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J Neurophysiol 90: 843-850, 2003. First published April 23, 2003; doi:10.1152/jn.00225.2003
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Neuromedin U Depolarizes Rat Hypothalamic Paraventricular Nucleus Neurons In Vitro by Enhancing IH Channel Activity

De-Lai Qiu1,4, Chun-Ping Chu1, Tetsuro Shirasaka2, Takashi Nabekura1, Takato Kunitake1, Kazuo Kato1, Masamitsu Nakazato3, Takahiko Katoh4 and Hiroshi Kannan1

1 Department of Physiology, Miyazaki Medical College, 5200 Kihara, Kiyotake, Miyazaki 889-1692, Japan; 2 Department of Anesthesiology, Miyazaki Medical College, 5200 Kihara, Kiyotake, Miyazaki 889-1692, Japan; 3 Department of Internal Medicine, Miyazaki Medical College, 5200 Kihara, Kiyotake, Miyazaki 889-1692, Japan; 4 Department of Public Health, Miyazaki Medical College, 5200 Kihara, Kiyotake, Miyazaki 889-1692, Japan

Submitted 10 March 2003; accepted in final form 11 April 2003


    ABSTRACT
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 DISCLOSURES
 REFERENCES
 
The effect of neuromedin U (NMU) on rat paraventricular nucleus (PVN) neurons was examined using whole cell patch-clamp recordings. Under current-clamp, 31% of PVN parvocellular neurons (n = 243) were depolarized by 100 nM NMU, but magnocellular neurons were not affected. NMU (10 nM to 1 µM) resulted in increased basal firing rate and depolarization in a dose-dependent manner with an EC50 of 70 nM. NMU-induced depolarization was unaffected by co-perfusion with 0.5 µM TTX + 10 µM 6-cyano-7-nitroquinoxaline-2,3-dione (CNQX) + 10 µM bicuculline. Extracellular application of 70 µM ZD 7288 completely inhibited NMU-induced depolarization. Under voltage-clamp, 1 µM NMU produced negligible inward current but did increase the hyperpolarization-activated current (IH) at step potentials less than –80 mV. The effects of NMU on IH were voltage-dependent, and NMU shifted the IH conductance-voltage relationship (V1/2) by about 10.8 mV and enhanced IH kinetics without changing the slope constant (k). Extracellular application of 70 µM ZD 7288 or 3 mM Cs+ blocked IH and the effects of NMU in voltage-clamp. These results suggest that NMU selectively depolarizes the subpopulation of PVN parvocellular neurons via enhancement of the hyperpolarization-activated inward current.


    INTRODUCTION
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 DISCLOSURES
 REFERENCES
 
Neuromedin U (NMU) is a neuropeptide that is present in the gut and CNS (Ballesta et al. 1988Go; Minamino et al. 1985Go) and has potent effects on smooth muscle. The two receptors for NMU, NMU-R1 and NMU-R2, are G protein-coupled receptors (GPCRs) (Howard et al. 2000Go). NMU-R2 is expressed in the paraventricular nucleus (PVN) of the rat hypothalamus (Raddatz et al. 2000Go). NMU induces extracellular acidification, arachidonic acid metabolite release, and intracellular Ca2+ mobilization in cells expressing NMU-R1 or NMU-R2 (Howard et al. 2000Go; Shan et al. 2000Go). Recently, we found that intracerebroventricular (icv) administration of NMU can provoke an increase in mean arterial blood pressure (MABP), heart rate (HR), and plasma norepinephrine. This suggests that NMU regulates sympathetic nervous system activity and affects cardiovascular function (Chu et al. 2002Go).

Conductance of K+ and Na+ by IH channels is activated by membrane hyperpolarization, gated by cyclic nucleotides (cAMP, cGMP), and is blocked by extracellular Cs+ and ZD 7288, a selective blocker of IH (Ghamari-Langroudi and Bourque 2000Go; Harris and Constanti 1995Go; Ludwig et al. 1998Go; Moosmang et al. 2001Go; Santoro et al. 1998Go). IH mediates inward rectification of the membrane in response to voltage changes. It has also been functionally implicated in maintaining resting membrane potential (RMP), thereby providing an excitatory drive that contributes to phasic and tonic firing (Doan and Kunze 1999Go; Ghamari-Langroudi and Bourque 2000Go). Four different isoforms of the IH channel have been cloned, and two different isoforms (HCN1 and HCN3) are highly expressed in rat PVN (Monteggia et al. 2000Go).

Because IH channels and NMU receptors are both present in rat PVN, the goal of the present study was to determine the effect of NMU activation on IH channels and PVN neuron activity. We used a whole cell patch-clamp method to examine the effects of NMU on rat PVN neurons in vitro.


    METHODS
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 DISCLOSURES
 REFERENCES
 
Hypothalamic slice preparation

Hypothalamic slices were prepared from P12- to P14-day-old male Wistar rats, as previously described (Shirasaka et al. 2001Go). All experiments were approved by the Ethics Committee of the Miyazaki Medical College and were in accordance with international guidelines on the ethical use of animals in laboratory experiments. Briefly, the brain was quickly removed and placed into ice-cold artificial cerebrospinal fluid (ACSF) consisting of (in mM) 140 NaCl, 3 KCl, 1.3 MgSO4, 1.4 NaH2PO4, 11 D-glucose, 5 HEPES, 2.4 CaCl2, and 3.25 NaOH. The pH was 7.3; the osmolarity was 290–300 mOsm, and the fluid was bubbled with 100% O2. Coronal slices were 250 µm in thickness, including PVN, and were prepared using a vibrating brain slicer (DSK-2000; Dosaka, Kyoto, Japan). The slices were incubated for >=1 h in a chamber filled with equilibrated ACSF at room temperature (24–26°C) before recordings were started.

Electrophysiology

Patch pipettes were made with a puller (PB-7; Narishige, Tokyo) from thick-wall borosilicate glass (GD-1.5; Narishige). They were filled with a solution consisting of (in mM) 130 potassium gluconate, 10 HEPES, 10 KCl, 1 CaCl2, 5 EGTA, 1 MgCl2, 2 Na2ATP, and 0.5 Na3GTP. The pH was adjusted to 7.2 with KOH. Patch pipette resistances were 5–7 M{Omega} in the bath, with series resistances in the range of 10–20 M{Omega}, compensated by 80%. The liquid junction potential (10 mV) was corrected for according to the method described by Neher (1992Go). Membrane potentials and/or currents were monitored with an Axopatch 200B amplifier (Axon Instruments, Foster City, CA), acquired through a Digidata 1200 series A/D interface on a personal computer using Clampex 7.0 software (Axon Instruments). Selected traces were saved to the hard drive of a computer, and all data were saved to a 4.7-GB DVD-RAM.

The membrane potential and current were low-pass-filtered at 1–5 KHz. Whole cell recordings were made from microscopically identified cells. Once stable recording conditions were obtained, a PVN neuron was identified electrophysiologically as type I (magnocellular) or type II (parvocellular) according to previously established criteria by current-clamp in standard ACSF (Luther et al. 2000Go). Type I neurons displayed transient outward rectification, while Type II did not. In voltage-clamp, TTX was routinely included in external recording solutions to block voltage-gated Na+ channels.

Chemicals

Reagents included rat NMU-23 (Peptide Institute, Japan), ZD 7288 (Tocris Cookson, Ballwin, MO), CsCl (Sigma, St. Louis, MO), and TTX (Sigma). ZD 7288 was prepared as a 50 mM stock solution (in H2O) and stored at –20°C until use. The other drugs were dissolved in ACSF.

Data analysis

Data were analyzed using Clampfit 8.0 (Axon Instruments) and are expressed as mean ± SE. IH was determined by subtracting IIns from Iss at each hyperpolarizing voltage step using the equation

(1)
and IH conductance (GH) was estimated as the amplitude of IH measured at various potentials (V) divided by the driving force (VEH), where EH is the reversal potential of IH (Ghamari-Langroudi and Bourque 2000Go) as follows

(2)

Differences between mean values recorded under control and test conditions were evaluated using Student's t-test or one-way ANOVA with Tukey's post-hoc test. Differences were considered significant at P < 0.05.


    RESULTS
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 DISCLOSURES
 REFERENCES
 
Neuronal membrane properties

A total of 309 PVN neurons (66 type I, 243 type II) were sampled under whole cell current-clamp conditions. While none of the type I neurons showed a response to NMU, 76 of the type II neurons (31%) were sensitive to NMU. These neurons expressed a depolarizing response approximately 1 min after application of 100 nM NMU; specifically, they displayed time-dependent inward rectification during the hyperpolarizing pulses (Fig. 1, C and D) that was blocked by 70 µM ZD 7288 (Fig. 1B) or 3 mM Cs+ (not shown). These characteristics are consistent with IH conductance (Ludwig et al. 1998Go; Santoro et al. 1998Go). Further, the responsive neurons exhibited a lack of transient outward rectification in response to a series of depolarizing current pulses delivered at a hyperpolarized membrane potential (Fig. 1A) (Luther et al. 2000Go).



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FIG. 1. Electrophysiological properties of paraventricular nucleus (PVN) neuromedin U (NMU)-sensitive neurons. A: the neuron displayed time-dependent inward rectification and lacked transient outward rectification (black arrow) in response to a series of depolarizing current pulses delivered at a hyperpolarized membrane potential. B: the neuron displayed inward rectification which was blocked by 70 µM ZD 7288. Holding potential was –60 mV. C: the neuron responded to a series of hyperpolarizing current pulses, expressing inward rectification. D: current-voltage relationships were obtained at the peak voltage ({circ}) and at the steady-state voltage ({bullet}) during the hyperpolarizing pulses.

 

Effects of NMU on membrane potential

Applications of NMU in concentrations ranging from 10 nM to 1 µM NMU resulted in depolarization and increased firing rate in a concentration-dependent manner in MNU-sensitive PVN neurons when the holding potentials were –60 mV (Fig. 2); however, the characteristics of the action potentials were not changed (not shown). The depolarization response appeared approximately 40 s after NMU exposure and peaked at approximately 100 s, with a maximal depolarization range of 1.75 ± 0.47 to 7.18 ± 1.21 mV (Fig. 2C). The minimum NMU dose required to elicit an effect on membrane potential was 1 nM, and the maximum dose was approximately 1 µM. The EC50 was approximately 70 nM. This response was unaffected by the presence of 0.5 µM TTX + 10 µM 6-cyano-7-nitroquinoxaline-2,3-dione (CNQX) + 10 µM bicuculline (7.18 ± 1.21 mV in the presence of 1 µM NMU, 6.79 ± 1.13 mV in the presence of TTX, CNQX, and bicuculline following the application of 1 µM NMU; mean ± SE, P > 0.05, n = 5).



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FIG. 2. Effects of NMU on PVN NMU-sensitive neurons in current-clamp. A1, A2, and A3 are the responses to 10 nM, 100 nM, and 1 µM NMU, respectively (bar, Vh = –60 mV). B1, B2, and B3 are the instantaneous spike rates of the neurons in A1, A2, and A3, respectively. NMU elicited increases in firing-action potential in a dose-dependent manner. C: the mean time courses of NMU-induced depolarizations. Note that NMU induced dose-dependent depolarization. (+) P < 0.05 vs. ACSF, (*) P < 0.05 vs. 10 nM NMU, (#) P < 0.05 vs. 100 nM NMU. D: the concentration-response curve of NMU-induced depolarization. The EC50 value obtained from the curve was approximately 70 nM. The number of neurons tested for each concentration is indicated near the bars.

 

Effects of NMU on membrane current

Application of 1 µM NMU to NMU-sensitive neurons with voltage-clamp at –60 mV produced a negligible inward current (7.5 ± 2.1 pA, n = 16). However, when neurons were held at –60 mV and a series of 1-s hyperpolarizing voltage steps were held from –60 to –150 mV, NMU induced a significant increment in steady-state current (Iss) at step potentials less than –80 mV (Fig. 3, A and B, P < 0.05, n = 7) and instantaneous current (IIns) at step potentials less than –100 mV (Fig. 3, A and C, P < 0.05, n = 7). NMU-induced increases in IIns was not affected by Ba2+ (Fig. 4A), but was blocked by ZD 7288 (Fig. 5C) or Cs+ (not shown). Simultaneously, the net reversal potential of the NMU-sensitive component of the fast current (determined in the presence of 100 µM Ba2+) was compared with the reversal potential for IH (also determined in the presence of 100 µM Ba2+) (Cardenas et al. 1999Go). As illustrated in Fig. 4, A and B, the reversal potential was –34.0 ± 2.6 mV (n = 4) under control and NMU conditions. This was similar to the reversal potential of –33.5 ± 2.1 mV (n = 4) obtained with another group of NMU-sensitive neurons for the portion of IIns which was increased by changing the holding potential from –60 to –80 mV in the presence of Ba2+ (Fig. 4, C and D). Thus the increase in IIns produced by the shift in holding potential likely reflects an increase in tonically open IH channels (Mayer and Westbrook 1983Go).



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FIG. 3. Effects of NMU on PVN NMU-sensitive neuron in voltage-clamp. A: current traces elicited by a series of 1-s hyperpolarizing voltage steps (10-mV decrement, holding potential was –60 mV) in artificial cerebrospinal fluid (ACSF; control) and during the application of 1 µM NMU. B: plots of steady-state current (Iss) in the control ({circ}), during the application of NMU ({bullet}), and the subtraction of NMU from control ({diamond}) against the membrane potential ({circ} and {bullet} shown in A). C: plots of instantaneous current (IIns) in the control ({circ}), during the application of NMU ({bullet}), and the subtraction of NMU from control (x) against the membrane potential ({circ} and {bullet} shown in A). Note that NMU increased Iss and IIns. D: plots of the difference between Iss and IIns (IssIIns = IH) in the control ({triangleup}), during the application of NMU ({blacktriangleup}) against the membrane potential. Note that NMU increased IH at step potentials less than –80 mV. All data are mean ± SE; n = 7, *P < 0.05 vs. ACSF.

 


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FIG. 4. Determination of reversal potentials for the fast current increased by NMU or hyperpolarization in the presence of 100 µM Ba2+. A: current traces elicited by a series of 100-ms hyperpolarizing voltage steps (10-mV decrement, holding potential was –60 mV) in the presence of 100 µM Ba2+ (A1) and in the presence of 100 µM Ba2+ + 1 µM NMU (A2). B: plots of fast current amplitude vs. command voltage for the currents shown in A1 and A2: 100 µM Ba2+; 100 µM Ba2+ +1 µM NMU. Straight lines were fitted to the data points using best fit values for slope and intercept determined by linear regression. The theoretical reversal potential for NMU increased fast current, indicated by the intersection of 2 lines, was extrapolated to –36 mV. C: families of currents evoked in the same cell as depicted in A, using 750-ms hyperpolarizing commands ranging from –70 to –120 mV from a Vh of –60 mV (C1) and –80 mV (C2), in the presence of 100 µM Ba2+. D: plots of fast current amplitude vs. command voltage for the current shown in C1 and C2: 100 µM Ba2+, Vh = –60 mV; 100 µM Ba2+, Vh = –80 mV. Straight lines were fitted to the data points for Vh values as described for B. The theoretical reversal potential for the hyperpolarization increased fast current was –34 mV, as estimated from straight lines fitted to the data.

 


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FIG. 5. Blockade of the effects of NMU by ZD 7288. A: 1 µM NMU (bar) provoked a reversible membrane depolarization accompanied by an increase in firing rate, and the NMU-induced membrane depolarization was unaffected by preperfusion with 0.5 µM TTX. B: 0.5 µM TTX, 70 µM ZD 7288 blocked NMU-induced depolarization. C: current traces elicited by 1-s –120 mV hyperpolarizing voltage steps (Vh = –60 mV) under ACSF, NMU, ZD 7288, ZD 7288 + NMU, and recovery. ACSF, NMU, and recovery are shown in C1; ACSF, ZD 7288, and ZD 7288 + NMU are shown in C2. D: plots of IIns (white arrow shown in C) vs. the command voltage for control ({circ}), 1 µM NMU ({bullet}), 70 µM ZD 7288 ({triangleup}), and 70 µM ZD 7288 + 1 µM NMU ({blacktriangleup}). E: plots of Iss (black arrow shown in C) vs. the command voltage for control ({circ}), 1 µM NMU ({bullet}), 70 µM ZD 7288, and 70 µM ZD 7288 + 1 µM NMU ({blacktriangledown}). Note that 70 µM ZD 7288 abolished the effects of NMU. All data are mean ± SE, n = 6.

 

Blockade of the effects of NMU by ZD 7288 or Cs+

In current clamp, NMU-induced depolarization was not affected by TTX (Fig. 5A). However, application of ZD 7288 induced slight hyperpolarization in NMU-sensitive PVN neurons and abolished NMU-induced depolarization (Fig. 5B). NMU increased Iss and IIns according to hyperpolarizing pulses. To determine whether NMU-induced increase in ISS and IIins represented enhanced IH channels, ZD 7288 and Cs+ (not shown) were used as IH channel blockers (Harris and Constanti 1995Go; Maccaferri and McBain 1996Go; McCormick and Pape 1990Go; Pape 1996Go). ZD 7288 significantly blocked IIns and NMU-induced increments of IIns at step potentials less than –80 mV. The I-V relationships were linear in the presence of ZD 7288 (Fig. 5, C and D). Further, ZD 7288 blocked Iss and NMU-induced increments of Iss at step potentials less than –80 mV. The I-V relationships were also linear in the presence of ZD 7288 (Fig. 5, C and E). This finding indicates that NMU-sensitive neurons have IH channels, which produce hyperpolarization-activated ZD 7288-sensitive inward currents (IH) and are activated at RMP, thus producing ZD 7288 sensitive IIns.

Effects of NMU on IH

In this study, 1 µM NMU significantly enhanced IH activity at step potentials less than –80 mV, and the maximal effects were at step potentials of –100 to –120 mV (Fig. 3D). Furthermore, we estimated the effect of NMU on IH conductance (GH) (see METHODS), EH, was obtained in the NMU-sensitive neurons as shown in Fig. 6A: following a step to –120 mV (1-s duration), the membrane voltage was stepped in the range of –110 to –50 mV (1-s duration, 10-mV increments) (Maccaferri and McBain 1996Go). The plot of the instantaneous current at each test potential yielded the fully activated I-V relationship, which was linear (Fig. 6B). The extrapolated reversal potential (EH) was –33.1 ± 1.8 mV (Fig. 6B, n = 5), similar to that previously reported for EH in other nervous preparations (Maccaferri and McBain 1996Go; McCormick and Pape 1990Go; Pape 1996Go). The mean GH-V relations are shown in Fig. 6C. Note that NMU enhanced IH conductance at step potentials more negative than –80 mV (P < 0.05, n = 7). Furthermore, the modified Boltzmann equation was used as follows

(3)
where GH(V) is the fraction of maximal GH observed at V, k is the slope factor, and V1/2 is the half-maximal voltage. The mean values were as follows: V1/2 = –110.2 ± 2.3 mV, k = 13.1 ± 2.0 in control, and V1/2 = –99.5 ± 3.4 mV, k = 11.5 ± 1.9 during the application of NMU. These data reveal that NMU produced a significant shift in V1/2 to a more depolarized potential (Fig. 6C, insert; P < 0.05). The slope factor values were not altered by NMU (P > 0.05).



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FIG. 6. Effects of NMU on IH. A: the reversal potential of IH was determined by clamping the NMU-sensitive neuron to –120 mV for 1 s and depolarizing in 10 mV at 1-s increments to –50 mV. B: mean (n = 6) instantaneous currents of IH ({bullet} showed in A) were plotted with respect to membrane potential, and a linear regression was performed. The reversal potential of IH (EH) was about –33 mV. C: the current (IH) data shown in Fig. 3D were converted into conductance (GH) using the equation GH = IH/(V + 33) (V is the test voltage). The solid lines are the best fit through the data points using the Boltzmann equation (ACSF, {circ}; 1 µM NMU, {bullet}; n = 7). The mean values were as follows: V1/2 = –110.2 ± 2.3 mV, k = 13.1 ± 1.9 in the control and V1/2 = –99.5 ± 3.4 mV, k = 11.5 ± 1.8 during the application of NMU. The insert is bar-graph summarizing effect of 1 µM NMU on half-maximal voltage (V1/2); note that 1 µM NMU significantly reduced V1/2 and elicited a positive shift V1/2 by about 10.8 mV. All data are mean ± SE. *P < 0.05 vs. ACSF. D1: IH traces evoked by steps to various voltages in the ACSF and during the application of 1 µM NMU. Superimposed on each trace is a monoexponential fit of the data points (a solid line extending to the right). The time constant used in the fits ({tau}) is indicated beside each trace. D2: plots of the mean ± SE (n = 7) IH activation time constants against voltage steps. Note that NMU enhanced IH kinetics at step potentials less than –80 mV. *P < 0.05 vs. ACSF.

 

Effects of NMU on the kinetics of IH activation

The time course of activation of IH was obtained from an analysis of the rising phase of the NMU-induced IH current evoked by hyperpolarizing steps to various voltages. As shown in Fig. 6D1, the IH current traces were fit to a single exponential function of the form At = A{infty}(1 – et/{tau}), where At is the amplitude of IH at time t, A is the amplitude of IH at a steady state, and {tau} is the activation time constant (Ghamari-Langroudi and Bourque 2000Go). Figure 6D2 reveals the plots of the means ± SE (n = 7) against voltage steps. The {tau} of NMU-sensitive neurons decreased from 800 ms at –70 mV to 100 ms at –140 mV and exhibited fast kinetics. NMU enhanced IH channels kinetics exhibiting decrements of {tau} at step potentials more negative than approximately –80 mV (P < 0.05 vs. ACSF, n = 7).


    DISCUSSION
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 DISCLOSURES
 REFERENCES
 
This study demonstrated that NMU enhanced IH channels activity leading to excitatory responses in a subpopulation of PVN type II neurons.

Expression of IH in PVN NMU-sensitive neurons

In the present study, NMU-sensitive PVN neurons displayed a time-dependent strong inward rectification during hyperpolarizing pulses (Fig. 1, C and D) that was blocked by 70 µM ZD 7288 (Fig. 1B). Further, these neurons did not display transient outward rectification. These properties are consistent with IH conductance produced by IH channels (Ludwig et al. 1998Go; Luther et al. 2000Go; Santoro et al. 1998Go; Stern 2001Go; Tasker and Dudek 1991Go).

NMU excited PVN NMU-sensitive neurons by enhanced IH

NMU evoked small depolarization and increased neuronal excitability. Several previous studies have demonstrated that enhancement of IH results in increased neuronal excitability and responsiveness to excitatory input. This occurs via release of neurons from tonic hyperpolarizing synaptic input and via facilitation of action potential triggering by depolarizing input or counter-balancing after-hyperpolarizations following action potentials (Pape 1996Go; Pape and McCormick 1989Go; Yagi and Sumino 1998Go). The presence of IH in magnocellular neurosecretory cells of rat supraoptic nucleus provides an excitatory drive that contributes to phasic and tonic firing (Ghamari-Langroudi and Bourque 2000Go). IH plays a significant role in setting both the RMP and the baseline level of excitability of hippocampal GABAergic interneurons found in the stratum oriens of area CA1 (Lupica et al. 2001Go).

Several findings in the current study suggest that NMU excites PVN neurons via enhanced IH channel activity. First, the RMP of NMU-sensitive neurons was approximately –58 mV (Vh = –60 mV), and the EH was approximately –33 mV (Fig. 6B), suggesting that IH channels are partially active at RMP (Yagi and Sumino 1998Go). NMU enhanced the activity of IH channels at RMP, induced NMU-sensitive neurons depolarizing in current-clamp (Fig. 2), and evoked increments of IIns by hyperpolarizing steps (Fig. 3C). NMU-induced increment in IIns was almost completely blocked by ZD 7288 (Fig. 5C), but not by Ba2+ (Fig. 4, A and B). Thus this likely reflects an increase in tonically activated IH (Mayer and Westbrook 1983Go). Second, in voltage clamp, NMU resulted in an increase of IH current and enhanced channel kinetics at step potentials less than –80 mV. NMU also produced a significant shift in V1/2 to a more depolarized potential. Third, ZD 7288 completely blocked NMU-induced depolarization (Fig. 5B) and abolished the effects of NMU on the neurons in voltage clamp (Fig. 5, C, D, and E). Collectively, these data suggest that NMU enhanced IH, resulting in a shift in the membrane potential toward more depolarized levels and firing action potential.

In this study, NMU resulted in depolarization of membrane potential in a dose-dependent manner with an EC50 of 70 nM. However, NMU did not induce large depolarization, likely because IH maintains the membrane potential of neurons within the range necessary for the generation of tonic action potential firing (Ghamari-Langroudi and Bourque 2000Go; Williams et al. 2002Go). Recently, it was reported that icv administration of NMU induced c-fos expression in magnocellular cells (type I) and parvocellular cells (type II) (Ozaki et al. 2002Go). The expression of the c-fos gene in the PVN should reflect the neural activation either directly or indirectly after icv administration of NMU (Ozaki et al. 2002Go). NMU-R2 is expressed in the PVN of the hypothalamus, along the wall of the third ventricle in the hypothalamus (Howard et al. 2000Go). In this study, NMU-induced responses in membrane potential were unaffected by TTX + CNQX + bicuculline. This evidence suggests that NMU depolarizes PVN type II neurons via a direct postsynaptic action rather than by indirect modulation of neurotransmission. On the other hand, none of the type I neurons showed a response to NMU. According to our data, we suggest that the expression of the c-fos gene in the PVN magnocellular may be mainly via an unknown indirect pathway after icv administration of NMU.

Possible mechanism of NMU action

NMU-R2 is expressed in the PVN of the rat hypothalamus (Howard et al. 2000Go), and HCN1 and HCN3 mRNA expression is highly enriched in the PVN (Monteggia et al. 2000Go). It is possible that PVN NMU-sensitive PVN neurons contain IH (HCNs) channels and NMU-R2. A key property of neuronal HCN channels is their regulation by neurotransmitters and hormones that act via cAMP, cGMP, or intracellular Ca2+ (Pape 1996Go). The cAMP and cGMP affect HCN channels by directly interacting with the cyclic nucleotide-binding domain protein of the C-terminus (Ludwig et al. 1998Go). The increment of intracellular Ca2+ in thalamic relay cells can result in modifications of IH that are similar to those observed following increases in cAMP (Lüthi and McCormick 1998Go). NMU-R1 is coupled to phospholipase C stimulation via a Gq-type G protein, resulting in the release of the inositol phosphate (IP) second messenger and increased intracellular Ca2+ in COS-7 cells (Raddatz et al. 2000Go). NMU-R2 is also coupled to the Gq family of G proteins in cells, inducing a rapid increase in intracellular Ca2+ (Shan et al. 2000Go). In thalamic neurons, transient increases in intracellular Ca2+ appeared to cause a reversible augmentation of IH attributable to the rapid, Ca2+-dependent formation of cyclic nucleotides (Lüthi and McCormick 1998Go). The increment of intracellular Ca2+ activates soluble guanylate cyclase, leading to increased cGMP levels (Kuzmiski and Macvicar 2001Go).

Thus we propose that NMU binds to NMU-R2, resulting in increased intracellular calcium and cGMP. This leads to an increment in IH current and neuronal excitation. This response may contribute to activation of autonomic centers in the brain stem and spinal cord that regulate MABP, HR, and plasma norepinephrine.


    DISCLOSURES
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 DISCLOSURES
 REFERENCES
 
This work was supported in part by a Grant-in-Aid for Science Research (14370024) from the Ministry of Education, Science, Sports, and Culture, Japan, and the Japanese Center of Excellence Program (Section of Life Science). This study was also carried out as part of the "Ground Research Announcement for Space Utilization" promoted by the Japan Space Forum.


    FOOTNOTES
 
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.

Address for reprint requests: H. Kannan, Department of Physiology, Miyazaki Medical College, 5200 Kihara, Kiyotake-cho, Miyazaki-gun, Miyazaki 889-1692, Japan (E-mail: kannanh{at}post.miyazaki-med.ac.jp).


    REFERENCES
 TOP
 ABSTRACT
 INTRODUCTION
 METHODS
 RESULTS
 DISCUSSION
 DISCLOSURES
 REFERENCES
 
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