Vol. 280, Issue 3, R612-R622, March 2001
Electrogenic Na+-dependent
L-alanine transport in the lizard duodenum. Involvement
of systems A and ASC
Virtudes
Medina,
Antonio
Lorenzo, and
Mario
Díaz
Laboratorio de Fisiología Animal, Departamento de
Biología Animal, Universidad de La Laguna, 38206 Tenerife,
Spain
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ABSTRACT |
L-Alanine transport across the isolated duodenal mucosa of
the lizard Gallotia galloti has been studied in Ussing
chambers under short-circuit conditions. Net L-alanine
fluxes, transepithelial potential difference (PD), and short-circuit
current (Isc) showed concentration-dependent relationships.
Na+-dependent L-alanine transport was
substantially inhibited by the analog
-methyl aminoisobutyric acid
(MeAIB). Likewise, MeAIB fluxes were completely inhibited by
L-alanine, indicating the presence of system A for
neutral amino acid transport. System A transport activity was
electrogenic and exhibited hyperbolic relationships for net MeAIB
fluxes, PD, and Isc, which displayed similar apparent
Km values. Na+-dependent
L-alanine transport, but not MeAIB transport, was partially inhibited by L-serine and L-cysteine,
indicating the participation of system ASC. This transport activity
represents the major pathway for L-alanine absorption and
seemed to operate in an electroneutral mode with a negligible
contribution to the L-alanine-induced electrogenicity. It
is concluded from the present study that the active
Na+-dependent L-alanine transport across the
isolated duodenal mucosa of Gallotia galloti results from
the independent activity of systems A and ASC for neutral amino acid transport.
neutral amino acid absorption; Na+-coupled amino acid
transport; reptilian intestine
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INTRODUCTION |
TRANSPORT PROCESSES
ACROSS the small intestine enterocytes involve the uptake from
the gut across the brush-border membrane and the exit to the portal
blood across the basolateral membrane. It is generally accepted that
the uphill transport of amino acids in intestinal cells occurs
secondarily to the coupling of amino acid transfer to the metabolic
energy stored in the transmembrane Na+ electrochemical
gradient, which is maintained by the activity of the basolateral
Na+-K+-ATPase. This vectorial movement of
sodium occurs with a concomitant change in the transepithelial
potential difference and has led researchers to establish that the
Na+-coupled amino acid cotransport across the apical
membranes of small intestine is both rheogenic and conductive
(22, 29).
It has been shown that amino acid transport across the small intestinal
epithelium comprises several Na+-dependent and -independent
transport systems (11, 29, 30). For neutral amino acids,
the existence of systems that transport [NBB system (neutral brush
border system, transports most neutral amino acids but excludes
MeAIB); system A; system ASC; Phe system (primarily phenylalanine,
glycine, and methionine);
-amino (
-amino acids such as taurine
and
-alanine); Imino (imino acids such as proline, hydroxyproline);
and the Na+-independent system L] have been
reported in isolated cells or membrane vesicles obtained from the small
intestine of different species of mammals (11, 19, 30).
Recently, we have demonstrated the presence both of
Na+-dependent and -independent active-transport mechanisms
for L-alanine in the duodenum of the lizard Gallotia
galloti (13).
In the present study, with the use of the short-circuit technique
together with radioisotope fluxes, we aimed at determining the
characteristics of the Na+-dependent L-alanine
transport in the isolated lizard duodenum to identify the possible
transport systems involved as well as their individual contribution to
the overall amino acid absorption. Finally, we explored the
electrophysiological correlations associated with the activity of the
different Na+-dependent L-alanine transport systems.
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MATERIAL AND METHODS |
Animals and solutions.
Adult male lizards (Gallotia galloti) weighing 25-40 g
were killed by spinal transection, and the duodenum was removed and rinsed in ice-cold bathing solution. The standard bathing solution contained (in mM) 107 NaCl, 4.5 KCl, 25 NaHCO3, 1.8 Na2HPO4, 0.2 NaH2PO4,
1.25 CaCl2, and 1.0 MgCl2 and had a final pH of
7.3. The intestinal segments were mounted in water-jacketed Ussing chambers with exposed area of 0.21 cm2 and bathed on both
sides with 4 ml of Ringer solution. Chambers were continuously
gassed with 5% CO2 and 95% O2, and the
temperature was maintained at 27°C. In some experiments, choline was
used to replace sodium ions in the bathing solutions.
Electrical measurements.
The electrical measurements were made as described previously
[using calomel (for voltage sensing) and Ag/AgCl electrodes (for
current passage) connected to the bathing solutions through 4%
(vol/wt) agar bridges (4, 13)]. Electrical measurements were continuously monitored with an automatic computer-controlled voltage-clamp device (AC-microclamp). The tissues were
first incubated under open-circuit conditions for 20 min and then
short-circuited; the potential difference (PD) and the short-circuit
current (Isc) were determined every minute. Every
5 s the tissues were pulsed with ±10 µA pulses of 1-s duration,
and from the displacement of the PD, the tissue conductance
(Gt) was derived. Corrections for electrode
offset potential and solution resistance were determined at the
beginning of every experiment and stored in the computer-controlled voltage-clamp device.
Transepithelial fluxes.
Unidirectional amino acid fluxes were measured under short-circuit
conditions using the procedure described in detail by Bolaños et
al. (4). Briefly, 20 min after the tissues were properly mounted in the chamber, 5.0 µCi of the appropriate labeled substrate [3H-labeled L-alanine or
14C-labeled methylaminoisobutyric acid (MeAIB)] were added
to the serosal or mucosal sides of the tissue. After an additional 20 min, by which isotope fluxes had reached the steady state, duplicate 200-µl aliquot samples were taken from the unlabeled side at regular 20-min intervals for 1 h and replaced by an equal volume of Ringer solution. Isotope radioactivity was measured in a liquid scintillation spectrometer (LKB-1209, Rackbeta), and the unidirectional and net
fluxes were determined using a computer program written in our
laboratory (12) that also provided the statistical tools required for data analysis. Inhibition experiments were carried out by
adding small volumes (100 µl) of concentrated stock solutions, containing the amino acids or analogs, to the mucosal and/or serosal compartments.
Statistical and mathematical analysis.
Results are expressed as means ± SE. Statistical comparison of
mean values was made using one-way ANOVA, and two-tailed Students's t-test were appropriate. Curve fitting of experimental data
was performed by nonlinear regression analysis by using a
computer-iteration procedure provided in the SigmaPlot package (Jandel
Scientific). Experimental PD and Isc data were fitted to the
following equations:
And
where Km is the apparent Michaelis-Menten
constant, PDmax and Iscmax are the
PD and Isc estimates at saturation, and PDo and
Isco are the background PD and Isc
(offset) values obtained in the absence of substrate, respectively. The
normalized PD (
PD) and Isc (
Isc) parameters
were calculated by subtracting the average offset values from the
corresponding electrical parameters.
Materials.
MeAIB, L-alanine, L-cysteine, and
L-serine were obtained from Sigma-Aldrich.
3H-labeled L-alanine and
14C-labeled MeAIB were purchased from Amersham
Ibérica. All reagents used were analytical grade.
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RESULTS |
Transepithelial L-alanine fluxes.
Figure 1A illustrates the
results of unidirectional and net fluxes of L-alanine (1 mM) across the isolated lizard duodenum measured under short-circuit
conditions. With the use of Na+-containing Ringer
solutions, the mucosal-to-serosal flux (Jms) was 50.9 ± 4.9 nmol/cm2 · h, whereas the serosal-to-mucosal
flux (Jsm) was 35.8 ± 5.8 nmol/cm2 · h, resulting in a statistically
different from zero net absorptive flux (Jnet) of 15.2 ± 1.7 nmol/cm2 · h (P < 0.01).
Replacement of the standard Ringer solution with an
Na+-free solution brought about a considerable reduction of
Jms compared with the value in the presence of
Na+, with no change in Jsm, which significantly
decreased Jnet to 7.8 ± 0.1 nmol/cm2 · h (P < 0.01), still
significantly different from zero (P < 0.05). This is
in agreement with our previous observations demonstrating that the
lizard duodenum displays Na+-dependent and -independent
L-alanine transport pathways (13).

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Fig. 1.
A: unidirectional and net
L-alanine fluxes across the duodenal mucosa of the lizard
Gallotia galloti under short-circuit conditions in the
presence (Ringer solution) and in the absence of sodium
(Na+ free). L-Alanine was added to both sides
of the tissue at a final concentration of 1 mM. Results are means ± SE for 12 determinations. Jms, unidirectional
mucosa-to-serosa L-alanine flux; Jsm,
unidirectional serosa-to-mucosa L-alanine flux;
Jnet, net L-alanine flux. **Significant
difference (P < 0.01) between the presence and the
absence of sodium. B: concentration dependence for net
L-alanine flux under short-circuit conditions. The
rectangular hyperbola represents the Michaelis-Menten fit for the data
as deduced by nonlinear regression analysis. Each measurement is
mean ± SE of 6 different experiments.
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Kinetic analysis of L-alanine fluxes.
The kinetic characteristics of L-alanine transport in the
presence of sodium were further assessed under short-circuit conditions and in the presence of identical L-alanine concentrations
(50 µM to 10 mM) on both the mucosal and serosal reservoirs. Thus the
changes on the net transepithelial fluxes are entirely attributable to
active-transport processes, because the diffusive components are
presumably identical in the two opposite directions (mucosa-to-serosa and serosa-to-mucosa).
As can be seen in Fig. 1B, the increase on the external
L-alanine concentration was followed by a hyperbolic rise
on the calculated net L-alanine fluxes. The kinetic
constants describing this saturable transport were computed by
nonlinear regression and were as follows: apparent
Km = 0.18 ± 0.01 mM; maximum flux
(Jmax) = 47.6 ± 2.9 nmol/cm2 · h. Interestingly, the
Jmax value determined under these conditions was about
threefold that obtained in the absence of sodium (14.8 ± 1.3 nmol/cm2 · h) (13) and strongly
indicates the presence of an Na+-dependent carrier-mediated
pathway being responsible for the majority of transepithelial
L-alanine transport.
Kinetic analysis of L-alanine-induced
electrical responses.
To determine the possible relationship between the concentration of
L-alanine in the bathing solutions and the bioelectrical parameters, we accomplished the analysis of the variations on the PD
and Isc in response to changes in the external
L-alanine concentration. The concentration-response curves
for the PD and Isc elicited in the range of
L-alanine concentrations tested (Fig. 2) demonstrated that both PD and
Isc displayed hyperbolic relationships. The kinetic
parameters that were computed from nonlinear regression-fitting analysis to the saturation equations (see METHODS) showed
apparent Michaelis constant values (apparent Km)
of 0.42 ± 0.17 mM and 0.36 ± 0.17 mM for PD and
Isc, respectively, which were not statistically different.
The PDmax and Iscmax estimates,
representing the L-alanine-induced increase on PD and
Isc values at saturation, were 1.39 ± 0.16 mV and
8.89 ± 1.14 µA/cm2, and the values of
PDo and Isco obtained in the absence
of L-alanine were 2.49 ± 0.11 mV and 22.07 ± 0.85 µA/cm2, respectively. The values of PDo
and Isco were similar to those reported earlier
for the lizard duodenum in the presence of sodium (24) and
are consistent with the existence of a basal electrogenic Na+ absorption that accounts for ~50% of the total
sodium uptake (24).

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Fig. 2.
Kinetic analyses of potential difference (PD;
A) and short-circuit current (Isc; B)
at increasing L-alanine concentrations added to both sides
of the epithelia. Data were fitted to the apparent Michaelis-Menten
(Kmap) equation (for details, see MATERIAL
AND METHODS). The insets show the Lineweaver-Burk
plots for the L-alanine-induced electrical effects. Each
point corresponds to the mean of 16 determinations.
Iscmax, Isc estimate at saturation;
Isco, Isc values obtained in the
absence of substrate.
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In addition, the regression analysis performed on the results of the
experiments in which the electrical PD, Isc, and amino acid
fluxes were measured simultaneously (Fig.
3) revealed the existence of a positive
correlation between
PD or
Isc and Jnet or
Jms (P < 0.05, r2 > 0.81 in all cases). The fact that the slope constants for each dependent variable (
PD or
Isc) were similar for
Jms or Jnet indicate that the magnitude of
L-alanine fluxes may be estimated from the change of either
PD or
Isc.

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Fig. 3.
Regression analyses for the L-alanine fluxes
and normalized PD ( PD; A) or Isc
( Isc; B) simultaneously determined in the same
tissues. Linear regression equations and correlation coefficients are
indicated. JL-alanine,
L-alanine flux.
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Effects of MeAIB on transepithelial
L-alanine fluxes, PD and
Isc.
In an attempt to identify different transport systems carrying
L-alanine in the isolated lizard duodenum, we used
well-known specific analogs and substrates to emphasize the differences
in molecular recognition by each transport system. It has been
described that amino acid analogs with N-methyl group on
-amino N are recognized by system A and are excluded by other
systems. The unidirectional and net fluxes of L-alanine (1 mM) across the isolated lizard duodenum in the absence and in the
presence of saturating concentrations of MeAIB (20 mM) in the bathing
solution are given in Fig. 4A. Under control conditions, using Na+-containing Ringer
solutions, Jms was 33.1 ± 3.4 nmol/cm2 · h and Jsm was 25.4 ± 2.9 nmol/cm2 · h, resulting in a statistically
different from zero net absorptive Jnet of 7.7 ± 0.5 nmol/cm2 · h (P < 0.01). Once the
analog was added to the bathing solutions, both Jms and
Jnet were considerably decreased compared with control conditions (Fig. 4A). Thus Jms was reduced to
24.8 ± 2.9 nmol/cm2 · h and the calculated
Jnet was decreased by 41.3% down to 4.2 ± 0.1 nmol/cm2 · h (P < 0.01). The
finding that this Jnet was significantly different from zero
(P < 0.05) strongly indicates that the lizard duodenum
possesses different Na+-dependent L-alanine
transport pathways. Interestingly, despite the dramatic reduction of
L-alanine Jms and Jnet caused by the addition of MeAIB, neither the transepithelial PD nor the
Isc were affected by the addition of the amino acid analog
(Table 1, L-alanine
experiments).

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Fig. 4.
A: effects of -methyl aminoisobutyric acid
(MeAIB) on L-alanine unidirectional and net fluxes under
short-circuit conditions in the presence of Na+ in the
bathing solutions. MeAIB was added to both sides of the tissues to
yield a final concentration of 20 mM. The concentration of
L-alanine was 1 mM throughout the experiment. B:
effect of L-alanine on unidirectional and net MeAIB fluxes
under short-circuit conditions in the presence of sodium in the bathing
solutions. The concentrations of MeAIB and L-alanine were
10 and 20 mM, respectively. L-alanine was added to the
bathing solutions 20 min after the control values were obtained.
C: concentration dependence for net MeAIB flux under
short-circuit conditions. The rectangular hyperbola represents the
Michaelis-Menten fit for the data as deduced by nonlinear regression
analysis. Results are mean ± SE for 8 (A and
B) and 6 (C) different experiments. Statistically
different from the control (*P < 0.05 and
**P < 0.01).
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Parallel experiments performed under Na+-free conditions
showed that MeAIB produced no appreciable changes on
L-alanine transport (data not shown), indicating that the
effects of MeAIB were remarkably dependent on the presence of
Na+.
Effects of L-alanine on
MeAIB fluxes, transepithelial PD, and Isc.
Because a substantial amount of Na+-dependent alanine
uptake was inhibited by the system A-specific analog MeAIB, we designed experiments to test whether active MeAIB transport could be measured under short-circuit conditions and, if this was the case, to determine whether MeAIB fluxes were affected by the addition of
L-alanine. The results of these experiments are shown in
Fig. 4B. As can be seen, MeAIB fluxes were 15.4 ± 1.6 (Jms) and 9.3 ± 0.7 (Jsm) nmol/cm2 · h, resulting in a Jnet value
of 6.1 ± 0.3 nmol/cm2 · h. Addition of
L-alanine (20 mM) to the bathing solutions brought about a
considerable reduction of Jms and Jnet, with
Jnet not statistically different from zero.
Together, these experiments clearly demonstrate the presence of a
system A-like component involved in the duodenal transport pathways for
L-alanine. Interestingly, the inhibition of MeAIB fluxes
caused by the addition of L-alanine was accompanied by a
significant increase in the Isc and PD, whereas the tissue
conductance was not changed (Table 1, MeAIB experiments). These results
indicated that in addition to the system A activity, L-alanine had activated another electrically conductive process.
Kinetic analysis of MeAIB transport.
Figure 4C summarizes the results of the experiments designed
to determine the concentration-response curves for transepithelial MeAIB fluxes under short-circuit conditions. As can be seen in Fig.
4C, net MeAIB fluxes followed a saturable transport kinetic with an apparent Km of 0.64 ± 0.20 mM and
the Jmax was 6.9 ± 0.4 nmol/cm2 · h. These results strongly suggest the
presence of a carrier-mediated system being responsible for net MeAIB transport.
The concentration-response curves for PD and Isc elicited in
the presence of different concentrations of MeAIB (Fig.
5) also revealed hyperbolic relationships
with apparent Michaelis constants of 0.47 ± 0.07 and 0.45 ± 0.1 mM for PD and Isc, respectively, which were not
statistically different. The PDmax and
Iscmax estimates, representing the MeAIB-induced
increase on PD and Isc values at saturation, were 0.50 ± 0.02 mV and 3.26 ± 0.17 µA/cm2, respectively.
The offset values, corresponding to the PDo and Isco obtained in the absence of
L-alanine, were 1.50 ± 0.02 mV and 20.10 ± 1.37 µA/cm2, respectively. Preliminary experiments performed
in the absence of sodium showed that MeAIB addition to the bath failed
to produce any appreciable effect on either PD or Isc;
hence, the electrogenic effects of MeAIB transport are consistent with
MeAIB/Na+ cotransport activity.

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Fig. 5.
Kinetic analyses of PD (A) and Isc
(B) with increasing MeAIB concentrations added to both sides
of the epithelia. Data were fitted to the Michaelis-Menten equations
indicated in MATERIAL AND METHODS. The insets
show the Lineweaver-Burk plots for the MeAIB-induced electrical
effects. Each point corresponds to the mean of 16 determinations.
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Given the hyperbolic relationship between the electrical parameters and
the L-alanine concentration, we performed regression analysis to test whether the magnitude of the unidirectional or net
fluxes could provide a prediction of the change on the
PD or
Isc. The results shown in Fig.
6 show that the data could be
significantly fitted to linear equations with
r2 > 0.84 in all cases, indicating that
the magnitude of net MeAIB fluxes may be adequately inferred from the
change of either
PD or
Isc.

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Fig. 6.
Regression analyses for the MeAIB fluxes and PD (A) or
Isc (B) simultaneously determined in the same tissues.
Linear regression equations and correlation coefficients are
indicated.
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MeAIB-resistant, sodium-dependent
L-alanine transport.
The next set of experiments was designed to test whether active
MeAIB-resistant L-alanine transport could be ascribed to
the presence of some other neutral amino acid transport system, using a
substrate-discrimination methodology under short-circuit conditions. Figure 7 shows the results of the effects
of L-serine, L-cysteine (typical substrates for
system ASC), and L-threonine (substrate for system NBB) on
L-alanine unidirectional and net fluxes. As can be seen, in
the presence of sodium, both L-serine and
L-cysteine (Fig. 7, A and B) markedly
reduced the mucosa-to-serosa and net L-alanine fluxes,
whereas L-threonine was without effect (Fig. 7C). Both amino acids, L-serine and
L-cysteine, inhibited L-alanine transport by
the same magnitude (49.1% and 54%, respectively), and these effects
appear to be Na+-dependent because they were not observed
in Na+-free solutions (Fig. 7D), suggesting that
these amino acids interact with the same Na+-dependent
transport system. The inhibition by L-serine and
L-cysteine together with the absolute Na+
requirement exhibited by this transport system are compatible with
system ASC being responsible for a significant fraction of the
transepithelial alanine transport across the isolated duodenum of
Gallotia galloti. Interestingly, the addition of
L-cysteine, L-serine, or
L-threonine failed to induce any change on the
transepithelial PD, Isc, or Gt (Table
2).

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Fig. 7.
Effects of L-serine (A, D),
L-cysteine (B), and L-threonine
(C) on L-alanine unidirectional and net fluxes
under short-circuit conditions. Experiments A-C
were carried out in the presence of sodium, whereas experiment
D was performed under Na+-free conditions. The amino
acids were added to both sides of the tissue at a final concentration
of 20 mM. L-Alanine (1 mM) was present throughout the
experiments and was added to the bathing solutions 20 min before the
control values were obtained. Results are means ± SE
for 8 (A, B, and C) and 6 experiments
(D). **Statistically different from the control
(P < 0.01).
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Table 2.
Electrical parameters associated with the
Na+-dependent L-alanine
transport under control conditions and in the presence of
different amino acids and analogs
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To test for the independence of the MeAIB-transporting system (system
A) and the L-cysteine- and L-serine-sensitive
L-alanine transport system (system ASC) in the lizard
duodenum we assessed the effects of L-cysteine on MeAIB
transport. The results of these experiments are displayed in Fig.
8A. Clearly, the addition of saturating concentrations of L-cysteine did not alter
either the unidirectional or net MeAIB fluxes, indicating that the
effects of L-cysteine (and L-serine, not shown)
on the L-alanine transport observed above were due to the
inhibition of a transport system distinguishable from and independent
to that transporting MeAIB.

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Fig. 8.
A: effects of L-cysteine on MeAIB
unidirectional and net fluxes under short-circuit conditions in the
presence of sodium. L-Cysteine was added to both sides of
the tissues to reach a final concentration of 20 mM. The concentration
of MeAIB was 10 mM throughout the experiment. B: effect of
the sequential addition of MeAIB (20 mM), L-cysteine
(L-Cys; 20 mM), and cycloleucine (CL, 20 mM) on
L-alanine (1 mM) unidirectional and net fluxes under
short-circuit conditions in the presence of sodium. Results are
means ± SE for 6 different experiments. Statistically different
from the previous condition (*P < 0.05 and
**P < 0.01).
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Strikingly, the addition of L-cysteine to
MeAIB-transporting tissues did not affect any of the bioelectrical
parameters (Table 3), as it would be
expected if the activity of system ASC were electrogenic, and suggests
that although the activity of system ASC can be demonstrated under
voltage-clamp conditions and in the absence of electrochemical
gradients, its activity is clearly not electrogenic but consistent with
an active electroneutral process.
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Table 3.
Electrical parameters associated with the
Na+-dependent MeAIB transport under
control conditions and in the presence of L-cysteine
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Relative contribution of different pathways.
The evidence presented until now indicates that the
Na+-dependent L-alanine transport can be
explained in terms of the synergistic activity of two different
components, systems A and ASC. It was found interesting to assess the
relative contribution of each individual transport system to the
overall L-alanine transport across the duodenal mucosa of
G. galloti using a strategy of combining inhibitors in a
series of steps to isolate the different transport systems on the basis
of their substrate affinity (7).
As shown in Fig. 8B, L-alanine Jms
and Jnet were partially inhibited by MeAIB. When
L-cysteine was added to the incubation media, net
L-alanine fluxes were further inhibited. The percentages of
inhibition of net L-alanine fluxes by MeAIB and
L-cysteine were 43.6% and 82.2%, respectively, and were
caused by the reduction of Jms; inasmuch, neither MeAIB nor
L-cysteine significantly affected the L-alanine
Jsm. We have shown previously that MeAIB and
L-serine do not affect L-alanine transport in
the absence of sodium; thereby these effects are entirely attributable
to the inhibition of the Na+-dependent transport systems.
The remaining L-alanine Jnet (3.2 ± 0.6 nmol/cm2 · h) was totally inhibited by the addition
of cycloleucine, an amino acid analog that selectively inhibits
sodium-independent L-alanine transport in different cell
preparations, including the lizard duodenum (7, 11, 13).
Kinetic of system ASC.
Although L-cysteine has been identified as the typical
substrate for system ASC in rat hepatocytes (21), there is
general agreement that this transport system lacks an exclusive
substrate, and this has usually hindered the detailed characterization
of this transport mechanism. To characterize system ASC in the duodenal epithelium, we have further extended the criteria of identification to
include mathematical discrimination by nonlinear regression assuming
that total L-alanine transport results from the
simultaneous activity of the three transport systems identified and
coexisting here. Thus
And
where Jmax corresponds to the net flux at saturation,
Km is the apparent Michaelis-Menten constant for
each transport component [Total, A, ASC, and
Na+-Independent (Ind)], and [S] is the substrate concentration.
Thus with the use of the kinetic constants computed here for the total
and system A transport activities and the parameters determined for the
Na+-independent net fluxes reported earlier
(13), a hyperbolic concentration-dependence relationship
was obtained with an apparent Km value of 0.16 mM and a Jmax value of 25.64 nmol/cm2 · h that presumably corresponds to the
Na+-dependent ASC activity (Fig.
9A).

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Fig. 9.
A: concentration-dependence deduced for net
L-alanine transport through system ASC under short-circuit
conditions. The rectangular hyperbolas were computed by nonlinear
regression analysis according to the procedures described in
MATERIAL AND METHODS and RESULTS. B
and C: kinetic analysis of L-alanine-induced PD
(B) and Isc (C). Saturation equations
for Total (curve 1), system A, and
Na+-independent pathways (curve 2) were based on
the kinetic parameters computed over the experimental data. The dotted
line (curve 3) represents the residual PD or Isc
attributable to system ASC activity. For details see MATERIAL AND
METHODS and RESULTS sections.
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In an attempt to assess the contribution of system ASC to the
electrogenicity induced by L-alanine, we followed a similar mathematical approach by using the equations stated above. The analyses
were performed by determining the residual electrical activity obtained
by subtracting from the total electrical response those corresponding
to system A and Na+-independent transport (Fig. 9,
B and C). Interestingly, these analyses revealed
that L-alanine-induced electrogenicity (curve 1)
may be explained by the activity of two components, namely system A and
Na+-independent transport (curve 2), with little
or no contribution of system ASC (curve 3), which strongly
suggest that, at least under short-circuit conditions, this transport
system behaves as an electrically neutral transporter.
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DISCUSSION |
The present data clearly demonstrate that L-alanine
transport across the duodenal mucosa of the lizard Gallotia
galloti can take place under controlled short-circuit conditions,
in the virtual absence of transepithelial electrochemical gradients,
and both in the presence and in the absence of sodium in the bathing
solution. These data indicate that the isolated lizard duodenum
contains active processes for both Na+-dependent and
-independent L-alanine transport, being the transport in
the presence of sodium quantitatively much greater than in its absence,
a finding that agrees with the results obtained in many other
preparations from renal cultured cells to hepatocytes (3, 22,
23). Because the features of the Na+-independent
L-alanine transport have been explored in detail in a
previous publication (13), the present article focuses on
the characterization of the Na+-dependent transport.
In the presence of sodium, duodenal L-alanine net transport
displays a clear saturation kinetic that could be described by an
apparent Km of 0.18 mM and a Jmax of
47.6 nmol/cm2 · h. Because the diffusive pathways
for alanine are presumably the same in both directions, Jms
and Jsm, the transport kinetic obtained for the net
L-alanine transport under the present conditions corresponds to a carrier-mediated transport with no contribution of the
diffusive components. On the other hand, the comparison of the kinetic
constants calculated in the presence of sodium with the parameters
reported for L-alanine transport in the absence of sodium
in this same preparation (13) indicate that at saturation, ~31% of the total transport is carried by the
Na+-independent system.
The measurements of bioelectrical parameters showed that the addition
of L-alanine induced a concentration-dependent increase in
transepithelial PD and Isc, without varying
Gt. Furthermore, L-alanine-induced
changes on PD or Isc exhibited a good correlation with
Jnet. These observations strongly suggest that
L-alanine has triggered the activation of some electrogenic
process, likely carried by the transepithelial movement of sodium
toward the serosal compartment, that eventually leads to the
development of a serosally positive PD. The concentration-dependence
analyses of L-alanine-induced electrogenicity show that the
apparent Km values for PD and Isc are
very similar and confirm the observation that the electrical phenomena
associated with the amino acid transport occur without changes in the
transepithelial Gt, which is consistent with the notion that transport of substrates occurs as a secondary process coupled to the influx of Na+. Indeed, electrophysiological
studies performed using microelectrode measurements of membrane
potential in the lizard duodenum revealed that the presence of a
saturating L-alanine concentration in the Na+-containing luminal solution depolarizes the membrane
potential by 20 mV and increases the transmural potential with a
concomitant increase in the equivalent short-circuit current
(17). Similar findings have been demonstrated in other
nonmammalian preparations including Necturus intestine
(18) and Aplysia californica intestine (16).
A number of studies using uptake kinetic techniques in vesicles
obtained from mammalian small intestine have demonstrated that neutral
amino acid transport by the brush-border membranes is mediated by
different processes including Na+-dependent and
-independent systems (29, 30). Among the
Na+-dependent neutral amino acid transport systems
identified in eukaryotic animal cells so far, system A is a ubiquitous
carrier that serves mainly the uptake of amino acids with short, polar side chains. System A activity is subject to significant regulation by
hormones, but its most relevant characteristic is its tolerance of N-methylated substrates such as the nonmetabolizable
substrate MeAIB (6, 8).
The results presented here led to the conclusion that a fraction of the
total carrier-mediated Na+-dependent L-alanine
transport in the mucosal epithelium of Gallotia galloti is
actively carried by system A. Several pieces of evidence support this
conclusion: 1) unidirectional mucosa-to-serosa and net
L-alanine transport are reduced by the addition of MeAIB to the bathing solutions; 2) MeAIB fluxes can be measured under
short-circuit conditions and in the absence of electrochemical
gradients; 3) MeAIB fluxes were considerably inhibited by
the addition of L-alanine to the bathing solution; and
4) MeAIB transport across short-circuited tissues displayed
a saturation kinetic. Additionally, our data demonstrate that the
activity of system A is clearly electrogenic and displays a hyperbolic
relationship between the concentration of MeAIB and the transepithelial
PD and Isc. Furthermore, the calculated apparent
Km values for the concentration-response
analyses performed on Jnet, PD, and Isc show a
considerable similarity that can only be explained if there is a direct
relationship between MeAIB fluxes and the electrophysiological
parameters. Supporting this hypothesis, there exists a positive
correlation between Jnet and PD or Isc as
measured in the same tissues. Because active MeAIB transport has not
been observed under Na+-free conditions, the most
straightforward explanation for our results is that an
Na+/MeAIB (L-alanine) cotransport drives the
active accumulation of both substrates within the absorptive cells,
which eventually exit through the plasma membrane toward the serosal
solution via undetermined pathways. Studies performed in human
fibroblasts (9), mouse erythrocytes (32),
hepatocytes (21), rabbit distal ileum (26),
and mouse ascites tumor cells (14, 20) have shown that
Na+-symport via system A is electrogenic, affected by the
transmembrane potential, and exhibits a one-to-one stoichiometry.
Additionally, direct electrophysiological measurements have
unequivocally demonstrated that MeAIB uptake causes an
Na+-dependent membrane depolarization in Ehrlich ascites
tumor cells (10) that is consistent with the
Na+ entry into the cells during the cotransport process.
On the basis of the uptake kinetics and cross-inhibition studies, four
different Na+-dependent transport systems for neutral amino
acids have been identified in the brush-border membrane and have not
been found in other cellular preparations (1, 31): NBB,
Phe, Imino, and a
-system. The MeAIB transport observed here cannot
be attributed to the activity of the Imino system because although it
accounts for MeAIB uptake in brush-border membranes of several
mammalian intestines (1, 31), it is different from system
A because it excludes alanine and other short-chained amino acids.
L-Threonine has been shown to be an ideal substrate for the
characterization of system NBB in intestinal brush border (22, 25). We have assessed the participation of system NBB in the duodenum of G. galloti by measuring the effects of
L-threonine on the transepithelial transport of
L-alanine. The experiments summarized in Fig. 7 and Table 3
clearly indicate that saturating concentrations of
L-threonine failed to produce any appreciable change on
L-alanine transport or electrical parameters. These results
rule out a significant contribution of system NBB to transepithelial L-alanine transport in the lizard duodenum. On the
contrary, addition of either L-serine or
L-cysteine to the bathing solutions caused a considerable
inhibition of Jnet and Jms. The effects of
L-cysteine were specific for a component of
L-alanine transport pathways other than system A, because
MeAIB fluxes were not affected by the addition of
L-cysteine to the bathing solutions (Fig. 8A). Inhibition by L-serine and L-cysteine and
resistance to MeAIB confer to this mechanism the characteristics of
system ASC. This transport system has been demonstrated in a wide
variety of cell preparations (15, 21, 28) and, although
the kinetic characterization of system ASC has been hampered because of
the lack of a specific substrate, in most untransformed cell types,
system ASC is the major Na+-dependent system
(6).
Our present data also indicate that the active
Na+-independent L-alanine transport, described
earlier in this same preparation (13), might coexist with
the two Na+-dependent systems and, more interestingly, that
the combined activity of the three transport systems may explain the
whole L-alanine transport under short-circuit conditions.
This has been demonstrated by using a partition strategy combining a
series of substrates and analogs in excess to isolate components of
transport one by one, as suggested by Christensen (7).
Thus the sequential addition of MeAIB and L-cysteine served
to inhibit the Na+-dependent components of
L-alanine transport attributed to systems A and ASC. The
final incorporation of cycloleucine, a nonhydrolizable amino acid
analog, which was shown to be a potent inhibitor of the
Na+-independent H+-coupled
L-alanine transport in the lizard duodenum
(13), vanished the remaining net L-alanine
transport (Fig. 8B). Although alternative explanations are
possible, the most plausible hypothesis is that the
Na+-independent L-alanine transport might
coexist with the Na+-dependent transport systems.
In an attempt to characterize system ASC, we have included a
mathematical discrimination by nonlinear regression under the assumption that the combined activity of systems A and ASC and the
Na+-independent system accounts for the total
L-alanine transport under short-circuit conditions. The
results of these analyses revealed a hyperbolic relationship with a
Jmax of 25.6 nmol/cm2 · h, which
represents 79% of the total Na+-dependent
L-alanine transport, and an apparent
Km of 0.16 mM (Fig. 9). As judged by the
relevant kinetic parameters of transport obtained here, the apparent
affinity for alanine of the putative system ASC carrier is higher than
for system A, suggesting that at low luminal L-alanine
concentrations, the major transport component corresponds to an
Na+-mediation endowed with characteristics of system ASC.
The finding that system ASC predominates over other neutral amino acid
transport pathways has been observed in different preparations
including human fibroblasts (15), renal LLC-PK1 cells
(23), Chinese hamster ovary cells (3, 28),
and skate hepatocytes (2).
The electrical measurements obtained under short-circuit conditions
point out that system ASC behaves as an electroneutral transporter. In
support of this hypothesis, the observations that PD or Isc
were not altered when L-cysteine was added to tissues transporting MeAIB and that addition of saturating concentrations of
either L-serine or L-cysteine to
L-alanine transporting tissues also failed to induce any
electrical change. These findings were corroborated by a mathematical
approach to the experimental data aimed at determining the fraction of
transepithelial PD or Isc remaining after subtracting the
contribution of both the electrogenic Na+-independent and
system A components from the total L-alanine-induced electrogenicity. The results of these analyses clearly showed that
L-alanine-induced electrogenicity could be adequately
explained in terms of the synergistic actions of system A and the
Na+-independent system with no contribution of system ASC.
This finding is in agreement with the previous studies on human
fibroblasts demonstrating that ASC activity accommodates a nonrheogenic
model in which an electrically silent translocation, with no net
movement of charge during a complete cycle of the carrier, is dominant (5).
To our knowledge, this is the first report demonstrating multiple
pathways for L-alanine transport in the small intestine of
reptiles. Comparison of the data reported here with those of mammalian
tissues indicates that the distribution of neutral amino acid transport
systems in the lizard duodenum closely resembles that proposed for
nonepithelial cells (22, 29). The difference with regard
to the small intestine of mammals, like rabbit, rat, or pig, is
striking, since system NBB is the main transporter serving neutral
amino acids (1, 25), while systems A and ASC
activities are small or nonexistent. Nevertheless, in agreement with
our findings, detailed studies performed in guinea pig small intestine
have unambiguously concluded that the concentrative L-alanine transport in the presence of an Na+
gradient is carried out by systems A, ASC, and L both in isolated cells
(11) and brush-border membranes (19, 27). The
reasons for the different predominance of the various neutral amino
acid transport pathways between the same tissues in different species are not known. The fact that the different transport systems display different substrate specificities as well as kinetic features (transport capacity and substrate affinity) allows the intestinal absorption of amino acids taking place under a wider range of dietary
conditions, which is especially important for omnivorous species (as is
the case of G. galloti). Presumably, evolutionary pressure
may select transport systems that are most compatible with the
nutritional requirements and food availability.
Perspectives
It has been ascertained that some transport systems (like system
A) are clearly subject to adaptive regulation, a phenomena by which the
expression levels of a particular transport protein are influenced by
the availability of substrates (22). Although the
regulation of amino acid transport systems has not been explored in
reptiles, this mode of regulation is likely to be relevant in this
group of vertebrates inasmuch as the metabolic needs vary during
hibernation, starvation, or reproduction periods. Indeed, we have
observed a dramatic reduction of transepithelial L-alanine transport in animals captured in midwinter, where starvation is common
(unpublished observations). At present, we are undertaking new
experiments to ascertain the possible short- and long-term regulation
of the different transport systems demonstrated in the duodenal mucosa
of Gallotia galloti.
 |
ACKNOWLEDGEMENTS |
We express our gratitude to L. Acosta for excellent technical
assistance and almost maternal maintenance of the lizards in a
"five-star" terrarium. Also, we are very grateful to Prof. Miquel Moretó and Dr. Simon P. Hardy for advice and critical reading of
the manuscript. We thank Neil Abrey for the careful and conscientious revision of English usage throughout the manuscript.
 |
FOOTNOTES |
Address for reprint requests and other correspondence: M. Díaz, Laboratorio de Fisiología Animal, Departamento de
Biología Animal, Universidad de La Laguna, 38206 Tenerife,
Spain (E-mail: madiaz{at}ull.es).
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.
Received 8 June 2000; accepted in final form 27 September 2000.
 |
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