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The Journal of Neuroscience, December 15, 1999, 19(24):10647-10655
Similarities and Differences between the Responses of Rat Sensory
Neurons to Noxious Heat and Capsaicin
Istvan
Nagy1, 2 and
Humphrey P.
Rang1
1 Novartis Institute for Medical Sciences, London, WC1E
6BN, United Kingdom, and 2 Department of Anesthetics,
Imperial College of Science, Technology and Medicine, School of
Medicine, St. Mary's Hospital, London, W2 1NY, United Kingdom
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ABSTRACT |
We have compared the membrane response of rat primary sensory
neurons to capsaicin and noxious heat, using electrophysiological and
ion flux measurements. Our aim was to determine whether, as recently
proposed, the same molecular entity accounts for excitation by both
types of stimulus.
The properties of the ion channels activated by heat and capsaicin show
many similarities but also important differences. The calcium
permeability of heat-activated channels is lower than that of
capsaicin-activated channels. Distinct single channels respond to heat
or capsaicin, and only a few show dual sensitivity. At the whole-cell
level, individual cells invariably show dual sensitivity, but the
amplitudes of the responses show little correlation.
We conclude that distinct molecular entities, which are both likely to
be derived from the VR1 gene product, account for the membrane
responses to heat and capsaicin.
Key words:
sensory neurons; capsaicin; heat; VR1; whole-cell; single-channel
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INTRODUCTION |
Primary afferent neurons that
respond to noxious stimuli belong mainly to the class of C-polymodal
nociceptors. They are sensitive to various types of stimulus, including
chemicals such as capsaicin (collectively known as vanilloids),
temperatures in the noxious range (>45°C), and mechanical stimuli of
moderate to high intensity (Szolcsanyi et al., 1988 ; Campbell and
Meyer, 1996 ). Studies on the membrane responses of these neurons to
vanilloids (Bevan and Szolcsanyi, 1990 ; Bevan and Docherty, 1993 ; Oh et
al., 1996 ) have shown that these compounds act by opening a specific
class of nonselective cation channels. The discovery of specific
binding of a potent vanilloid agonist, resiniferatoxin, to the
membranes of dorsal root ganglion neurons (Szallasi and Blumberg,
1990 ), and of a competitive vanilloid antagonist, capsazepine (Bevan et
al., 1992 ), proved the existence of a specific receptor, which was
recently cloned and designated VR1 (Caterina et al., 1997 ). Membrane
responses to noxious heat had previously been recorded from sensory
neurons grown in culture (Cesare and McNaughton, 1996 ; Kirschstein et
al., 1997 ; Reichling and Levine, 1997 ), and work by Caterina et al.
(1997) and Tominaga et al. (1998) showed that when VR1 was expressed in
oocytes or in a mammalian cell line, these cells showed sensitivity to
noxious heat as well as to vanilloids, leading to the suggestion that
the same molecular entity the VR1 gene product functions as the
"receptor" for both vanilloids and noxious heat. VR1 was shown to
function as a membrane ion channel, gated by vanilloid agonists and by
noxious heat, and to be expressed mainly in small-diameter sensory
neurons (Tominaga et al., 1998 ; Michael and Priestley, 1999 ), leading
to the suggestion that VR1 functions as a physiological heat transducer
in sensory nerve terminals.
Consistent with this hypothesis, we reported recently that all of the
small- to medium-sized rat dorsal root ganglion (DRG) neurons that
respond to temperatures in the noxious range [average threshold
45.3°C, designated low-threshold (LT) cells] are also capsaicin-sensitive, although there is a second class of heat-sensitive neurons, larger in size, with a threshold of 51°C [high-threshold (HT) cells], which are insensitive to capsaicin, (Nagy and Rang, 1999 )
and presumably possess a heat-sensitive mechanism distinct from VR1.
This could correspond to VRL-1, a VR1 homolog that codes for a
high-threshold heat-activated channel that is insensitive to capsaicin
(Caterina et al., 1999 ).
The present study was designed to test the hypothesis that heat and
capsaicin activate the same membrane channels in low-threshold cells,
by comparing the membrane responses of rat sensory neurons to these
stimuli at the whole-cell and single-channel level. We conclude that
although there are close similarities, the channels activated by heat
and capsaicin are in fact different, possibly representing molecular
variants of the VR1 gene product.
Preliminary reports of some of this work have been published previously
(Nagy and Rang, 1997 , 1998 ).
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MATERIALS AND METHODS |
Cell preparation. Cultures of DRG neurons were
prepared according to Lindsay (1988) . Adult rats (150-200 gm) were
killed with CO2, and DRGs from all segments were
removed and collected in Ham's Nutrient Mixture F14 (Imperial
Laboratories) culture medium containing L-glutamine (2 mM; Life Technologies, Gaithersburg, MD),
penicillin/streptomycin (Life Technologies; 50 IU/ml penicillin and 50 µg/ml streptomycin), and 4% Ultroser G (Life Technologies). Ganglia
were then incubated in culture medium containing collagenase (Type IV,
0.16-0.32 IU/ml; Sigma, St. Louis, MO) for 3 hr at 37°C in a 3%
CO2 incubator. After several washes DRG neurons
were dissociated by trituration with a fire-polished Pasteur pipette.
Cells were spun through sterile 15% bovine serum albumin (Sigma) and
plated on glass coverslips coated with poly-DL-ornithine.
DRG neurons were cultured for 1-5 d in F14 medium containing 50 ng/ml
nerve growth factor (NGF) (Promega, Madison, WI) at 37°C in the
presence of 3% CO2.
Superior cervical ganglion (SCG) neurons were cultured according to
Leaney et al. (1997) . Sixteen-day-old rats were killed with
CO2 and decapitated. The ganglia were dissected,
cleaned of connective tissue, and incubated in Leibovitz L-15 culture medium (Sigma) containing collagenase (Sigma; 400 IU/ml) for 15 min,
then transferred to medium containing trypsin (Sigma; 1 mg/ml) for 30 min, incubations being carried out at 37°C in 6%
CO2 incubator. Ganglia were washed and triturated
with a fire-polished Pasteur pipette. Cells were plated on glass
coverslips coated with poly-DL-ornithine and laminin, and
cultured for 1-5 d in the presence of 6% CO2 at
37°C in L-15 medium containing NaHCO3 (24 mM), fetal calf serum (0.85%, Life Technologies), glucose
(38 mM), L-glutamine (2 mM, Life
Technologies), penicillin/streptomycin (100 IU penicillin and 100 µg/ml streptomycin, Life Technologies), and NGF (50 ng/ml, Sigma).
Electrophysiology. Coverslips were placed in a recording
chamber superfused by 37 ± 0.5°C bath solution (1 ml/min).
Recordings of whole-cell currents under voltage clamp were made by
standard techniques with an Axopatch 200A amplifier (Axon Instruments) and PCs running the pCLAMP6 and AxoScope software packages (Axon Instruments). For whole-cell recording, the capacitance transient and
the series resistance were compensated to >80% before each recording.
Single-channel recordings were made in either the cell-attached or
inside-out configuration (Hammill et al., 1981 ). Electrodes of ~5
M were pulled from borosilicate glass capillaries (Clark Electromedical Instruments) and fire-polished. For single-channel recordings, electrodes were coated with Sylgard (Dow Corning). Recordings were filtered at 2 kHz, digitized at 4 kHz for whole-cell or
16.6 kHz for single-channel recordings with a DigiData 1200 interface,
and stored on hard disk.
The standard bath solution contained (in mM): NaCl 130, KCl
10, MgCl2 1.26, CaCl2 1.26, glucose 10, HEPES 10 (pH 7.4, adjusted with NaOH). For whole
recordings, the pipette solution contained (in mM): NaCl
10, KCl 130, MgCl2 1.26, EGTA 1, HEPES 10, (pH
7.4, adjusted with KOH). For ionic-selectivity studies, NaCl in the pipette solution and KCl in the bath solution were omitted, and the KCl
in the pipette solution was replaced by 130 mM CsCl. In some experiments either Na+ was replaced
by equimolar N-methyl-D-glucamine
(NMDG) or the CaCl2 concentration was altered in
the bath solution. The holding membrane potential was 60 mV. Reversal
potentials of whole-cell currents were established by linear voltage
ramps (+40 to 100 mV in 0.5 sec) generated by the pClamp6 software.
The potential was held at +40 mV for 0.2 sec at the start of the ramp
to inactivate voltage-gated inward currents as far as possible. Cells
that showed inflections on the control current-voltage
(I-V) curve, indicative of such currents,
were not used for estimation of reversal potentials. The relative ion
permeabilities were calculated by using the Goldman-Hodgkin-Katz equations (Lewis, 1979 ; Hille, 1992 ). The experiments were performed on
the low-threshold, capsaicin-sensitive group of cells (Nagy and Rang,
1999 ), defined as those that produced an inward current of >100 pA in
response to 2 µM capsaicin. To test the effect
of inhibitors (ruthenium red and capsazepine) on the response of the
neurons to capsaicin and heat, brief stimuli (2 sec at 49°C, or 1 sec
perfusion with 2 µM capsaicin at 37°C) were
applied every 2 min. EGTA (5 µM ) was added to
the pipette solution to minimize increases in intracellular calcium
concentration and thereby reduce desensitization. The inhibitor was
added immediately after the first (control) response, and the second
(test) response was used to measure the degree of inhibition. With no
inhibitor added, the second response to capsaicin averaged 79.5 ± 11.5% (n = 6) of the first, whereas the second
response to heat averaged 82.1 ± 4.4% (n = 7) of
the first. The effects of inhibitors were corrected for these
desensitization factors.
Single-channel recordings were performed in cell-attached patch or
inside-out patch configuration established after giga-seal formation
(Hammill et al., 1981 ). To ensure that the cell was fully
depolarized, the bath solution contained (in mM):
K-aspartate 115, KCl 15, MgCl2 1.26, HEPES 10, glucose 10, EGTA 1 (pH 7.4, adjusted with KOH). The composition of the
pipette solution was (in mM): NaCl 130, KCl 10, MgCl2 1.26, CaCl2 1.26 HEPES 10 (pH 7.4, adjusted with NaOH). The junction potential was
compensated, and the pipette potential was set to + 60 mV. The voltage
dependence of the single-channel currents was established by applying
200 msec voltage steps to vary the pipette potential between + 100 and
40 mV. Analysis of single-channel records was performed by means of
SCAN and EKDIST software (Colquhoun and Sigworth, 1995 ), kindly
provided by Prof. D. Colquhoun (Department of Pharmacology, University
College London, UK). Because the mean open time of heat-activated
channels was brief (see Results), their amplitudes were often reduced
by the low-pass filter that was needed to diminish background noise. By
correcting for the characteristics of the filter, the SCAN program
gives improved estimates of the amplitude and duration of brief openings.
Heat stimuli were applied by perfusing bath solution at ~0.5 ml/min
through a plastic tube positioned <100 µm from the cell. The
solution was passed through a silver heat exchanger the temperature of
which was regulated by a feedback-controlled Peltier element. Heat
stimulation was applied either as a pulse produced by switching between
heat exchangers held at 37°C and 52°C, respectively, or by ramping
the temperature of the heat exchanger from 37° to 52°C over 10 sec
with a temperature controller/power supply (Marlow Instruments). The
temperature of the stimulating solution, which was monitored by means
of a fine thermocouple at the tip of the perfusion tube, increased from
37° to 52°C. With "pulse" stimulation, the new temperature was
reached within 2-3 sec. Drugs were applied to the cells through the
same perfusion system at 37°C, and antagonists were applied for 2 min
before the test stimulation.
The longest diameter of the neurons in some experiments was measured by
an eyepiece graticule.
45Ca uptake experiments. The
method described by Wood et al. (1988) was used to measure the increase
in 45Ca uptake evoked by capsaicin or
heat. In brief, DRG neuron cultures (~300 cells per sample) on glass
coverslips were washed for 10 min at 37°C in physiological buffer
containing no added Ca2+. They were then
transferred for 10 min to buffer containing
45Ca (~1 µCi/ml) that either contained
capsaicin at a given concentration or was maintained at raised
temperature (up to 52°C). The coverslips were then washed three times
(2 min washes) in buffer containing 2 mM
CaCl2 and placed in plastic counting vials to
which 5 ml scintillant was added for determination of the
45Ca activity by liquid scintillation
counting. The radioactivity in each sample was expressed relative to
the mean radioactivity of cells that had been exposed to
45Ca-containing buffer at 37°C. Most
experiments were run with quadruplicate samples.
The composition of the Ca-free physiological buffer was (in
mM): NaCl 135, KCl 5, glucose 10, HEPES 10, brought to pH
7.4 with NaOH.
Cell viability determination. To determine whether cells
were killed by raised temperatures, combined staining with two
fluorescent markers was used (Viability/cytotoxicity kit, Molecular
Probes, Eugene, OR). Intact cells trap calcein AM, producing green
fluorescence, whereas ethidium bromide enters only damaged cells,
producing orange fluorescence. Cell cultures were exposed to normal
physiological buffer (as above, plus CaCl2 2 mM, MgCl2 2 mM) at
various temperatures for 10 min, returned to room temperature for 30 min, then stained for 45 min with calcein AM (1 µM),
which gives green fluorescence in intact cells, and ethidium bromide (2 µM), which gives orange fluorescence in damaged cells.
The dyes were made up in physiological buffer. After they were washed
in physiological buffer, the cells were photographed with a
fluorescence microscope (Nikon).
Statistical analyses were performed by the Clinstat software package.
Data are expressed as mean ± SEM.
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RESULTS |
Whole-cell recordings
Capsaicin application was used to distinguish low-threshold
heat-sensitive DRG cells (Nagy and Rang, 1999 ). Capsaicin (2 µM for 1.5 sec at 37°C) evoked inward current in 109 of
355 neurons selected at random (31%). Other distinct populations were
(1) insensitive cells that responded to neither capsaicin nor heat (163 of 355, 46%) and (2) high-threshold heat-sensitive cells that were
insensitive to capsaicin (83 of 355, 23%). The results presented here
were obtained from cells of the low-threshold type. The average
amplitude of the inward current evoked by capsaicin, in cells clamped
at 60 mV, was 1.39 ± 0.11 nA (n = 109). The mean threshold of the heat-evoked current, measured from the
temperature at which the inward current appeared during a heat ramp,
was 45 ± 0.2°C (n = 109) (Fig.
1A,B),
and the maximum amplitude recorded at the end of the standard heat ramp
(52°C) was 2.22 ± 0.14 nA (n = 109).
Capsaicin-sensitive cells were among the small- and medium-sized
neurons, with an average diameter of 22.8 ± 0.5 µm (n = 109). DRG neurons classed as heat-insensitive
usually showed a small, linearly increasing inward current in response
to a temperature ramp, averaging 0.1 nA at the end of the ramp (Fig.
1A), which was very similar to the response seen in
all superior cervical ganglion neurons tested. This was taken to be a
nonspecific response to heating and was not analyzed further.

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Figure 1.
A, Whole-cell voltage-clamp
recordings obtained from cultured dorsal root ganglion and superior
cervical ganglion neurons reveal a subpopulation of DRG cells that
produce inward cationic currents when stimulated by heat in the noxious
range. Averaged current temperature plots of noxious heat-sensitive DRG
neurons (squares, n = 22), noxious
heat-insensitive DRG neurons (triangles,
n = 20), and SCG neurons (circles,
n = 17). Inset shows recording from
a noxious heat-sensitive DRG cell. Top and bottom
traces are temperature and current recordings, respectively.
Holding potential: 60 mV. B, Heat ramp from 37 52°C
(1.75°C/sec) evokes specific heat-activated inward current that
increases sharply above 45°C. C, Capsaicin superfusion
(2 µM, 2 sec) to the same neuron as B also
produces an inward current. D, Relationship between
maximum amplitudes of currents evoked by the standard heat ramp
stimulation (37 52°C, 1.75°C/sec) and subsequent capsaicin
application (2 µM, 2 sec). Correlation coefficient,
r2 = 0.53.
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Correlation of heat and capsaicin sensitivity
If heat and capsaicin act on the same membrane channels, a close
correlation between the amplitudes of the two responses in individual
cells would be predicted. Figure 1D shows data for 86 capsaicin-sensitive cells (defined as those giving a response >0.1 nA
when tested with 2 µM capsaicin) that were also
tested with a standard heat ramp. The correlation between the response amplitudes was weak, although statistically significant
(r2 = 0.53; p < 0.001).
Ionic selectivity of channels
For further characterization of the heat- and capsaicin-evoked
currents in LT neurons, voltage ramps from +40 to 100 mV were applied before and during the heat- and capsaicin-induced currents. Net
I-V curves of the responses were constructed by
subtracting the control current from that recorded during the response
(Fig. 2A). As reported
previously in heat- or capsaicin-sensitive DRG neurons (Cesare and
McNaughton, 1996 ; Oh et al., 1996 ) and in VR1-transfected human
embryonic kidney (HEK) 293 cells (Tominaga et al., 1998 ), the net
currents evoked by capsaicin and by heat show a similar degree of
outward rectification, with low slope conductances at potentials
negative to 40 mV, and they have similar reversal potentials (Fig.
2B,C). The
I-V curves and mean reversal potentials for
heat- and capsaicin-activated currents in various ionic solutions are
shown in Figure 2 and Table 1. In these
experiments, intracellular K+ was replaced
by Cs+ to eliminate the large outward
K+ current from the control
I-V curve, which makes the determination of the
net currents unreliable at positive membrane potentials.

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Figure 2.
Current-voltage relationship of heat- and
capsaicin-evoked currents established by voltage ramps (from +40 to
100 mV, 500 msec). The pipette solution contained
Cs+ in place of K+ to eliminate
voltage-activated K currents. A, Estimation of the net
heat-activated I-V curve by digital
subtraction of the control from the test curve. B,
Averaged net I-V curves of heat-evoked
currents recorded with different ionic composition of the bath
solution. C, Averaged net
I-V curves of capsaicin-evoked currents
recorded with different ionic composition of the bath solution. Error
bars show SEM for points at intervals along the curves. Reversal
potentials and number of experiments are given in Table 1.
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Table 1.
Reversal potentials (mV, mean ± SEM) of heat- and
capsaicin-activated currents in various bath solutions
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The reversal potentials of both currents were close to 0 mV when the
main extracellular and intracellular cations were
Na+ and Cs+,
respectively, implying that the permeability of the channel to
Na+ and Cs+
was similar (Table 1). In the absence of
Ca2+, replacement of extracellular
Na+ by NMDG reduced the amplitude of the
currents, and shifted the reversal potential to approximately 55 mV,
with no significant difference between heat- and capsaicin-activated
currents, implying that the permeability of the channel to NMDG is
similar for both, although much less than the
Na+ permeability, as shown by the
calculated permeability ratios given in Table 1, which agree well with
the values estimated by Cesare and McNaughton (1996) . When
Na+ was substituted by NMDG, addition of
1.3-10 mM Ca2+ shifted the
reversal potential to more positive values, implying a relatively high
permeability of the channels to Ca2+. In
these solutions, the reversal potential for the capsaicin-activated current was significantly more positive than that of the heat-activated current, showing that the relative Ca2+
permeability of the channels is larger in the former case. Exact estimates are difficult, but calculations based on either the simple
bi-ionic equation (Hille, 1992 , Eq. 1.13 and 13.11), which disregards
the contribution of NMDG, or the more complicated Lewis equation
(Lewis, 1979 , Eq. A6), which takes it into account, show that the
Ca2+ permeability associated with
capsaicin-activated currents is approximately double that of
heat-activated currents, a difference in the same direction as that
reported by Tominaga et al. (1998) for responses measured in
VR1-transfected HEK293 cells.
Pharmacological properties
The effect of two known capsaicin antagonists the competitive
antagonist capsazepine (Bevan et al., 1992 ) and the nonselective channel blocking compound ruthenium red (Dray et al., 1990 ; Maggi et
al., 1993 ) on heat-evoked and capsaicin-evoked currents in low-threshold neurons is shown in Figure
3.

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Figure 3.
Effect of ruthenium red and capsazepine on
capsaicin- and heat-evoked currents. In these experiments both
capsaicin-evoked and heat stimulation were brief (2 sec), and 5 mM EGTA was added to the pipette solution to reduce
desensitization of subsequent responses. A, Ruthenium
red (RR) produces reversible reduction of both
capsaicin- and heat-activated currents. B,
Dose-response curve of ruthenium red on responses (±SEM) to heat
( , n = 3-6) and capsaicin ( ,
n = 3-6) currents. IC50 of RR for both
currents is in the same range (1-2 µM), although at low
concentrations, RR significantly increased heat-induced current.
C, Capsazepine selectively inhibited the
capsaicin-evoked currents but had little effect on the heat-induced
current. D, Dose-response curve of capsazepine on
responses to heat ( , n = 4-6) and capsaicin
( , n = 4-6).
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Ruthenium red inhibited the capsaicin-evoked current with an
IC50 close to 1 µM but produced a
biphasic effect on the heat-evoked current, increasing it significantly
at concentrations below 1 µM and inhibiting it at higher
concentrations (Fig. 3C). Capsazepine (Fig.
3B,D) strongly inhibited
capsaicin-evoked responses (IC50 < 0.5 µM) but was much less active against
heat-evoked currents, producing only slight inhibition at 10 µM.
Calcium uptake
Capsaicin (at 37°C) evoked a graded increase in
45Ca uptake, as reported in previous
studies (Wood et al., 1988 ); the maximum effect was an average
sevenfold increase over control (Fig. 4). Heating to temperatures above 46°C also produced an increase, maximally threefold at 49°C, a level significantly lower than that
achieved by capsaicin.

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Figure 4.
45Ca accumulation, expressed as
relative activity
(cpmtest/cpmcontrol) ± SEM, by
cultured DRG neurons induced by capsaicin ( , n = 4-6) and heat ( , n = 3-5).
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Because of the relatively small response to heat in this assay, the
effect of inhibitors was not tested.
Cell viability assay
In electrophysiological studies, brief heating of the cells to
52°C appeared to produce no obvious irreversible effects. We tested
for nonspecific cell damage at higher temperatures and longer exposure
times, using a fluorescent labeling technique that detects damaged
cells by the leakiness of their membranes to hydrophilic dyes (see
Materials and Methods). When the cells were exposed to raised
temperatures for 10 min in normal physiological buffer and then kept at
room temperature for 30 min, all of the neurons appeared viable after a
49°C challenge but were killed at 60°C, graded degrees of damage
being evident at intermediate temperatures.
Single-channel recordings
Single-channel activity evoked by heat was observed in 19 of 97 cell-attached patches of DRG cells (Fig.
5A,B),
and in 25 of 161 excised inside-out patches (Fig.
5F). Channel activity was absent at 37°C, and
channel events stopped as soon as the temperature was restored to
37°C (Fig. 5A). None of the patches obtained from superior
cervical ganglion neurons (n = 37) showed heat-activated channel activity (Fig. 5C).
Capsaicin-activated channels were also recorded from 10 of 100 cell-attached patches (capsaicin included in the pipette solution, bath
temperature 37°C) and from 18 of 161 inside-out patches. In the
majority of the patches (~70%), both heat and capsaicin induced
multiple level of openings at 60 mV membrane potential.

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Figure 5.
Single-channel recording from membrane patches
expressing heat-sensitive ion channels in cell-attached patch and
inside-out patch configuration. Bath solution in these experiments
contained 130 mM K+, and the pipette
solution contained 130 mM Na+. The
pipette potential was set to +60 mV. A, Heat ramp from
37°C to 51°C evokes multiple channel activity in cell-attached
patch configuration (n = 19 of 97). The activity
starts at 44°C and stops when the temperature returns to 37°C.
B, Sweeps (100 msec) of a recording from a
heat-sensitive membrane patch (cell-attached configuration) showing
channel activity (upward deflections) at 51°C. C, SCG
neuron membrane patch in cell-attached configuration, showing no
heat-activated channel activity. D, Temperature
dependence of channel activity in a cell-attached membrane patch
stimulated by a slow heat ramp. The dotted line shows
shut level. E, Mean single-channel current ( ,
mean ± SEM of 8 cell-attached patches) as a function of
temperature, compared with the mean whole-cell current ( , mean of 23 cells). F, Heat-induced channel activity at 50°C in
the same membrane patch, recorded in cell-attached and inside-out
mode.
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Overall single-channel activity, expressed as the mean channel current,
is plotted against temperature in Figure 5E. This curve does
not differ significantly from the temperature-current curve obtained
in whole-cell recordings. The single-channel current-voltage relationship (Fig.
6A,B)
was similar to that for whole-cell currents recorded under similar
ionic conditions; both curves showed pronounced outward rectification
at membrane potentials negative to 40 mV, similar to that of
capsaicin-activated channels (Fig. 6C,D).
Detailed analysis of single-channel currents by the Scan software
package was performed for nine heat-activated (50°C) and 10 capsaicin-activated (1 µM at 37°C) membrane
patches in which no multiple openings were observed. Typical amplitude
and open and shut time distributions are shown in Figure
7. The results are summarized in Table
2. This analysis suggested the existence
of two distinct amplitude levels for both heat- and capsaicin-activated
channels (Fig. 7), the main level being significantly higher for heat
(3.4 pA) than for capsaicin (2.8 pA). The low-amplitude channels
accounted for an estimated average of 17 and 8% of the openings for
heat and capsaicin, respectively, but were not detected in all patches. The open time distributions were well fitted by a single component, the
average open time ( open) of heat-activated
channels being significantly shorter (0.41 msec) than that of
capsaicin-activated channels (0.69 msec). The shut time distributions,
as expected, were more complex and contained more than one component.
The distributions were similar for capsaicin and for heat. In both
cases, the most numerous events consisted of very brief closures of <1
msec but much longer closures also occurred. Quantitative analysis of
the shut time distribution patterns was not performed, because
interpretable data would require longer stretches of record and a
systematic study with varying temperatures and capsaicin
concentrations.

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Figure 6.
Single-channel current-voltage relationship of
heat- and capsaicin-gated ion channels studied by applying voltage
steps between 100 and +40 mV. Pipette solution contained 130 mM NaCl; bath solution contained 130 mM KCl.
A, Recordings of heat-induced single-channel events at
different membrane potentials in inside-out patch configuration.
B, The single-channel I-V
curve of heat-activated channels in inside-out patches ( ,
n = 3), compared with that for whole-cell currents
(open circles, n = 5) recorded with the same
internal and external solutions. Data for cell-attached patches (data
not shown) were superimposable. The curves show outward
rectification and reversal potentials close to 20 mV, different from
the values given in Table 1, where Cs+ was the main
internal cation. C, Channel activity in an inside-out
membrane patch evoked by perfusion of capsaicin (2 µM) to
the inside surface at different membrane potentials. D,
The I-V curve of capsaicin induced
single-channel current (n = 3) showing the same
shape and reversal potential as in B. In single-channel
recordings, the dotted line indicates shut state.
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Figure 7.
Comparison of the characteristics of
single-channel events produced by heat and capsaicin recorded from
inside-out patches at 60 mV. Single-channel events were fitted by
SCAN and analyzed by EKDIST software. SCAN estimates the amplitudes of
single-channel events after correcting for low-pass filtering, and
EKDIST plots the frequency distribution of the duration of individual
open and closed states. A, E,
Single-channel events induced by heat and capsaicin. B,
F, Amplitude histogram of channel events, fitted by the
maximum likelihood method. Curve fitting reveals a significant number
of low-amplitude events, in addition to the main level, for both heat-
and capsaicin-evoked activity. Both conductance levels are smaller for
capsaicin than for heat (Table 2). C, G,
Open time distribution of channel openings induced by heat
(C) and capsaicin (G). Both
distributions can be fitted by a single component. D,
H, Shut time distribution of channel activity produced
by heat and capsaicin. In most cases, as here, the fitted distribution
indicated the presence of several components, which could not be
reliably estimated from the available data. Ordinates of open and shut
time distributions are plotted on square root scale, and abscissae are
plotted on a logarithmic scale (Colquhoun and Sigworth, 1995 ).
|
|
Expressing the open-channel characteristics (amplitude and
open) for heat- and capsaicin-activated
channels as ratios gives the following values for inside-out patches:
amplitude (heat, 50°C)/amplitude (cap, 37°C) = 1.21;
open (heat,
50°C)/ open (cap, 37°C) = 0.59. To
test whether these differences in single-channel characteristics could
be attributed to the temperature difference rather than to the nature
of the activating stimulus, capsaicin-activated channels recorded at
37°C and 50°C were compared in inside-out patches that showed no
channel openings in response to heat alone (see below). Two such
experiments were analyzed successfully: the ratio amplitude (cap,
50°C)/amplitude (cap,37°C) was 1.57 and 1.39, and the ratio
open (cap,
50°C)/ open (cap, 37°C) was 0.81 and 0.53. The difference between capsaicin-activated channels recorded at 37°C
and 50°C is similar to the difference between heat- and
capsaicin-activated channels in different patches, suggesting that the
latter difference could reflect the effect of temperature on the
channel properties, without necessarily implying that different channels are activated by the two stimuli.
To investigate directly whether heat and capsaicin activate different
populations of channels, we performed experiments in which individual
inside-out patches were tested successively with both stimuli. These
experiments (Fig. 8) showed that of 161 patches, 18 (11%) were sensitive to capsaicin and 25 (15%) were
sensitive to heat, but only 7 (4%) responded to both stimuli. Control
experiments showed that repeated application of heat or capsaicin in
sensitive patches remained effective in opening channels, so the low
proportion of dually responding patches could not be explained by
desensitization. These data show that distinct channels respond to heat
and to capsaicin. The number of dually responding patches (7 of 161) significantly exceeded the number expected by chance occurrence of
heat- and capsaicin-sensitive channels in the same patch
( 2 test, 0.01 < p < 0.05), suggesting that some channels exhibit dual sensitivity, but
the majority clearly do not.

View larger version (34K):
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|
Figure 8.
Lack of co-segregation of heat- and
capsaicin-sensitivity at the single-channel level. A-C,
Records from three inside-out patches that were stimulated
consecutively by heat and capsaicin. Patch A responded
only to heat, patch B responded only to capsaicin, and
patch C responded to both stimuli. Membrane potential
was 60 mV. Dotted lines in recordings indicate shut
state. D, Pie chart showing percentage of heat- and
capsaicin-sensitive membrane patches in a sample of 161 patches.
|
|
The characteristics of heat- or capsaicin-evoked channels were similar
in patches that responded to only one stimulus and in patches that
responded to both (Table 2).
 |
DISCUSSION |
The purpose of these experiments was to compare the
characteristics of capsaicin- and noxious heat-evoked responses of
sensory neurons to throw light on the question of whether both stimuli activate the same ion channels, as suggested recently (Caterina et al.,
1997 ; Tominaga et al., 1998 ).
Whole-cell electrophysiology
Our results confirm earlier reports (Cesare and McNaughton, 1996 ;
Kirschstein et al., 1997 ; Reichling and Levine, 1997 ) that a subset of
DRG neurons responds to heat with an increased cation conductance,
leading to an inward current at normal resting membrane potential. The
characteristics of these currents agree well with those reported by
Cesare and McNaughton (1996) . There are two classes of heat-sensitive
DRG neurons: LT cells that also respond to capsaicin and HT cells that
are insensitive to capsaicin (Nagy and Rang, 1999 ). In this study, we
have focused on the LT population. The threshold temperature for LT
cells was ~45°C, corresponding to the threshold of cutaneous
nociceptors (Campbell and Meyer, 1996 ). The heat-activated currents in
the present study had amplitudes similar to those described by
Vycklicky et al. (1999) but ~10 times greater than those reported
earlier (Cesare and McNaughton, 1996 ; Kirschstein et al., 1997 ;
Reichling and Levine, 1997 ). The reason for this discrepancy is not
clear but could be related to differences in experimental technique.
Cesare and McNaughton (1996) studied neurons from newborn rats;
Kirschstein et al. (1997) used very brief and relatively
imprecise heat pulses, whereas Reichling and Levine (1997) recorded
responses even at temperatures as low as 30°C, well below the
nociceptive threshold.
The reversal potential of the heat-activated current, and its ion
selectivity, also agree in general with the results reported by Cesare
and McNaughton (1996) . Published estimates of the cation permeability of the heat-activated and capsaicin-activated channels of
DRG neurons and VR1-transfected HEK cells are summarized in Table
3. All give similar values of relative
Cs+ and Na+
permeability of heat- and capsaicin-activated channels, but the values
obtained for Ca2+ permeability vary
widely. Our results suggest that
PCa/PNa is approximately
twofold greater for capsaicin- than for heat-activated channels in DRG
neurons, in agreement with results of Caterina et al. (1997) and
Tominaga et al. (1998) on VR1-transfected HEK cells. Because heat- and
capsaicin-evoked responses were necessarily recorded at different
temperatures, we cannot exclude the possibility that this could account
for the difference in Ca2+ permeability.
Alternatively, the nature of the stimulus chemical or physical could
influence in a subtle way the characteristics of the open channel.
View this table:
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|
Table 3.
Relative permeabilities (PNa = 1) to Ca2+ and Cs2+ of heat- and
capsaicin-activated channels in sensory neurons and in
VR1-transfected HEK cells
|
|
We found that capsazepine, a competitive antagonist of capsaicin,
strongly antagonized the effect of capsaicin, with an
IC50 close to 0.1 µM, but had no
effect on heat-evoked currents at concentrations up to 10 µM. This finding agrees with the observation on DRG
neurons (Reichling and Levine, 1997 ), but differs from that of Tominaga
et al. (1998) who found that 10 µM capsazepine significantly reduced the heat-induced current in a VR1-expressing cell
line. Ruthenium red blocked both responses at similar concentrations, but unexpectedly enhanced the heat response at 0.5 µM, an
effect never seen on the capsaicin-induced response. In VR1-expressing non-neuronal cells, ruthenium red reduced both capsaicin- and heat-induced currents (Caterina et al., 1997 ; Tominaga et al., 1998 );
however, it did not affect the heat-evoked current in DRG neurons
(Reichling and Levine, 1997 ), but the low-temperature threshold and the
Ca2+ dependence of the current studied by
Reichling and Levine (1997) suggest that those responses are different
from those that we have investigated.
Calcium uptake measurements
The temperature-dependent increase in
45Ca accumulation by DRG neurons resembles
the action of capsaicin and shows a threshold at ~46°C. The maximal
45Ca entry evoked by heat was only
approximately one-third of that induced by capsaicin (Fig. 4), and it
did not increase with temperature beyond 49°C. The smaller maximal
response to heat might have been caused by an adverse effect of high
temperature on the ability of intracellular storage mechanisms to
sequester calcium. However, the capsaicin-evoked
45Ca entry was not affected when the
temperature was raised to 49°C. We therefore conclude that the
difference in the heat- and capsaicin-evoked maximal
45Ca influx could be caused by the
relatively lower Ca2+ permeability of the channel during heat activation.
The results of the cell viability tests suggest that DRG neurons retain
their integrity well when exposed for 10 min to temperatures up to
52°C, so it is unlikely that nonspecific damage is a major factor in
these experiments.
Single-channel recordings
Heat stimulation evoked single-channel activity in one-fifth of
the patches taken from DRG cells. The characteristics of this single-channel activity correspond closely with those of the
heat-activated currents recorded in the whole-cell configuration. The
temperature activation curve is the same shape, with a threshold of
45°C and steep rise at temperatures above this. The
I-V relationship and reversal potential of the
single-channel currents also correspond with those of the whole-cell
currents, suggesting that the activity of these channels underlies the
heat-activated whole-cell current. Channel activity could be recorded
from both excised- and cell-attached patches, showing that heat
sensitivity is an integral property of the channels and is not
secondary to heat-evoked modulation of intracellular signals. This
conclusion agrees with the findings of Caterina et al. (1997 , 1999 ) on
the heat sensitivity of VR1-transfected cells, but not with the
suggestion of Reichling et al. (1997) that heat-activated currents in
DRG neurons are secondary to a rise in intracellular calcium concentration.
As with the whole-cell responses, there are strong similarities between
the characteristics of heat- and capsaicin-evoked single-channel
currents, and our findings on the latter agree well with those of Oh et
al. (1996) . The I-V curves and reversal potentials for capsaicin and heat agreed closely, although there were
significant differences in the mean amplitude and mean open time.
Compared with capsaicin-activated channels, heat-activated channels
gave currents of larger amplitude and shorter duration. Such
differences have not been reported on a VR1-expressing cell line
(Tominaga et al., 1998 ). Studies on the effect of temperature on other
types of ion channel [for references, see Chung and Kuyucak (1995) ]
show that channel conductance often shows Q10
values of 1.3-1.5, so the difference in amplitude between
capsaicin-activated and heat-activated single-channel events could be
explained on this basis. The difference in mean open time could be
explained similarly. Where we succeeded in measuring the effect of
temperature on the characteristics of capsaicin-activated channels, the
results were consistent with this interpretation
The amplitude histograms for both heat- and capsaicin-activated
channels show the presence of a small proportion of low-conductance channels, which has not previously been reported. It is difficult to be
certain whether these represent distinct channels or a subconductance state of a single type of channel. If there were two distinct types of
channel, occasional dual (high plus low) openings would be expected.
These were not detected, but typically the total open probability was
~0.2 (corresponding to ~0.17 for the large channels and 0.03 for
the small channels); the probability of both being open simultaneously
would therefore be only ~0.005, and such events could easily have
been missed. Occasional low-high and high-low transitions were
detected, as expected if the two levels represent distinct conductance
states of the same channels, but a more rigorous analysis would be
needed to establish this point. The open-time histograms showed only a
single component. Separating the channels into low and high conductance
events gave similar mean open times for each, so we were not able to
distinguish between them on this basis.
Our most unexpected finding was that most patches responded to either
heat or capsaicin, but rarely to both. It was important to be sure that
the separation of heat and capsaicin sensitivity was not an artifact
attributable to desensitization. Control experiments showed that
repetition of either stimulus, although resulting in progressive
reduction of the response, never caused complete desensitization.
Furthermore, it was frequently found that patches that failed to
respond to the first test would respond to the second, after switching
from heat to capsaicin, or vice versa. We therefore conclude that
distinct channels respond to heat and capsaicin, respectively. The
number of dual-sensitive patches somewhat exceeded the number expected
by chance. This could reflect the presence of some individual channels
that respond to both stimuli or a tendency for channels of both types
to aggregate in the same patch of membrane.
The work of Caterina et al. (1997) and Tominaga et al. (1998) shows
that transfection of HEK293 cells with the VR1 gene results in the
appearance of both heat- and capsaicin-sensitive channels, but it
remains to be established whether an individual channel responds to
both stimuli. The most economical explanation to reconcile our findings
would be that the VR1 gene product may assume different functional
states depending on other factors, including splice variants,
aggregation with other membrane proteins, the presence of different
multimeric species, or the degree of phosphorylation or glycosylation
of the channel protein.
The similarities and differences between heat- and capsaicin-evoked
responses presented in this paper are summarized in Table 4.
 |
FOOTNOTES |
Received June 21, 1999; revised Sept. 20, 1999; accepted Sept. 30, 1999.
Correspondence should be addressed to Istvan Nagy, Department of
Anesthetics, Imperial College of Science, Technology and Medicine,
School of Medicine, St. Mary's Hospital, London, W2 1NY, UK. E-mail:
i.nagy{at}ic.ac.uk.
 |
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S. Schwarz, W. Greffrath, D. Busselberg, and R.-D. Treede
Inactivation and tachyphylaxis of heat-evoked inward currents in nociceptive primary sensory neurones of rats
J. Physiol.,
November 1, 2000;
528(3):
539 - 549.
[Abstract]
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M. J Gunthorpe, M. H Harries, R. K Prinjha, J. B Davis, and A. Randall
Voltage- and time-dependent properties of the recombinant rat vanilloid receptor (rVR1)
J. Physiol.,
June 15, 2000;
525(3):
747 - 759.
[Abstract]
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M. J. Caterina, A. Leffler, A. B. Malmberg, W. J. Martin, J. Trafton, K. R. Petersen-Zeitz, M. Koltzenburg, A. I. Basbaum, and D. Julius
Impaired Nociception and Pain Sensation in Mice Lacking the Capsaicin Receptor
Science,
April 14, 2000;
288(5464):
306 - 313.
[Abstract]
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C. Garcia-Martinez, C. Morenilla-Palao, R. Planells-Cases, J. M. Merino, and A. Ferrer-Montiel
Identification of an Aspartic Residue in the P-loop of the Vanilloid Receptor That Modulates Pore Properties
J. Biol. Chem.,
October 13, 2000;
275(42):
32552 - 32558.
[Abstract]
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J. M. Welch, S. A. Simon, and P. H. Reinhart
The activation mechanism of rat vanilloid receptor 1 by capsaicin involves the pore domain and differs from the activation by either acid or heat
PNAS,
December 5, 2000;
97(25):
13889 - 13894.
[Abstract]
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