Departamento de Biología Vegetal, Facultad de Ciencias,
Universidad de Málaga, Campus de Teatinos s/n, 29071 Málaga, Spain
 |
INTRODUCTION |
Zostera marina L. is an aquatic angiosperm that grows
in a medium with a high salinity
seawater itself
with NaCl
concentrations in the region of 0.5 M. Leaf cells
of this plant exhibit a plasma membrane potential
(Em) of around
160 mV in natural
seawater (Fernández et al., 1999
). Molecular and physiological
evidence indicates that the Em in this
halophyte is maintained by the activity of a
H+-pump (Fukuhara et al., 1996
; Fernández
et al., 1999
). With this highly negative
Em, the uptake of essential anions
such as NO3
, which
usually occurs in seawater at concentrations of 1 to 500 µM (Riley and Chester, 1971
) and is probably
below 10 µM in the close environment of the
plant (Hernández et al., 1993
), must be energized.
Most studies on vascular plants and algae have reported that
NO3
transport is powered
by the electrochemical potential for protons present across the plasma
membrane of plant cells (Ullrich, 1992
). Evidence includes simultaneous
measurements of NO3
and
H+ fluxes (Mistrik and Ullrich, 1996
),
NO3
-evoked membrane
depolarizations (McClure et al., 1990
; Ullrich and Novacky, 1990
; Glass
et al., 1992
), and pH dependence of
NO3
-elicited inward
currents both in intact plants (Meharg and Blatt, 1995
) and in oocytes
expressing plant NO3
transporters (Tsay et al., 1993
; Zhou et al., 1998
; Liu et al., 1999
).
Four different NO3
uptake
systems have been identified in higher plants: both low- and
high-affinity systems are present and can be constitutive or inducible
(Wang and Crawford, 1996
; Liu et al., 1999
). High-affinity systems show
saturation kinetics and operate at concentrations lower than 0.5 mM with Km values in the
range of 7 to 100 µM; low-affinity systems show
linear kinetics and function at concentrations above 0.5 mM (Wang and Crawford, 1996
; Crawford and Glass,
1998
).
Energization of solute transport by H+ coupling
is prevalent among bacteria, fungi, and plants. Nevertheless, for the
plasma membrane of most cells the presence of an inwardly directed
electrochemical potential difference for Na+ can
potentially be exploited for energization of solute transport through
Na+ coupling. Accordingly, a number of
Na+-dependent transport systems have been
identified. Na+-dependent uptake of Glc and amino
acids has been shown in the marine diatom Cyclotella
(Hellebust, 1978
), and phosphate transport has been reported to be
stimulated by Na+ in several green algae (Raven,
1984
). In the case of
NO3
,
Na+-dependent uptake has been described only in
the marine diatom Phaeodactylum tricornutum (Rees et al.,
1980
) and in cyanobacteria (Lara et al., 1993
).
During the past decade an emerging number of
Na+-coupled transport systems have also been
discovered at the plasma membranes of multicellular plants. In
freshwater charophyte algae, the influx of K+,
urea, and Lys has been shown to be Na+ dependent
and/or directly coupled to the transport of Na+
(Smith and Walker, 1989
; Walker and Sanders, 1991
), and
Na+-dependent K+ uptake has
also been demonstrated in some aquatic angiosperms such as
Egeria, Elodea, and Vallisneria
(Walker, 1994
; Maathuis et al., 1996
). A
Na+,K+ symporter, HKT1, has
been cloned from wheat (Rubio et al., 1995
), but it remains
unclear whether Na+ coupling comprises the
dominant mode of energizing K+ uptake in
terrestrial angiosperms (Maathuis et al., 1996
).
The elevated Na+ concentration present in
seawater and the highly negative Em in
Z. marina makes feasible the existence of this type of
alternative transport system powered by the putative electrochemical
potential for Na+. To test this hypothesis, we
have investigated NO3
transport at the plasma membrane of leaf cells of Z. marina
to determine the possible interactions between
Na+ and
NO3
. These interactions
have been studied with respect to the electrophysiological properties
of the plasma membrane and to
NO3
depletion in media
surrounding whole leaves.
 |
MATERIALS AND METHODS |
Plant Material
Zostera marina L. plants were collected off the coast
of Málaga (Spain) at a 5-m depth. Plants were maintained in the
laboratory in natural seawater at 15°C and a light intensity of 150 µmol m
2 s
1, with a
photoperiod of 16 h of light and 8 h of darkness.
Plants were N-starved prior to experiments for at least 3 d in
N-free artificial seawater (ASW) adjusted to pH 8.0 with NaOH. The
composition of ASW was 0.010 mM
KH2PO4, 1.2 mM
NaHCO3, 5 mM K2SO4, 12 mM
CaCl2, 15 mM
MgSO4, 42.5 mM
MgCl2, and 500 mM NaCl.
Membrane Potential Measurements
Leaf pieces were excised to remove partially the epidermis, and
were mounted in a plexiglass chamber (volume 1.1 mL). Continuous perfusion of the assay medium was maintained at a flux of approximately 10 mL/min. Both epidermal and mesophyll cells were impaled with single-barrel electrodes. Membrane potentials were measured using the
standard glass microelectrode technique as described by Felle (1981)
.
Micropipettes were backfilled with 0.5 M KCl.
Microelectrodes were fixed to electrode holders containing an Ag/AgCl
pellet, and connected to a high-impedance differential amplifier
(FD-223, World Precision Instruments, Sarasota, FL). Tip
potentials never exceeded
10 mV.
Experiments were carried out in N-free ASW (as above) buffered
with 10 mM
4-(2-hydroxyethyl)-1-piperazineethanesulfonic acid (HEPES)-Tris(hydroxymethyl)-amino-methane (Tris) to pH 8.0. NO3
was added as
KNO3. To check the effect of pH, the same buffer was adjusted to pH 6.0 or 7.0. To test the effect of
Na+, N-free ASW with a slightly different
composition was used (NaCl-ASW: 2.5 mM
KHCO3, 2.5 mM
K2SO4, 5 mM
CaSO4, 5 mM
MgSO4, 500 mM NaCl, and 10 mM HEPES-Tris). In Na+-free ASW, NaCl
was substituted by 0.8 M sorbitol (sorbitol-ASW). Na+ was added to the medium at increasing
concentrations as Na2SO4 or NaCl.
NO3
Depletion Experiments
Whole plants were maintained for 3 d in N-free ASW and
were preincubated in the assay medium for 1 h before starting the
experiment. The composition of assay medium was the same as for
impalements. Whole leaves (0.6-0.9 g fresh weight) were incubated in
100-mL flasks. Three replicates were assayed for each treatment
(NaCl-ASW, sorbitol-ASW, sorbitol-ASW + 5 mM
Na2SO4, and sorbitol-ASW + 10 mM NaCl). The assay was carried out with slow and
constant agitation at 25°C and at a light intensity of 50 µmol
m
2 s
1. The first
treatment (NaCl-ASW) was also assayed in darkness. KNO3 was added at an initial concentration of 100 µM. Samples were taken at 0, 1, 2, 4, 8, 12, and 24 h. NO3
was analyzed
colorimetrically as described in García-Sánchez et al.
(1993)
.
Chemicals
pH buffers and sorbitol were from Sigma-Aldrich (St. Louis).
Monensin (Sigma) was dissolved in ethanol at a concentration of 50 mM.
Data Analysis
Data are given as means ± SE. Membrane
depolarization data were fitted with the Michaelis-Menten equation
using a non-linear regression computer program (KaleidaGraph, Synergy
Software, Reading, PA).
 |
RESULTS |
Effect of NO3
Additions on the Membrane
Potential
Figure 1A demonstrates that
NO3
evoked a rapid
membrane depolarization in N-starved plants in the light. Measurable
changes in Em were evident even at 1 µM
NO3
(not shown). When
NO3
was washed from the
medium, the membrane first hyperpolarized so that
Em was transiently more negative than
the original resting potential, and then depolarized with another
overshoot to a value close to that before
NO3
addition (Fig. 1A).
Depolarizations showed saturation at concentrations around 50 µM
NO3
(Fig.
2). Because depolarization is an integral
function of the net charge carried by the
NO3
transport system, the
concentration dependence of the depolarization can be taken as a rough
guide to the affinity of this system for its substrate. Fitting the
data with the Michaelis-Menten equation yielded a
Km value of 2.31 ± 0.78 µM
NO3
and a maximum
depolarization of 15.6 ± 0.9 mV (Fig. 2).

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Figure 1.
Effect of the addition of
NO3 on Em. A,
Tissue in the light, incubated in ASW, showing the response of a single
mesophyll leaf cell to the addition of 5 and 100 µM
KNO3. B, Tissue in the dark with KNO3 added at
the concentrations indicated. Small downward arrowheads indicate the
onset of the NO3 wash.
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Figure 2.
Membrane depolarizations induced by increasing the
NO3 concentration. Mesophyll leaf cells were
impaled in ASW in the light ( ) or in the dark ( ). Data are the
means ± SE of three independent replicates. Values in
the light were fitted with the Michaelis-Menten relationship, as shown
by the curve.
|
|
NO3
-induced
depolarizations were lower in the dark than in the light, with maximum
values around 10 mV, and they did not exhibit saturation kinetics
(Figs. 1B and 2). The response of Em
to NO3
additions was also
different (Fig. 1B): the depolarization was very rapid and when
NO3
was washed from the
medium the Em did not exhibit the
overshoot in the depolarizing direction before returning to the resting value.
The depolarizations elicited by
NO3
suggest that uptake
of this anion involves flow of positive charge into the cell.
Effect of pH on NO3
-Induced
Depolarizations
Many H+-coupled transport systems in plants
are activated by a rise in external H+
concentration (Bush, 1993
), and this enhancement of electrophoretic transport can be reflected in a larger transport-related depolarization as the pH is lowered. We therefore examined the pH dependence of the
NO3
-induced
depolarization. In contrast to many H+-coupled
transport systems, the depolarizations induced by saturating NO3
concentrations (100 µM) were lower at acidic than at alkaline pH (Fig.
3). A shift of external pH from 8.0 to
6.0 decreased the magnitude of the depolarization by a factor of about
3.

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Figure 3.
Effect of pH on
NO3 -induced depolarizations. Mesophyll leaf
cells were impaled in ASW buffered at different pHs and challenged with
saturating NO3 concentrations (100 µM KNO3). Values are the means ± SE of five independent replicates.
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Effect of Na+ on NO3
-Evoked
Depolarizations
To determine whether Na+ was involved as the
coupling ion, we examined the capacity of
NO3
to depolarize the
membrane in the absence of Na+. Replacement of
NaCl in the medium with isosmotic sorbitol produced a slight
hyperpolarization of the membrane (data not shown). In Na+-free conditions,
NO3
-induced membrane
depolarizations were abolished (Fig. 4).
The addition of Na+ (as
Na2SO4) at concentrations
as low as 250 µM to NaCl-free ASW (sorbitol-ASW) restored
the NO3
-induced
depolarizations observed in NaCl-ASW (Figs. 4 and
5). In contrast,
NO3
additions in the
presence of KCl did not produce any effect (Fig. 4) and depolarizations
were of the same order when Na+ was added as NaCl
or Na2SO4 (data not shown).

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Figure 4.
NO3 -induced
depolarizations in the presence and absence of Na+. Lines
show the response of Em of a single
mesophyll leaf cell to 100 µM KNO3 addition
( ). The tissue was incubated sequentially in different media: ASW
containing NaCl (NaCl-ASW), NaCl-free ASW (sorbitol-ASW), and
sorbitol-ASW to which KCl or Na2SO4 were added
as indicated. Downward arrows indicate onset of
NO3 wash.
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Figure 5.
Effect of increasing Na+
concentrations on NO3 -induced depolarization.
Leaf cells were incubated in NaCl-free ASW (sorbitol-ASW) and
challenged with saturating NO3 concentrations
(100 µM KNO3). Na+ was added as
Na2SO4. The data are the means ± SE of three independent replicates. The solid line
represents a non-linear least squares fit of the data to the
Michaelis-Menten equation.
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The kinetics with respect to Na+ ions was further
investigated, with depolarization in response to saturating
NO3
concentrations (100 µM) monitored over a range of Na+
concentrations (Fig. 5). The results demonstrate that the response is
effectively saturated at around 5 mM
Na+. Fitting of the data with the
Michaelis-Menten equation yielded a Km
of 0.72 ± 0.18 mM Na+
and a maximum depolarization of 13.1 ± 0.7 mV.
Effect of Monensin on NO3
-Induced
Depolarizations
The ionophore monensin, which dissipates the electrochemical
potential for Na+ (Pressman, 1976
), was added to
the assay medium at a concentration of 50 µM to determine
its effects on the
NO3
-induced
depolarization. The presence of monensin in absence of NO3
failed to evoke
significant changes in Em (data not
shown). However, monensin partially inhibited the depolarization
induced by NO3
(Fig. 6), showing a mean inhibition value
in tests with 100 µM NO3
of 85.0% ± 20.7%
(n = 8).

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Figure 6.
Response of Em of a
single mesophyll leaf cell to the addition of 100 µM
KNO3 (indicated by the long upward arrows) incubated in ASW
before (control) and after the addition of 50 µM
monensin. , Onset of NO3 wash.
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NO3
Uptake Rates in the Absence and
Presence of Na+
If NO3
transport in
Z. marina is Na+ coupled, then net
uptake from the medium should be enhanced in the presence of
Na+. Table I shows
that NO3
was depleted
from the medium by leaves at higher rates when
Na+ was present.
NO3
uptake rates were
measured in NaCl-free ASW (sorbitol-ASW) and in the same medium but
with the addition of 10 mM
Na+ as
Na2SO4 or NaCl. The
differences between the mean
NO3
uptake rates in the
presence and absence of Na+ were significant
(t test, P < 0.05), and the addition of
Na+ more than doubled the net
NO3
uptake rate.
Furthermore, there were no significant differences between the means
obtained in the presence of
Na2SO4 or NaCl.
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Table I.
Effect of Na+ on
NO3 uptake rates
Whole leaves were incubated in different assay media: ASW containing
0.5 M NaCl (NaCl-ASW) or ASW in which NaCl was substituted
with 0.8 M sorbitol (sorbitol-ASW). Additions of
Na+ were made to sorbitol-ASW as shown.
NO3 uptake rates were measured in the light
except where indicated. The values shown are the means ± SE of three replicates of a representative experiment.
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The uptake of NO3
was
also measured in ASW containing 0.5 M NaCl in the light and
in the dark. The difference between the mean values was significant
(t test, P < 0.1), being 2-fold higher in
the light than in the dark (Table I).
 |
DISCUSSION |
The depolarizations induced by
NO3
in Z. marina indicate that the uptake of this anion is coupled with the
inward movement of positive charge. However, since the magnitude of the
depolarization is decreased at acid pH, it appeared possible that in
this plant NO3
uptake is
not coupled with the entrance of H+ as is the
rule in other angiosperms (Ullrich, 1992
). Nevertheless, the decrease
in depolarization observed at low pH might be explained by a direct pH
effect on transporter kinetics or by an increase in membrane conductance.
In contrast, the lack of any
NO3
-induced
depolarization in Na+-free ASW and the restoring
of the depolarization when Na+ is added to the
medium suggest that NO3
uptake into leaf cells is coupled with the entrance of
Na+. The stimulation of
NO3
uptake rates by the
leaves in the presence of Na+ points to the same
conclusion, as does the inhibition of
NO3
-evoked
depolarizations in the presence of monensin, an ionophore that
dissipates the Na+ electrochemical gradient.
However, because monensin, like other cation-H+
exchangers, acts as an uncoupler of photosynthesis and respiration (Rottenberg, 1977
), the ionophore might also affect
NO3
transport indirectly
via an effect on nitrogen metabolism.
Na+-coupled
NO3
transport has been
demonstrated previously only in the marine diatom Phaeodactylum
tricornutum (Rees et al., 1980
) and in cyanobacteria, where it has
been well defined (Lara et al., 1993
). Calculated
Km values for
NO3
(2.31 ± 0.78 µM) and Na+ (0.72 ± 0.18 mM) in Z. marina are quite
similar to the values reported in the cyanobacterium
Anacystis nidulans, which exhibits a
Km for
NO3
of 1.6 ± 0.2 µM and for Na+ of
0.36 ± 0.04 mM (Rodríguez et al.,
1994
). The Km for
Na+ in Z. marina is also close to the
value reported for the marine diatom (2.58 ± 0.56 mM, Rees et al., 1980
). These low-millimolar Km values for
Na+ imply that the
NO3
transporter of
Z. marina, as well as those of the other organisms, will be
functioning at saturating Na+ concentrations in a
marine environment. It should be noted, though, that the
Km for Na+
reported in the present study was derived at a saturating concentration of NO3
, and that a rise
in Km as the concentration of the
substrate ion is lowered cannot be precluded (Sanders et al., 1984
).
Other features of NO3
transport are similar in Z. marina and cyanobacteria.
NO3
uptake in
cyanobacteria is inhibited by 60% in the presence of 25 µM monensin (Rodríguez et al., 1992
);
in Z. marina, 50 µM monensin
produces an inhibition of the
NO3
-induced
depolarizations of about 85%. Moreover, a cyanobacterium mutant
lacking NO3
reductase
activity shows an inhibition of
NO3
uptake at
concentrations around 25 µM (Rodríguez
et al., 1994
). In Z. marina
NO3
-evoked
depolarizations, as well as
NO3
uptake, are smaller
in the dark and depolarizations reach saturation at lower concentration
values than in the light. The lower
NO3
uptake rate in the
cyanobacterium mutant is explained by apparent substrate inhibition of
the transporter (Rodríguez et al., 1994
), as
NO3
cannot be reduced.
This effect might also be invoked here to explain the decrease in
NO3
transport in the dark
observed in Z. marina, as it is known that NO3
reductase activity
declines in the absence of light mainly due to a lack of reducing power
(Beevers and Hageman, 1980
).
Maximum NO3
-induced
depolarizations measured in Z. marina are of the same order
as the values reported in Arabidopsis root hairs (Meharg and Blatt,
1995
; Wang and Crawford, 1996
). The response of
Em when
NO3
is washed is more
complex in Z. marina than in Arabidopsis root hairs, and it
is different in the light and in the dark. This suggests a role of N
metabolism in determining the effect of
NO3
additions on
Em (Mistrik and Ullrich, 1996
) that
could be more important in the light and in photosynthetically active tissue.
A kinetic study of Na+-dependent
NO3
transport in A. nidulans indicates that Na+ and
NO3
ions are the real
substrates of the transporter and a minimum stoichiometry of one
Na+ per
NO3
and a maximum of two
has been proposed (Rodríguez et al., 1994
). In Z. marina, the stoichiometry must be >1, since we have recorded membrane depolarization in response to
NO3
.
Z. marina, as an angiosperm, evolved from terrestrial
species that presumably, like extant species, transported
NO3
from the soil using
H+-coupled transport systems. Therefore the
question arises as to why Na+-coupled
NO3
transport evolved in
Z. marina. This question might best be addressed by
considering the thermodynamic aspects of cation-coupled
NO3
transport in a marine
environment, and that requires knowledge of the respective
NO3
,
Na+, and H+ electrochemical
potentials across the plasma membrane. Cytosolic concentrations of
NO3
([NO3
]c)
and Na+
([Na+]c) have been
estimated in some marine plants, showing a range for
Na+ of 1 to 50 mM and for
NO3
of 0 to 1 mM (Raven, 1984
). More accurate cytosolic
measurements in non-marine plants give values of 3 to 5 mM for
NO3
in barley root
epidermal cells (Walker et al., 1995
; van der Leij et al., 1998
) and 50 mM for Na+ in a
salt-tolerant Chara species (Kiegle and Bisson, 1996
).
(Although total internal Na+ concentrations have
been estimated in two species of seagrass, being around 100 mM in epidermal leaf cells and showing higher values in other tissues [Beer et al., 1980
], such estimates will reflect primarily the composition of the large central vacuole rather
than that of the cytosol.) We might therefore take as reasonable estimates of
[NO3
]c
and [Na+]c in Z. marina respective values of 3 and 50 mM. The
cytosolic pH has been measured as 7.3 in leaf cells of this species
(Fernández et al., 1999
) and the membrane potential is typically
160 mV. Normal seawater concentrations of
NO3
and
Na+ can be taken as 10 µM
and 550 mM, respectively, and the pH is typically
8.0. The generalized free energy relationship for a plasma membrane
cation-NO3
symporter
operating with a stoichiometry of n cations per
NO3
is given (in
millivolts) as
|
(1)
|
where C+ is the coupling cation
(either Na+ or H+) and
subscripts o and c denote the external solution and cytoplasm,
respectively. Figure 7 shows the
resulting free energy relationships for hypothetical cation-NO3
symporters
operating in conditions appropriate to Z. marina. Clearly,
in the case of H+ coupling, a stoichiometry of
two is not sufficient to drive net uptake (free energy > 0), and even
a stoichiometry of three yields only a modest inward driving force of
5 kJ mol
1. It is likely that a still higher
value of n would be required to guarantee
NO3
influx in varying
external conditions. By contrast, Na+-coupled
transport would be strongly inwardly directed (
13 kJ mol
1), with a stoichiometry of just
2Na+:NO3
(Fig. 7).

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Figure 7.
Thermodynamic relationship of hypothetical
NO3 transporters employing either
H+ or Na+ as the coupling ion. Calculations
were performed with Equation 1, with parameter values assigned as
discussed in the text.
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NO3
transport kinetics in
Z. marina indicates the existence of a high-affinity
transport system, with a much lower Km
(2.31 ± 0.78 µM) than has to date been
reported for other angiosperms (where values reside in the range 6-20
µM, Crawford and Glass, 1998
), although the
value in Z. marina is in the same range (2-13 µM) as that described for marine algae (DeBoer,
1985
), the fungus Aspergillus nidulans (1 µM, A.J. Miller, personal
communication), and cyanobacteria (Rodríguez et al.,
1994
). The low Km observed in Z. marina is very likely to be an adaptation to an environment in
which NO3
concentrations
are typically <10 µM.
In higher plants, two high-affinity systems for
NO3
have been defined:
one inducible and another one constitutive (Wang and Crawford, 1996
;
Crawford and Glass, 1998
). We have found that the
Em response to
NO3
addition in N-starved
plants does not show any lag, which might indicate the existence of a
constitutive high-affinity system. However, we have also detected an
increase in the magnitude of depolarizations after repeated additions
of NO3
(data not shown),
which could be the manifestation of an inducible transport system.
In conclusion, several lines of evidence indicate that a
Na+-dependent high-affinity
NO3
transport system
operates in Z. marina. This is the first report of
Na+-dependent
NO3
transport in an
angiosperm and points to the potential relevance of
Na+-coupled transport in halophytic species. The
Na+ dependence of
NO3
transport in Z. marina also suggests that other anions could enter the cell using
a similar mechanism, and studies of other anion transporters are now in progress.
Received July 9, 1999; accepted November 16, 1999.