in their deuterium relaxation
rate measurements. As shown in this work, deuterium wide line NMR
spectroscopy is able to detect both mobile and rigid lattice waters
simultaneously. Our data demonstrate the existence of rigid lattice
water molecules in bacterial spores and that these molecules are in
a different chemical environment than water molecules within the tetrahedral
bonding network of frozen water. Additional data show that immobilized
water in spores is resilient and unable to undergo chemical exchange
with water molecules in exogenous solution.