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The Journal of Neuroscience, January 1, 2001, 21(1):215-220
Nerve Injury Induces a Rapid Efflux of Nitric Oxide (NO) Detected
with a Novel NO Microsensor
Shanta M.
Kumar1,
D.
Marshall
Porterfield4,
Kenneth J.
Muller3,
Peter J. S.
Smith2, and
Christie L.
Sahley1
1 Department of Biological Sciences, Purdue University,
West Lafayette, Indiana 47907, 2 BioCurrents Research
Center, Marine Biological Laboratory, Woods Hole, Massachusetts 02543, 3 Department of Physiology and Biophysics and Neuroscience
Program, University of Miami School of Medicine, Miami, Florida 33136, and 4 Department of Biological Sciences, University of
Missouri at Rolla, Rolla, Missouri 65409
 |
ABSTRACT |
An early step in repair of the leech CNS is the appearance of
endothelial nitric oxide synthase (eNOS) immunoreactivity and NOS
activity, but coincident generation of NO at the lesion after injury
has not been shown. This is important because NO can regulate microglial cell motility and axon growth. Indirect measurement of NO
with the standard citrulline assay demonstrated that NO was generated
within 30 min after nerve cord injury. A polarographic NO-selective
self-referencing microelectrode that measures NO flux noninvasively was
developed to obtain higher spatial and temporal resolution. With this
probe, it was possible to demonstrate that immediately after the leech
CNS was injured, NO left the lesion with a mean peak efflux of 803 ± 99 fmol NO cm
2 sec
1. NO
efflux exponentially declined to a constant value, as described through
the equation f(t) = yo + ae
t/
, with
= 117 ± 30 sec. The constant yo = 15.8 ± 4.5 fmol cm
2 represents a sustained efflux of
NO. Approximately 200 pmol NO cm
2 is produced at
the lesion (n = 8). Thus, injury activates eNOS already present in the CNS and precedes the accumulation of microglia at the lesion, consistent with the hypothesis that NO acts to stop the
migrating microglia at the lesion site.
Key words:
nitric oxide (NO); microglia; nerve injury; NO-selective
microsensor; NO efflux; endothelial nitric oxide synthase (eNOS); leech
CNS; regeneration; nerve repair
 |
INTRODUCTION |
CNS injury triggers a cascade of
sequential cellular events, but repair is ordinarily incomplete in
mammals (Brecknell and Fawcett, 1996
). In contrast, the sequence
of cellular events after neuronal injury in the leech CNS leads to
successful regeneration of axons, repair of synaptic connections, and
restoration of function (Nicholls, 1987
; Modney et al., 1997
). The
microglial cells are important elements of the repair process.
Significantly, their migration to and stopping at the site of injury
appear to be regulated by nitric oxide (NO) (Chen et al., 2000
). Nitric
oxide synthase (NOS) activity at the lesion is one of the earliest
events after crushing or cutting the leech nerve cord (Shafer et al.,
1998
), whereas in mammals, NOS activity reportedly appears only after hours or days. Nevertheless, few measurements of NO release at lesions
have been attempted in other animal species.
Several types of cells express NOS in response to injury and are
assumed to produce NO. In all nervous systems that have been examined,
microglial cells and macrophages are one source of NO (Banati et al.,
1993
). The inducible form (iNOS) reported for mammals has not been
described for leech. Microglia, glia, and nerve-associated muscle cells
in leech express active endothelial NOS (eNOS), beginning within 5 min
after injury (Shafer et al., 1998
), as some muscle cells do in mammals
(Cobbs et al., 1997
). Although neuronal-brain (nNOS) activity has not
been described specifically at lesions, nNOS appears or increases in
various neurons after injury (Fiallos-Estrada et al., 1993
; Vizzard et al., 1995
; Yu, 1997
).
Several techniques are currently available for the detection of NO,
perhaps the best established being the citrulline assay (Bredt and
Schmidt, 1996
). This approach, although suitable for demonstrating the
activity of NOS, has limited spatial resolution. To localize the
production of NO with a spatial resolution of millimeters or
micrometers, a microsensor is required. We have modified existing
designs, as described in Materials and Methods, to produce an
NO-selective microelectrode from carbon fibers with diameters as small
as 5 µm (Cahill and Wightman, 1995
) that combines sensitivity and
selectivity with ease of manufacturing. The reactive surface of this
design is 28 µm2. Furthermore, the
microsensor is used in a self-referencing mode (Smith, 1995
; Smith et
al., 1999
), allowing continuous measurement of flux and flux patterns
without the influence of drift and instabilities. The result is a
robust new method for monitoring the diffusion of NO away from a
source, in this case, the damaged nervous system of the leech.
Preliminary results have also demonstrated sensitivity at the single
cell level (Porterfield et al., 2000
).
Portions of this work have been published previously in abstract form
(Kumar et al., 1999
).
 |
MATERIALS AND METHODS |
Preparation and operations. Adult 4-6 gm adult
leeches (Hirudo medicinalis) were obtained from a commercial
supplier (Leeches USA, Westbury, NY) and maintained in artificial pond
water (Forty Fathoms, 0.5 gm/l H20; Marine
Enterprises, Towson, MD) at 22°C. For experiments, individual
segmental ganglia with connectives were dissected in physiological
saline (Nicholls and Baylor, 1968
) from the animal as shown in Figure
1A and pinned in a dish
coated with silicone rubber (Sylgard 184; Dow Corning, Midland, MI). The connectives were crushed with a pair of fine forceps (Dumont 5)
after recording baseline levels with the NO probe, as shown in Figure
1, B and C.

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Figure 1.
Diagram of the leech, showing the site of crushing
the nerve cord, and the recording arrangement. A, The
CNS of Hirudo medicinalis consists of head and tail
ganglia and 21 segmental ganglia. Each segmental ganglion contains
>400 cell bodies and is linked to its neighbors by thousands of axons
that form the connectives. Connectives were injured by crushing with
forceps (Materials and Methods). B, C,
Photographs of an injured leech nerve cord and the self-referencing NO
probe. During measurements, the probe was moved orthogonally to the
cord over a distance of 30 µm at a frequency of 0.3 Hz in a plane
parallel to the surface of the culture dish. The probe was positioned
at the injury site in B, whereas in C it
was displaced 30 µm. Scale bar, 100 µm.
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Citrulline assay. Production of NO after injury was
determined indirectly by measuring the conversion of
[3H]arginine to
[3H]citrulline using the NOS detect
Assay Kit (catalog #204500; Stratagene, La Jolla, CA). For an
uninjured control condition, an entire nerve cord was dissected from an
adult leech and incubated 30 min at room temperature. In the
experimental, injured preparation, an entire adult nerve cord was
similarly dissected, but the connectives were injured with forceps
between all ganglia before incubation for 30 min at room
temperature. Then each nerve cord was flash-frozen in liquid
N2 and homogenized in buffer containing 25 mM Tris-HCl, pH 7.4, 1 mM
EDTA, and 10 mM EGTA (Sigma, St. Louis, MO). The tissue homogenate was kept on ice, pipetted into 1.5 ml Eppendorf tubes, and spun at 14,000 × g for 5 min at 4°C. NOS
activity was measured in the supernatant. To verify that all samples
contained equal amounts of tissue extract, protein assays were
performed on similarly treated injured and uninjured tissue using the
dotMetric Protein Assay Kit (catalog #2030; Chemicon,
Temecula, CA).
A reaction mixture containing 250 µl of 2× reaction buffer, 50 µl
of 10 mM NADPH, 10 µl of
L-2,3,4,5-[3H]arginine
monohydrochloride TRK698 (1 µCi/µl) (Amersham Pharmacia Biotech, Piscataway, NJ), 50 µl of 6 mM
CaCl2, and 40 µl of H2O was stored on ice. For each reaction, 40 µl of reaction mixture was
combined with 10 µl of tissue extract. The positive control consisted
of 40 µl of reaction mixture added to 10 µl of rat cerebellum extract, previously demonstrated to contain NOS activity (Bredt and
Snyder, 1990
). As a negative control, 5 µl of the inhibitor N
-nitro-L-arginine
methyl ester hydrochloride (L-NAME) (Sigma) was
added to 40 µl of reaction buffer before adding 10 µl of tissue extract. Each reaction was incubated 30 min in reaction buffer at
25°C. The reactions were stopped by adding 400 µl of stop buffer containing 50 mM HEPES, pH 5.5, and 5 mM EDTA. Equilibrated resin (100 µl) was added
to each reaction sample, and the reaction samples were spun at
14,000 × g for 30 sec at 4°C. The
[3H]citrulline in the eluate was
measured as thousands of counts per minute using a 1450 Microbeta Plus
Liquid Scintillation Counter (Wallac, Gaithersburg, MD).
Nitric oxide microsensors. There are several designs of NO
sensors, including one by Malinski and Taha (1992)
that uses selective coatings of monomeric tetrakis (3-methoxy-4-hydroxyphenyl) porphyrin (Ni-TMPP) and Nafion over carbon to exclude reactants such as NO2
and ascorbate. The sensor can be flame-etched to
a fine tip < 1 µm with a reactive surface of ~4
µm2. These porphyrin electrodes have
since been the method of choice in several tissue or single-cell NO
studies ranging from smooth muscle cells, cardiac myocytes (Malinski
and Taha, 1992
; Balligand et al., 1994
), and endothelial cells
(Lantoine et al., 1998
) to human platelets and osteoclasts (Malinski et
al., 1993
; Silverton et al., 1995
). However, in several of these cases,
the finely etched tip, which is difficult to make, has been abandoned
for a more robust fiber design with larger reactive surfaces. Where spatial resolution was not critical, carbon fiber arrays with millimeter reactive lengths were used (Tschudi et al., 1996
). Friedemann et al. (1996)
developed an alternative to the porphyrin coating to produce NO selectivity in which Ni-TMPP is replaced by
o-phenylenediamine (o-PD) to produce an electrode
with excellent characteristics in terms of both sensitivity (35 ± 7 nM) and selectivity against
NO2
and ascorbate. Unfortunately, that probe
is relatively large, with a cylinder diameter of 30 µm and a reactive
area of 104
µm2.
For the measurements of nitric oxide in this study, a carbon fiber
electrode was modified with o-PD and Nafion. This procedure combined the protocol of Friedemann et al. (1996)
, described
above, with a fine carbon fiber described by Cahill and Wightman
(1995)
, resulting in a sensitive and robust microsensor that was
comparatively simple to build. The construction involved encasing a 5 µm carbon fiber (Amoco, Greenville, SC) in a glass microcapillary by
heating and pulling the glass over the fiber (Sutter P97; Sutter
Instrument Company, Novato, CA). The fiber was stabilized and sealed
within the pulled pipette using Epoxylite (Epoxylite Corp.,
Westerville, OH) cured in an oven at 110°C for 5-10 hr. The
electrode was backfilled with a graphite-epoxy paste (PX-grade
Graphpoxy; Dylon Industries, Cleveland, OH), a copper wire was inserted
to make electrical contact with the carbon fiber through the conductive
paste, and the graphite-epoxy paste was cured for 5-10 hr at 110°C.
The excess carbon fiber was chopped with a scalpel and beveled to
30°. Next, o-PD and Nafion were applied to the tip to
impart selectivity for the oxidation of NO (Friedemann et al., 1996
).
Nafion is a polysulfonated Teflon that carries an intrinsic negative
charge, repelling electrochemically active anions (nitrate, nitrite,
and ascorbate). The o-PD coating is thought to impart
selectivity to NO oxidation by size exclusion of noncharged
interferents such as electrochemically active catecholamines. Nafion
(5% in aliphatic alcohols; Aldrich, Milwaukee, WI) was applied in
three coats that were each dried at 110°C for 5-10 min. The
o-PD plating solution contained 5 mM
o-phenylenediamine dihydrochloride (Sigma) with 100 mM ascorbic acid in 100 mM
phosphate buffer, pH 7.4, and was freshly made for each plating
session. The o-PD was plated at a constant +0.90 V potential
until a stable current was obtained.
The modified carbon fiber electrodes (Fig.
2A) had final tip
diameters of 7-8 µm and were operated with an Ag/AgCl return electrode that completed the circuit in solution via a 3 M KCl/5% agar bridge. The polarization voltage
during operation was 0.90 V, and the electrode was operated in
self-referencing mode as described below and for the
self-referencing oxygen microelectrode (Land et al., 1999
). Before and
after use, the electrode was calibrated as described by Friedemann et
al. (1996)
against known concentrations of NO (Fig.
2B, see also below) and tested for specificity
against ascorbic acid.

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Figure 2.
Construction and calibration of the NO-selective
microelectrode. A, The electrode body was constructed by
pulling a heated glass microcapillary around a 5 µm carbon fiber. The
fiber was then sealed into the micropipette with epoxy. A copper wire
was connected to the fiber by filling the back of the electrode with
graphite paste. The tip was finished by beveling it, coating with
Nafion, and plating with o-phenylenediamine.
B, Before each experiment, the electrode was calibrated
with a series of known concentrations of NO, and its selectivity was
tested against ascorbic acid. The slope S of this
calibration curve was used to calculate the flux of NO released at the
injury site according to the Fick equation (see Materials and
Methods).
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The technique was validated with gradients created by the NO donor
S-nitroso-N-acetylpenicillamine (SNAP) (Lander et
al., 1993
). A source micropipette (diameter, 10 µm) was filled with a
0.5% agar solution containing 11.4 mM SNAP in
phosphate buffer, pH 7.4. The gelled source was maintained in a dish
containing phosphate buffer. The gradient was characterized and modeled
so that measured NO flux values could be compared with theoretically derived values as done during the validation of the self-referencing electrochemical detection of oxygen (Land et al., 1999
). As described in more detail below, a self-referencing electrode made two
measurements at known distances apart, with its analog signal digitized
and processed by computer. The derived differential value was converted to a flux measurement. Because the electrode was constrained in the
time that it remained at each position, underestimates were theoretically possible because of limitations on response time. This
was a concern with the original Seris probes (Smith et al., 1999
), but
not with electrochemical devices having shorter response times down to
the range of tens or hundreds of milliseconds, such as probes of the
present design (Friedemann et al., 1996
; Porterfield et al., 2000
).
Therefore, no correction factor was required with the nitric oxide
sensor operating as a self-referencing probe at a step frequency of 0.3 Hz.
Experimental setup for NO measurement. The experimental
setup for measuring the flux of nitric oxide with a self-referencing microsensor was similar to that originally described for the
self-referencing ion-selective (Seris) electrodes (Smith, 1995
; Smith
et al., 1999
) and recently modified for electrochemical microsensors
(Land et al., 1999
). The rig was constructed around an Axiovert 10 inverted microscope (Zeiss, Oberkochen, Germany) fitted with a stage
plate on which the head-stage and translational motion control system were mounted. The latter consisted of Newport 310 series translation stages arranged in an orthogonal array and driven by size 23 linear stepper motors. This arrangement provided nanometer resolution of
movement for the electrode over micrometers in either the square-wave measurement translation or single-step positional mode (Smith et al.,
1999
). A computer with IonView software controlled movement. The entire
assembly was mounted on an antivibration table and housed within a
Faraday box. This box was thermally insulated and equipped with a
temperature control system. The motion controllers, temperature
controllers, head-stage, main amplifiers, and controlling software were
products of the BioCurrents Research Center (Marine Biological
Laboratory, Woods Hole, MA; www.mbl.edu/BioCurrents).
Direct measurement of NO flux. Direct measurement of NO flux
is based on the translational movement of the microsensor at a given
frequency through a gradient of NO. The movement of NO through the
extracellular medium by diffusion can be described by Fick's Law. In
this relationship the flux is expressed as pmol cm
2
sec
1 and given as
J =
D
C/
r, where
D is the diffusion coefficient for NO (2.6 · 10
5
cm
2
sec
1),
C is the concentration
difference between the two measurement positions (pmol
cm
3), and
r is the
excursion distance of the sensor (in this application, 30 µm). The
differential current measured by the electrode was converted into a
concentration, as discussed by Land et al. (1999)
for oxygen.
In situ measurement of NO. Before every experiment, the
electrode was calibrated against known concentration gradients of NO. A
standard 2 mM NO
solution for calibration was made by bubbling
NO
gas (Matheson Gas Products,
Secaucus, NJ) to saturation in saline purged of
O2 with Ar gas (Gevantman, 1995
). In each
experiment the slope of the linear calibration curves (Fig.
2B) and the difference in current
(I) measured experimentally at two measurement
positions 30 µm apart (Fig. 1B,C)
were used to calculate the mean flux of nitric oxide from the injury
site according to the flux relationship described above and the
procedure in Land et al. (1999)
. The differential current measured in
response to the 0.9 V polarization was directly proportional to the
concentration of NO.
During measurements, the probe was moved orthogonally to the cord in a
plane parallel to the surface of the recording dish, a standard 35 mm
tissue culture dish (Falcon, Oxnard, CA) partly filled with Sylgard 184 silicone rubber (Dow Corning, Midland, MI). The Sylgard-filled dishes
were partially cured overnight at room temperature, baked 2 hr at
60°C, and soaked in distilled water for at least 3 d before use.
Four midbody leech ganglia with their connectives intact were dissected
from the leech and pinned to the Sylgard in the culture dish with
0.10-mm-diameter minutien pins (Original Emil, Orly, Austria) in leech
saline, pH 7.4 (Kuffler and Potter, 1964
). In experiments to test the specificity of the response, the NOS inhibitor
L-NAME and, as a control, its inactive enantiomer
N
-nitro-D-arginine
methyl ester (D-NAME) were used. Preparations were dissected and pinned in 1 mM
L-NAME or 1 mM
D-NAME in leech saline.
A drop in NO flux reflects a shallower gradient, stemming from either a
lowered production at the source or an increased accumulation at the
sink, but in fact there was little opportunity for accumulation of NO
with time. Experiments were performed in a large bath and NO, a
reactive molecule, could not accumulate. Furthermore, a drop in
absolute current levels with time during the rapid transient decay was
consistent with a decreased production at the source.
Statistics. To compare flux between treatments, a one-way
ANOVA and Scheffe's test were performed. These same tests were used to
compare the peak fluxes for each experiment, the mean half-life of the
NO efflux for various treatments, and the kilocounts per minute
from each citrulline assay. Nonlinear regression analysis was performed
to determine the decay of the injury-induced NO efflux. Data were
analyzed, and curves were fit with SigmaPlot 5.0 (SPSS, Chicago, IL).
Statistical analysis of the R correlation coefficients was
performed using a Student's t test and one-way factorial
ANOVA in Statview 512.
 |
RESULTS |
Injury increased citrulline, reflecting injury-induced
NO production
The standard citrulline assay revealed NO production 30 min after
injury to the leech CNS by measuring the conversion of
[3H]arginine to
[3H]citrulline, which generated NO mole
for mole. In the experimental group, cords were mechanically injured
between ganglia and incubated 30 min in physiological saline before
being processed further. Controls were uncrushed cords. For each
experiment, citrulline counts from blank controls with no tissue
extract were subtracted from each treatment. As a negative control,
crushed cords were treated with 1 mM L-NAME.
After calculation of the mean based on five replicate experiments for
each treatment, the following counts were obtained: crush, 2.23 ± 0.58 × 105 cpm; uncrushed controls,
3.67 ± 2.73 × 104 cpm; and
positive controls (rat cerebellum extract), 9.24 ± 0.91 × 104 cpm. There was a significant
difference between the citrulline counts of crushed cords compared with
uncrushed cords, as determined by a one-way ANOVA and Scheffe's test
[F(2,12) = 6.436; p < 0.01] (Fig. 3). The citrulline counts
of the crushed cords were higher than the citrulline counts of the
positive control, which was a rat cerebellum extract having NOS
activity (Bredt and Snyder, 1990
). The increased citrulline counts in
crushed cords as compared with uncrushed cords support the hypothesis
that injury causes an increase in NOS activity and consequent NO
production.

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Figure 3.
Injury to the leech CNS causes an
increase in citrulline, reflecting NO production. In the experimental
group, cords were injured and incubated in Ringer's for 30 min before
being processed in the citrulline assay. Uncrushed controls were
exposed and incubated for 30 min before being processed in the
citrulline assay. Citrulline counts from blank controls were subtracted
from each treatment. Statistical analysis of five experiments indicated
that there was a statistical difference, with 95% confidence,
according to Scheffe's test, between the citrulline counts of crushed
and uncrushed cords [DF(2,12) = 6.436, p < 0.01]. KCPM, 1000 cpm.
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Injury causes a rapid transient efflux of nitric oxide from the
nerve cord
To determine directly the NO fluxes caused by mechanical injury to
the nerve cord, the current of the electrode polarized to 0.9 V was
measured differentially between two points at the lesion. The
differential current was converted into a directional measurement of
flux using the Fick equation. The translational movement of the
microelectrode as a square wave helped assure that it was
self-referencing; calibration was determined using artificial gradients
of NO over a range of concentrations. Baseline currents were recorded
at nerve cords that then were focally crushed, and the resulting
increased currents were measured. From the change in NO concentration
over a given distance, a static measurement of nitric oxide flux was
calculated using the Fick equation within the gradient to measure the flux.
Crushing caused a rapid and transient efflux of NO, as illustrated in
Figure 4A, which shows
a representative example of the NO efflux (pmol
cm
2
sec
1) as a function of time after
crushing. This pattern of response after injury was consistently
observed for all experiments performed on fresh tissue. The mean peak
injury-induced NO efflux of these initial injury experiments was
calculated to be 803 ± 99 fmol cm
2
sec
1 (n = 8).
Integration of all the flux versus time graphs for these experiments,
performed in physiological saline, indicated that the injury caused
~200 pmol NO cm
2 to be produced within
30 min (Fig. 5).

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Figure 4.
Injury causes NO efflux generated by NOS at the
lesion. A, Representative response of the nerve cord to
injury in physiological saline at time indicated by
arrows. Differential current measured by the
self-referencing probe, converted to flux (vertical axis, see
Materials and Methods), jumped abruptly after injury. The mean peak
efflux was 803 ± 99 fmol cm 2
sec 1(n = 8). All data were
modeled to the equation y = Y0 ± ae bt. Modeled data are represented
by the solid line. B, Representative
response to injury (arrow) in saline containing 1 mM L-NAME. C, Same as
B, but in 1 mM D-NAME. Treatment
with 1 mM L-NAME reduced the injury response to
a mean peak efflux of 199 ± 20 fmol NO cm 2
sec 1 (n = 11), whereas treatment with the inert enantiomer
(D-NAME) resulted in a mean peak efflux of 1888 ± 773 fmol cm 2 sec 1
(n = 6). Results with L-NAME and
D-NAME controls illustrate that the injury-induced response
is caused specifically by the efflux of NO that is generated by
NOS.
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Figure 5.
Injury-induced NO is blocked by NOS inhibition.
Integration over time of the flux versus time graphs for each treatment
gives the amount of NO produced at the lesion expressed as fmol NO
cm 2 after crushing. Treatments were with
physiological saline alone (control), in 1 mM
L-NAME (a concentration that inhibits NOS isoforms), and in
D-NAME as another control. Comparisons between treatments
indicated that L-NAME significantly reduced (**) the NO
produced during control injury experiments in physiological saline
alone [one-way ANOVA, 95% confidence, Scheffe's test,
F(2,11) = 15.271; p < 0.001] or during treatment with 1 mM D-NAME
[one-way ANOVA, 95% confidence, Scheffe's test,
F(2,11) = 15.271; p < 0.001].
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The duration of this injury response was assessed by mathematically
modeling the data. Mathematical analysis indicated that the
injury-induced NO efflux could be well described by a single exponential decay model with a constant y term, given by the
equation f(t) = yo + ae
t/
, with
yo = 15.8 ± 4.5 fmol
cm
2 sec
1,
a = 787 ± 99 fmol
cm
2 sec
1,
and
= 117 ± 30 sec. Nonlinear regression analysis
indicated the mean correlation coefficient (R)
for the data from the control injury experiments (in physiological
saline) was 0.948 ± 0.015. Some of the large SEs for the
exponential decay constant (a) can be attributed to the
difference in time between injuring the cord and actually starting
measurement with the probe. These results indicate that after injury,
there is a large and transient initial NO efflux accompanied by a
lingering component.
NO efflux is significantly reduced in NOS
inhibitor L-NAME
Indirect evidence indicates that NO produced at the injury is
generated by NOS that is sensitive to the NOS inhibitor
L-NAME (Shafer et al., 1998
; Furmanski et al., 1999
). This
implies that incubation of the nerve cord in 1 mM
L-NAME should reduce the injury-induced current by
inhibiting NO production. To test this, nerve cords were dissected in 1 mM L-NAME, and measurements were made in that
solution. Treatment with 1 mM L-NAME reduced
the mean peak injury-induced efflux to 179 ± 3 fmol
cm
2 sec
1
(n = 11). Integration of the flux over time showed that
in the presence of L-NAME, the mean injury
response dropped to 4.27 ± 1.9 pmol NO
cm
2 (Fig. 5).
To verify that this reduction in response was not caused by a
nonspecific toxic effect of L-NAME, parallel control
experiments were performed with D-NAME, the inert
enantiomer of L-NAME. In D-NAME, the
injury-induced response was as large as that observed in initial,
control injury experiments (Fig. 4C). The mean peak NO
efflux in the presence of D-NAME was 2529 ± 585 fmol cm
2
sec
1 (n = 6). This
D-NAME injury response was significantly greater, with 95% confidence, than the mean of the peak injury response in the
presence of 1 mM L-NAME
(110 ± 21 fmol cm
2
sec
1)
[F(2,14) = 13.082; p < 0.001], but not significantly different from the mean peak response
observed in the control injury experiments (803 ± 99 fmol NO
cm
2 sec
1)
as determined by a one-way ANOVA and Scheffe's test,
[F(1,4) = 4.024; p > 0.05].
Integration of the NO flux in the D-NAME experiments gave
~250 pmol/mol NO cm
2
(n = 6) (Fig. 5). This NO production was significantly
higher than that in 1 mM
L-NAME, as determined by a one-way ANOVA and Scheffe's test [F(2,11) = 15.271;
p < 0.01]. There was also a significant difference
between results from the control experiments and the
L-NAME treatment, as determined by one-way ANOVA
and Scheffe's test [F(2,11) = 15.271; p < 0.001]. The data indicate that treatment with L-NAME attenuated the injury response by
preventing formation of NO. Treatment with L-NAME
also reduced the mean decay rate of the injury-induced NO efflux. In
the presence of L-NAME, the injury-induced flux
did not decay as rapidly as under the control injury experiments in
normal Ringer's and the control D-NAME
experiments. However, the L-NAME experiments did
not fit the single exponential decay model as well as the control
injury experiments and the D-NAME experiments.
The mean R value for the control injury experiments was
0.948 ± 0.02, the R value for the
D-NAME experiments was 0.98 ± 0.01, and the
R value for the L-NAME experiments was
0.472 ± 0.18.
In three of six experiments, the L-NAME completely
inhibited any NO production. For this reason, we calculated the mean
value for the control injury experiments as 117 ± 30 sec and
for the D-NAME experiments as 160 ± 60 sec, but we
did not calculate the mean
for the L-NAME experiments.
 |
DISCUSSION |
In this study, we have demonstrated with the use of a novel
self-referencing NO-selective microelectrode that after injury to the
leech CNS, there is rapid transient efflux of NO. Several techniques
are currently available for the detection of NO, perhaps the most
established being the citrulline assay (Bredt and Schmidt, 1996
). This
approach, although suitable for demonstrating the activity of NOS, has
limited spatial and temporal resolution. To localize the production of
NO with a spatial resolution of millimeters or micrometers, a
microsensor is required.
The discovery of entirely separate components of NO efflux, including a
hitherto unknown NO spike, is particularly novel. The smaller steady
component was already known and accounts for previously described
observations that persistent NO synthesis at the lesion stops microglia
there, but the probe revealed a large transient component that could
play a separate role, possibly activating microglia and thereby
enabling them to migrate to the lesion. Some of the same features that
have made the leech nervous system favorable for studies on synapse
regeneration and microglia involvement in repair, such as its plain
visibility and accessibility in situ, now provide new
insights into the timing of NO generation in a system in which NO
regulates cell movement involved in nerve repair.
Both the direct measurement using an NO-sensitive self-referencing
microelectrode and indirect NO assay demonstrated an increase in NO
production in the minutes after injury to the leech CNS, but the NO
probe provided better temporal and spatial resolution. Injury-induced
NO production began within minutes after injury, with a mean peak
efflux that was transient, decreasing exponentially within minutes, but
accompanied by a more slowly declining phase. Treatment of tissue with
1 mM L-NAME significantly reduced both the
duration and amplitude of the injury response, whereas control treatment with the inert enantiomer D-NAME had no effect,
indicating that NO was produced in response to the injury. Previous
results showed that injury to the leech CNS activates eNOS in the large ensheathing glial cells and microglia of the connective (Shafer et al., 1998
), consistent with the conclusion that these cells produce
NO at the lesion. The nonlinear regression analysis confirmed that the
injury response can be described by a large, rapidly decaying
component, and then a slower, lingering component. This expands
findings that injury-induced eNOS immunoreactivity occurs within
minutes after injury and remains active long after (Chen et al.,
2000
).
The mean peak flux in D-NAME was higher than in the saline
controls; however, this difference was not statistically significant. Because D-NAME is the inert enantiomer of
L-NAME, it is not surprising that the injury response of
the tissue in D-NAME was not significantly different from
that of the control injury response. Because the value of NO efflux was
in decline at the outset of measurements, there is uncertainty
concerning the true peak efflux, which likely accounts for any
apparent, insignificant difference from the controls. There were
technical difficulties in measuring the peak flux resulting from an
inevitable delay between crushing and detection with the NO-selective
microelectrode because the preparation had to be refocused under the
inverted microscope attached to the NO-selective microelectrode after
crushing (which was done with a separate dissecting microscope).
Therefore, it is likely that we did not measure the entire NO efflux
after injury and that the largest component of the NO spike remained
undetected. Modifications in the experimental setup might permit
measurement of a larger NO spike after injury than that detected in
this study.
The reason for the drop in NO efflux from the crushed nerve cord is not
understood, but it does not reflect a decline in substrate availability. A similar drop was observed both in saline and in Leibowitz-15 culture medium, in which L-arginine is
abundant at 3 mM and is used to help buffer the medium, so
it is not substrate limiting. In principle, NO efflux could drop
although NO production is sustained. This might happen if barriers to
NO efflux form or if NO scavengers (Zhao et al., 1999
) are activated,
although there is no indication that this occurs. One plausible
explanation for the rapid drop in NO efflux after injury is that the
downstream target of NO, soluble guanylate cyclase within the tissue,
rapidly and specifically traps NO (Zhao et al., 1999
).
The NO-mediated accumulation of microglia at the lesion may aid
regeneration of the injured CNS axons because leech microglia not only
phagocytize debris but also appear to deposit laminin along the pathway
followed by axons as they grow through the lesion (von Bernhardi and
Muller, 1995
). Other studies support our hypothesis that NO is a stop
signal for migrating microglia. In chick dorsal root ganglion explants,
NO halted neurite motility (Hess et al., 1993
) and collapsed growth
cones in retinal ganglion cell explants (Rentería and
Constantine-Paton, 1995
). Microglia themselves contain NOS (Shafer et
al., 1998
). Although the large signal recorded with the NO probe would
act only transiently on microglia, as those cells accumulate they might
maintain the lingering signal recorded at the lesion.
 |
FOOTNOTES |
Received May 12, 2000; revised Oct. 2, 2000; accepted Oct. 11, 2000.
This work was supported by National Institutes of Health Grants NS34927
and NS37025 to K.J.M. and C.L.S., National Center for Research
Resources Grant P41 RR01395 to P.J.S.S., and the Graduate
Assistance in Areas of National Need training grant to S.M.K. We thank
Dr. Don Ready for use of his laboratory to perform the citrulline
assays, Dr. Sandra Rossie for help and the use of her scintillation
counter, Kasia Hammar and family for their hospitality to S.M.K. during
her visit to the BioCurrents Research Center, Rick Sanger for help with
the NO selective probe, and Jane A. McLaughlin for help in coordinating
our collaboration. In addition, we are grateful to Drs. Ken Robinson,
Joe Vanable, and Mark Messerli for useful suggestions and to Dr. John
Burnger for his help in analyzing the data.
Correspondence should be addressed to Dr. Christie L. Sahley,
Department of Biology, B326 Lilly Hall, 1392 State Street, Purdue University, West Lafayette, IN 47907. E-mail:
csahley{at}bilbo.bio.purdue.edu.
 |
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