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Am J Physiol Regul Integr Comp Physiol 276: R1479-R1488, 1999;
0363-6119/99 $5.00
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Vol. 276, Issue 5, R1479-R1488, May 1999

Effect of hyposmotic challenge on microvillous membrane potential in isolated human placental villi

T. J. Birdsey1, R. D. H. Boyd2, C. P. Sibley1, and S. L. Greenwood1

1 Department of Child Health and School of Biological Sciences, University of Manchester, St. Mary's Hospital, Manchester, M13 0JH; and 2 St. George's Hospital Medical School, London, SW17 0RE United Kingdom


    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

This study examined the effect of hyposmotic solutions on the syncytiotrophoblast microvillous membrane potential (Em) in mature intermediate villi isolated from term human placentas. When villi were exposed to a control solution (280 mosmol/kgH2O; 116 mM NaCl) and then to either a 138-hyposmotic (138 mosmol/kgH2O; 37 mM NaCl) or 170-hyposmotic (170 mosmol/kgH2O; 55 mM NaCl) solution, there was a significant hyperpolarization of Em (-5.1 ± 1.5 mV, P < 0.01 and -5.0 ± 0.5 mV, P < 0.001, respectively; n = 10), which was reversible on removal of the hyposmotic stimulus. Low-NaCl (37 and 55 mM) solutions made isosmotic with control (i.e., 280 mosmol/kgH2O) by addition of raffinose did not significantly alter Em, suggesting that reducing NaCl concentration per se had no effect on Em. Exposure to 170-hyposmotic solution in the presence of 5 mM BaCl2 depolarized Em by +4.1 ± 0.7 mV (P < 0.001, n = 6); BaCl2 similarly depolarized Em when added in control solution (+5.6 ± 1.1 mV, n = 5). Exposure to 170-hyposmotic solution containing 1 mM DIDS hyperpolarized Em by -9.0 ± 1.7 mV (P < 0.001, n = 5). This degree of hyperpolarization was significantly greater than that observed in hyposmotic solution alone (P < 0.01) but was not different from the hyperpolarization when DIDS was added to control solution (-7.4 ± 0.2 mV, n = 6). We conclude 1) that Ba2+-sensitive K+ conductances and DIDS-sensitive anion conductances contribute to the resting potential of the syncytiotrophoblast microvillous membrane and 2) that the syncytiotrophoblast microvillous membrane responds to a hyposmotic stimulus by activating both Ba2+-sensitive K+ and DIDS-sensitive anion conductances.

potassium; chloride; conductance; placenta; volume regulation


    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

THE PLACENTA plays a central role in the transfer of solutes and water between mother and fetus. The major functional components of the human placenta are the villi, which project into the intervillous space, where they are bathed in maternal blood. The capillary circulation of the villus is supplied via the umbilical cord of the fetus. During the last two-thirds of pregnancy, the barrier that separates maternal blood in the intervillous space from fetal blood in the villus capillaries comprises two cell layers: the syncytiotrophoblast, in immediate contact with maternal blood, and the fetal capillary endothelium. The syncytiotrophoblast is thought to be the transporting epithelium of the human placenta (24). It is a true syncytium that extends over the entire surface of the villous tree. The plasma membrane of the syncytiotrophoblast facing the intervillous space is covered in microvilli [the microvillous membrane (MVM)] (22).

In epithelia the control of cellular hydration is challenged by changing solute transport rates (19). If solute uptake exceeds solute exit, accumulation of osmolytes in the cytoplasm leads to intracellular hypertonicity, water entry, and cell swelling (18). Under these circumstances, volume regulatory mechanisms are initiated to return cell volume to its original value [regulatory volume decrease (RVD)] (19, 20, 34). When cell swelling is induced experimentally by exposure to a hyposmotic solution, RVD is achieved by the loss from the cell cytoplasm of inorganic osmolytes, predominantly K+ and Cl- (13, 19, 20, 34) and organic solutes, for example amino acids, methylamines, and polyols (19, 35).

In fulfilling its role in effecting maternofetal solute exchange, the syncytiotrophoblast is exposed to conditions that challenge cell volume homeostasis. Indeed, there is evidence to suggest that the placenta, in common with other epithelia, has the ability to regulate its volume. For example, fragments of placental tissue and cytotrophoblast cells isolated from human placenta respond to a hyposmotic stimulus by releasing 86Rb, used as a marker for K+ (8, 15, 16); 125I, used as a marker for Cl- (31, 37); and amino acids, including taurine, glutamic acid, methylaminoisobutyric acid, and aspartate (27, 32, 33). However, as yet there is little information concerning the mechanisms of swelling-induced osmolyte loss. Furthermore, it is not known whether, in the intact placental villus, the solutes lost during RVD pass over the basal membrane of the syncytiotrophoblast into the fetal circulation or cross over the MVM into maternal blood.

There are several mechanisms by which K+ and Cl- are lost from the cytoplasm in response to cell swelling, including the activation of K+ and Cl- channels, KCl cotransport, and coupled K+/H+ and Cl-/HCO-3 transporters (19, 20). Activation of K+ and Cl- channels is probably the predominant mechanism effecting K+ and Cl- loss in epithelial cells (18). The activation of K+ and Cl- conductances in response to swelling has been shown to affect the potential across the plasma membrane of cells in culture [e.g., liver (12, 13), proximal tubule (11), colonic carcinoma (3), and Madin Darby canine kidney cells (26, 29)] and across the basolateral membrane of cells in intact tissues such as the intestine and gallbladder (30, 36).

The primary aim of this study was to determine whether ions are lost over the microvillous membrane of the syncytiotrophoblast in response to swelling. This was achieved by measuring the response of the microvillous membrane potential (Em) to a hyposmotic stimulus in isolated intact placental villi and examining the effect of ion channel blockers. The studies constitute the first step toward characterizing the role of ion conductances in volume regulation by this unique human syncytial epithelium. Preliminary findings were published in abstract form (5).


    METHODS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Tissue Collection

Experiments were performed on villi from human placentas at term (weeks 38-41, as determined from date of last menstrual period, usually confirmed by ultrasound scan) collected from uncomplicated pregnancies delivered vaginally or by cesarean section at St. Mary's Hospital. Samples (~1 cm3) of villous tissue were collected in HEPES-Earle's solution (in mM; 116 NaCl, 5.4 KCl, 1.8 CaCl2, 0.4 MgSO4, 1.0 NaH2PO4, 5.5 glucose, 5.0 HEPES, pH 7.4 with NaOH) at ambient temperature and washed thoroughly. The tissue was then transferred to HCO-3-Earle's solution (in mM; 116 NaCl, 5.4 KCl, 1.8 CaCl2, 0.4 MgSO4, 1.0 NaH2PO4, 5.5 glucose, 26 NaHCO3; 280 mosmol/kgH2O), gassed with 95% O2-5% CO2 (to pH 7.4), and maintained at room temperature.

Measurement of Em

Em was measured in villi isolated from term placentas via a previously described method (6, 14). Individual mature intermediate villi (22) were removed, placed in a thermostatically regulated heated tissue perfusion chamber (Intracel, Royston, UK), and immobilized with glass suction pipettes in such a way as to isolate the villous core from the bath at the cut end of the villus. The villi were continuously superfused (1.5 ml/min) with HCO-3-Earle's solution (control solution) at 37°C and gassed with 95% O2-5% CO2. The perfusion chamber had microenvironmental control, which allowed a stream of gas (95% O2-5% CO2) to pass across the surface of solution in the perfusion chamber, maintaining a pH of 7.4. The perfusion chamber was placed on the stage of an inverted microscope (Nikon Diaphot), and the electrical measurements were made using an AxoClamp 2B amplifier (Axon Instruments, Foster City, CA). After being mounted, the villus was allowed to equilibrate with the control solution for a minimum of 10 min.

Em was then measured between a recording microelectrode (A) tapped into the outermost layer of the tissue (syncytiotrophoblast) and a similar electrode (B) placed in the bathing fluid. Both electrodes were pulled with a horizontal puller (Brown and Flaming model P-87; Sutter Instruments, Novato, CA) from 1.2-mm (outer diameter) borosilicate glass containing a filament (Clark Electromedical Instruments, Reading, UK). These electrodes had resistances of 80-100 MOmega when filled with 1.5 M KCl. A and B were in circuit with an Ag:AgCl reference pellet (R; ground) positioned directly in the bath fluid. Em was recorded as
<IT>E</IT><SUB>m</SUB> = (A − R) − (B − R)
With both the bath and recording electrodes immersed in control solution, the baseline potential difference between bath and recording electrodes and ground was set at 0 mV. An impalement was taken to be successful if the following criteria were met: 1) a rapid voltage deflection from baseline occurred on impalement, 2) a stable Em at a value ± 2 mV of the initial deflection was maintained for >1 min, and 3) Em returned to 0 ± 2 mV on withdrawal of the electrode from the tissue.

Effect of Hyposmotic and Isosmotic Solutions on Em

Effect of hyposmotic solution on Em. Em was measured after villi were exposed to solutions made hyposmotic by removal of NaCl from the control solution. Two hyposmotic challenges were used: a 138-hyposmotic solution (138 mosmol/kgH2O; 37 mM NaCl; concentrations of other solutes as for control solution) and a 170-hyposmotic solution (170 mosmol/kgH2O; 55 mM NaCl). Osmolalities were measured by freezing point depression (Roebling MOD 100; Camlab, Cambridge, UK).

After equilibration in control solution, each villus was impaled with a recording microelectrode (as described in Measurement of Em). If a stable impalement was achieved (meeting criteria 1 and 2), a control Em was recorded for a minimum of 2 min. Then, with the electrode still positioned in the tissue, the inflow to the bath was exchanged for either 138-hyposmotic or 170-hyposmotic solution. Em was measured during a 13-min exposure to hyposmotic challenge, after which the bath fluid was changed to control solution, and Em was recorded during a 5-min (minimum) recovery period. The electrode was then removed from the tissue, and the impalement was considered acceptable if the potential difference returned to 0 ± 2 mV. In this way each villus acted as its own control.

Effect of isosmotic solution on Em. In the experiments described above, the solutions were made hyposmotic by removal of NaCl. To determine whether the response observed with hyposmotic challenge was a result of the reduction in osmolality of the solution or the reduction in NaCl concentration or ionic strength, the protocol described in Effect of hyposmotic solution on Em was repeated with low-NaCl (i.e., 138-hyposmotic and 170-hyposmotic) solutions made isosmotic to the control solution (i.e., 280 mosmol/kgH2O) by addition of either mannitol or raffinose.

Effect of Inhibitors on Em Response to Hyposmotic Solutions and on Resting Em

Cell swelling and subsequent volume recovery during exposure to low-NaCl hyposmotic solution will be accompanied by dynamic and unpredictable changes in intracellular ion content. The concurrent change in Em will thus reflect both activation of membrane ion conductances and changes in intracellular ion activities. The role of K+ and Cl- conductances in the hyperpolarization of syncytiotrophoblast Em in response to hyposmotic challenge was investigated by measuring Em in hyposmotic or control solution in the presence of the K+ channel blocker barium chloride (Ba2+) or the anion transport inhibitor DIDS. Ba2+ forms an insoluble product in the presence of sulfate; therefore, in these inhibitor experiments 0.4 mM MgSO4 was replaced in control and hyposmotic solutions with 0.4 mM MgCl2.

As before, the isolated villus was equilibrated by superfusing with control solution, a stable impalement was achieved (meeting criteria 1 and 2), and the Em was recorded. Then, with the electrode still positioned in the tissue, the inflow to the bath was exchanged for either 170-hyposmotic solution containing 5 mM Ba2+ or 1 mM DIDS or control solution containing 5 mM Ba2+ or 1 mM DIDS. Em was measured during a 10-min exposure to solutions containing Ba2+ and during a 14-min application of solutions containing DIDS. The electrode was then removed from the tissue, and the impalement was considered acceptable if the potential difference returned to 0 ± 2 mV. In this way each villus again acted as its own control.

Chemicals

All reagents were analytic grade from standard suppliers. Ba2+ was purchased from Sigma (Poole, UK), and DIDS was purchased from Calbiochem-Novabiochem (Beeston, UK).

Statistics

The effects of hyposmotic challenge, isosmotic solution, Ba2+, and DIDS (under control and hyposmotic conditions) on MVM Em were assessed statistically with a repeated-measures ANOVA followed by a Bonferroni multiple comparisons test.

A two-way ANOVA was used to determine whether the change in Em observed in 138-hyposmotic and equivalent isosmotic solutions differed significantly from the change in Em observed with 170-hyposmotic and equivalent isosmotic solutions. Any significant differences identified by this analysis were examined further with a Mann-Whitney test (nonparametric statistics were used for this comparison because the 138-hyposmotic and equivalent isosmotic data did not follow a normal distribution; Bartlett's test for homogeneity).

The maximum change in Em measured in 138-hyposmotic and equivalent isosmotic solutions (containing mannitol or raffinose) was compared statistically using a Kruskal-Wallis nonparametric ANOVA followed by a Mann-Whitney test.

An ANOVA followed by a Bonferroni multiple comparisons test was used to compare 1) the maximum change in Em measured in 170-hyposmotic and equivalent isosmotic solutions (containing mannitol or raffinose) and 2) the change in Em measured in 170-hyposmotic and control solutions containing either Ba2+ or DIDS.


    RESULTS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Effect of Hyposmotic and Isosmotic Solutions on Em

Effect of hyposmotic solutions on Em. The effects of 138-hyposmotic and 170-hyposmotic solutions on isolated placental villus Em are shown in Figs. 1A and 2A, respectively; an example trace from an individual experiment is shown together with the mean data. Exposure to both 138-hyposmotic and 170-hyposmotic solutions induced a significant hyperpolarization of Em, which was reversible on removal of the hyposmotic stimulus (P < 0.01 and P < 0.001 vs. control recovery for 138-hyposmotic and 170-hyposmotic solutions, respectively; repeated-measures ANOVA plus Bonferroni). Despite the difference in the degree of osmotic challenge, the mean change in Em was similar with both 138-hyposmotic and 170-hyposmotic solutions (Fig. 3).


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Fig. 1.   Membrane potential (Em) response to 138-hyposmotic solution (A), 138-isosmotic (mannitol) solution (B), and 138-isosmotic (raffinose) solution (C). Example recordings of Em from individual experiments are shown at left. Duration of exposure to hyposmotic or isosmotic solution is indicated by horizontal bar for each trace. Bar graphs show control Em, maximum Em measured in hyposmotic or isosmotic solution, and Em at end of recovery period, respectively (means ± SE; n = 10 villi from 8 placentas, 9 villi from 5 placentas, and 6 villi from 3 placentas in A, B, and C, respectively). ** P < 0.01 vs. control; ## P < 0.01 vs. recovery; ### P < 0.001 vs. recovery (repeated-measures ANOVA plus Bonferroni multiple comparisons test).



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Fig. 2.   Em response to 170-hyposmotic solution (A), 170-isosmotic (mannitol) solution (B), and 170-isosmotic (raffinose) solution (C). Example recordings of Em from individual experiments are shown at left. Duration of exposure to hyposmotic or isosmotic solution is indicated by horizontal bar for each trace. Bar graphs show control Em, maximum Em measured in hyposmotic or isosmotic solution, and Em at end of recovery period, respectively (means ± SE; n = 10 villi from 9 placentas, 9 villi from 5 placentas, and 7 villi from 3 placentas in A, B, and C, respectively). *** P < 0.001 vs. control; ### P < 0.001 vs. recovery (repeated-measures ANOVA plus Bonferroni multiple comparisons test).



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Fig. 3.   Maximum change in Em observed during exposure to hyposmotic, isosmotic (mannitol), and isosmotic (raffinose) solutions. Values are means ± SE; n = 10 villi from 8 placentas for 138-hyposmotic solution, 10 villi from 9 placentas for 170-hyposmotic solution, 9 villi from 5 placentas for 138-isosmotic (mannitol) solution, 9 villi from 5 placentas for 170-isosmotic (mannitol) solution, 6 villi from 3 placentas for 138-isosmotic (raffinose) solution, and 7 villi from 3 placentas for 170-isosmotic (raffinose) solution. * P < 0.05 vs. 170-hyposmotic; *** P < 0.001 vs. 170-hyposmotic; dagger  P < 0.01 vs. 170-isosmotic (mannitol) (ANOVA plus Bonferroni multiple comparisons test). Data for 138-hyposmotic and 138-isosmotic solutions were analyzed with Kruskal-Wallis nonparametric ANOVA.

Effect of isosmotic solution on Em. In the hyposmotic experiments described in Effect of hyposmotic solutions on Em, the osmolality of the solutions was reduced by removal of NaCl. The hyperpolarization of Em during exposure to these hyposmotic solutions may therefore be caused by the reduction in osmolality or the reduction in NaCl concentration or ionic strength of the solutions. To distinguish between these possibilities, the villi were exposed to solutions with low NaCl concentration (i.e., 138-hyposmotic or 170-hyposmotic solutions), whose osmolality was increased to 280 mosmol/kgH2O (isosmotic with control solution) by addition of mannitol or raffinose.

The effects of 138-hyposmotic and 170-hyposmotic solutions made isosmotic by the addition of mannitol [hereafter termed 138-isosmotic (mannitol) and 170-isosmotic (mannitol)] on placental villus Em are shown in Figs. 1B and 2B, respectively. An example trace from an individual experiment is shown together with the mean data. Application of either 138-isosmotic (mannitol) or 170-isosmotic (mannitol) solution induced a significant hyperpolarization of Em, which was reversible on removal of the isosmotic (mannitol) solution [P < 0.01 vs. control, P < 0.001 vs. recovery for 138-isosmotic (mannitol), and P < 0.001 vs. control and recovery for 170-isosmotic (mannitol); repeated-measures ANOVA plus Bonferroni]. The degree of hyperpolarization induced by 138-isosmotic (mannitol) solution did not differ significantly from that observed during exposure to 170-isosmotic (mannitol) solution. Both 138-isosmotic (mannitol) and 138-hyposmotic solutions caused a similar change in Em. However, the hyperpolarization of Em observed during application of 170-isosmotic (mannitol) solution was smaller than that initiated during 170-hyposmotic challenge (Fig. 3).

The Em responses to 138-hyposmotic and 170-hyposmotic solutions made isosmotic by the addition of raffinose [hereafter termed 138-isosmotic (raffinose) and 170-isosmotic (raffinose)] are shown in Figs. 1C and 2C, respectively. Again, an example trace from an individual experiment is shown together with the mean data. Neither 138-isosmotic (raffinose) nor 170-isosmotic (raffinose) solution had any significant effect on Em (repeated-measures ANOVA plus Bonferroni). The change in Em observed with 170-isosmotic (raffinose) solution was significantly smaller than that induced by both 170-hyposmotic solution (P < 0.001; ANOVA plus Bonferroni) and 170-isosmotic (mannitol) solution (P < 0.01; ANOVA plus Bonferroni). The change in Em in 138-isosmotic (raffinose) solution was not significantly different at the 5% level (Kruskal-Wallis nonparametric ANOVA) from that observed with 138-hyposmotic and 138-isosmotic (mannitol) solutions.

Effect of Inhibitors on Resting Em and Em Response to Hyposmotic Solutions

Effect of Ba2+. The Em responses to 170-hyposmotic solution containing 5 mM Ba2+ and control solution containing 5 mM Ba2+ are shown in Fig. 4, B and C, respectively. The Em response to 170-hyposmotic solution previously presented in Fig. 2A is shown again in Fig. 4A to allow direct comparison of the data. Ba2+ applied in control solution induced a depolarization of resting Em (P < 0.001 at 4 and 10 min vs. control; repeated-measures ANOVA plus Bonferroni). The maximum depolarization induced in the presence of Ba2+ was similar when the inhibitor was applied in either 170-hyposmotic or control solution (Fig. 6). The hyperpolarization of Em observed previously (Fig. 4A) during exposure to hyposmotic challenge did not occur in the presence of Ba2+ (P < 0.001, 170-hyposmotic Ba2+ vs. 170-hyposmotic; ANOVA plus Bonferroni; Fig. 6). Indeed, exposure to 170-hyposmotic solution in the presence of Ba2+ significantly depolarized Em (P < 0.01 at 4 min and P < 0.001 at 10 min vs. control; repeated-measures ANOVA plus Bonferroni; Fig. 4B).


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Fig. 4.   Em response to 170-hyposmotic solution (A), 170-hyposmotic solution containing 5 mM Ba2+ (B), and control solution containing 5 mM Ba2+ (C). Em response to 170-hyposmotic solution previously presented in Fig. 2A is shown again here (A) to allow direct comparison of data. Example recordings from individual experiments are shown at left. Duration of exposure to experimental solution is indicated by horizontal bar for each trace. Data are means ± SE; n = 10 villi from 8 placentas, 6 villi from 3 placentas, and 5 villi from 4 placentas in A, B, and C, respectively. A: control Em, maximum Em measured in hyposmotic solution, and Em after a 5-min recovery period (*** P < 0.001 vs. control; ### P < 0.001 vs. recovery; repeated-measures ANOVA plus Bonferroni multiple comparisons test). B and C: control Em and Em after 4- and 10-min exposure to hyposmotic or control solution containing 5 mM Ba2+ (** P < 0.01 vs. control; *** P < 0.001 vs. control; dagger  P < 0.01 vs. 4 min; repeated-measures ANOVA plus Bonferroni multiple comparisons test).

Effect of DIDS. The Em responses to 170-hyposmotic solution containing 1 mM DIDS and control solution containing 1 mM DIDS are shown in Fig. 5, B and C, respectively. The Em response to 170-hyposmotic solution previously presented in Fig. 2A is shown again in Fig. 5A to allow direct comparison of the data. Exposure to both control solution containing DIDS and 170-hyposmotic solution containing DIDS significantly hyperpolarized Em (P < 0.001 at 4 and 10 min vs. control and P < 0.001 vs. control, respectively; repeated-measures ANOVA plus Bonferroni). The hyperpolarization of Em usually observed with 170-hyposmotic solution alone was potentiated when this hyposmotic solution was applied in the presence of DIDS (Fig. 6). The degree of hyperpolarization observed during exposure to control solution containing DIDS or to 170-hyposmotic solution containing DIDS did not differ significantly (Fig. 6). In these experiments DIDS was initially dissolved in DMSO. This vehicle alone (at concentration used in DIDS-containing solution) has no significant effect on placental villus Em (control Em -18.9 ± 1.0 mV, after 10-min exposure to DMSO -18.3 ± 1.0 mV; n = 6, repeated-measures ANOVA plus Bonferroni).


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Fig. 5.   Em response to 170-hyposmotic solution (A), 170-hyposmotic solution containing 1 mM DIDS (B), and control solution containing 1 mM DIDS (C). Em response to 170-hyposmotic solution previously presented in Fig. 2A is shown again here (A) to allow direct comparison of data. Example recordings from individual experiments are shown at left. Duration of exposure to experimental solution is indicated by horizontal bar for each trace. Data are means ± SE; n = 10 villi from 8 placentas, 5 villi from 3 placentas, and 6 villi from 3 placentas in A, B, and C, respectively. A: control Em, maximum Em measured during hyposmotic challenge, and Em after 5-min recovery period (*** P < 0.001 vs. control, ### P < 0.001 vs. recovery; repeated-measures ANOVA plus Bonferroni multiple comparisons test). B and C: control Em and Em after 4- and 10-min exposure to hyposmotic or control solution containing 1 mM DIDS (*** P < 0.001 vs. control; dagger  P < 0.01 vs. 4 min; dagger dagger P < 0.001 vs. 4 min; repeated-measures ANOVA plus Bonferroni multiple comparisons test).



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Fig. 6.   Maximum change in Em observed during exposure to 170-hyposmotic solution (n = 10 villi from 8 placentas) and after 10-min exposure to 170-hyposmotic solution containing Ba2+ (n = 6 villi from 3 placentas), control solution containing Ba2+ (n = 5 villi from 4 placentas), 170-hyposmotic solution containing DIDS (n = 5 villi from 3 placentas), and control solution containing DIDS (n = 6 villi from 3 placentas). Data are means ± SE. ** P < 0.01 vs. 170-hyposmotic; *** P < 0.001 vs. 170-hyposmotic (ANOVA plus Bonferroni multiple comparisons test).


    DISCUSSION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Effect of Hyposmotic and Isosmotic Solutions on Em

Exposure of placental villi to 138-hyposmotic or 170-hyposmotic solutions induced a sustained hyperpolarization of Em, which was reversible on removal of the hyposmotic stimulus. These data suggest that ion conductances are activated in the MVM of the syncytiotrophoblast during hyposmotic challenge. The observation that Em hyperpolarized when villi were bathed in hyposmotic solution suggests that there is a net loss of positive ions from the syncytiotrophoblast in response to this stimulus.

In these experiments the solutions were made hyposmotic by removal of NaCl. The hyperpolarization of Em observed during exposure to these hyposmotic solutions might therefore be caused by the reduction in NaCl concentration or ionic strength per se, rather than the reduction in osmolality of the solution. To distinguish between these two possibilities, the villi were exposed to solutions with low NaCl concentration (i.e., 138-hyposmotic or 170-hyposmotic solutions) made isosmotic to control solution by addition of mannitol or raffinose. Solutions made isosmotic by the addition of mannitol induced a significant hyperpolarization of Em; however, those made isosmotic with raffinose had no effect on Em.

The ionic composition of the 138-isosmotic (mannitol) and 138-isosmotic (raffinose) solutions were identical, as were the compositions of the 170-isosmotic (mannitol) and 170-isosmotic (raffinose) solutions. Therefore, the differing Em responses observed with isosmotic (mannitol) and isosmotic (raffinose) solutions cannot have occurred as a consequence of the reduction in NaCl concentration. The probable explanation for the different Em responses to isosmotic (mannitol) and isosmotic (raffinose) solutions is differential permeability of the syncytiotrophoblast MVM to the two saccharides. Jansson et al. (21) found that the MVM of the syncytiotrophoblast is more permeable to the monosaccharide mannitol than to the trisaccharide raffinose, whose molecular weight and molecular radius are substantially greater. It is likely that, in our experiments, mannitol enters the syncytiotrophoblast across the MVM down its concentration gradient, inducing intracellular hypertonicity, which in turn causes cell swelling and activation of volume regulatory mechanisms resulting in hyperpolarization of Em. The lack of effect of isosmotic (raffinose) solutions on Em supports the theory that hyperpolarization during exposure to hyposmotic solutions was a response to the reduction in osmolality per se, not specifically to a reduction in NaCl concentration.

Previous observations in other tissues suggest that the magnitude of ion loss during RVD increases with decreasing extracellular fluid osmolality. For example, the magnitude of the whole cell chloride conductance increases in several cell types as extracellular osmolality is decreased (1, 2, 25). However, because the degree of hyperpolarization induced in isolated placental villi in response to 138-hyposmotic and 170-hyposmotic solutions is similar, there does not appear to be a differential loss of positive or negative ions from the syncytiotrophoblast as the hyposmotic challenge increases. In this context it is interesting that 86Rb (K+) efflux from villous fragments in response to hyposmotic challenge is increased as solution osmolality is decreased from 170 mosmol/kgH2O to 138 mosmol/kgH2O (S. L. Greenwood and C. P. Sibley, unpublished observations). Thus it is probable that, although quantitatively more K+ and Cl- ions might be lost from the syncytiotrophoblast on exposure to 138-hyposmotic than would be lost on exposure to 170-hyposmotic solution, the relative loss of ions is the same with both solutions.

Although the response of Em to a hyposmotic stimulus has been measured in several types of cell in culture [e.g., liver (12, 13), rabbit proximal tubule (11), human colonic carcinoma (3), and Madin Darby canine kidney (26, 29)], there are fewer observations in intact tissues. A sustained hyperpolarization, similar to that measured here in placental villi, has also been observed in liver slices (12, 13) and in Necturus small intestine and gallbladder (30, 36). In the latter studies the changes in Em with hyposmotic swelling were measured at the basolateral (contraluminal) membrane, suggesting that ions are lost from the cell cytoplasm to plasma during RVD. It is interesting to note that the hyperpolarization in response to the 138-hyposmotic and 170-hyposmotic solutions is slower in onset than is the time for recovery of Em on reintroducing the control solution. We have not investigated the mechanism of the repolarization, but it is similar to the time course of the response reported in liver (12). One explanation is that K+ (and Cl-) conductances are inactivated more rapidly in response to shrinking than they are activated during swelling.

Effect of Inhibitors on Response to Hyposmotic Challenge and on Resting Em

In epithelial cells the most common mechanism effecting RVD is the loss of K+ and Cl- from the cytoplasm by the activation of K+ and Cl- channels (18). Preliminary evidence suggests that K+ and Cl- channels are also activated in placenta in response to swelling. In multinucleated cytotrophoblast cells, RVD in response to a hyposmotic stimulus is associated with an increase in 86Rb efflux, and both volume recovery and 86Rb loss are inhibited by the K+ channel blocker Ba2+ (15, 17). Hyposmotic swelling induces 86Rb efflux and 125I efflux from placental villous fragments, and the latter is sensitive to the anion transport inhibitor niflumic acid (8, 31). These data suggest K+ and Cl- channel involvement in RVD by the placenta, although the studies cannot discriminate between the microvillous and basal membrane of the syncytiotrophoblast as the site of channel activation. Therefore, we investigated the presence of volume-sensitive K+ and Cl- conductances in the MVM of the intact syncytiotrophoblast by evaluating the Em response to a hyposmotic solution in the presence of Ba2+ and DIDS.

Effect of Ba2+. The hyperpolarization of Em usually observed in isolated placental villi in response to 170-hyposmotic solution did not occur in the presence of Ba2+; in fact, the Em depolarized to a value significantly less negative than the resting Em. The observation that Em depolarized during application of hyposmotic solution containing Ba2+ suggests that Ba2+ inhibits both a volume-activated K+ conductance and a K+ conductance that normally contributes to the resting Em. Indeed, application of Ba2+ in control solution resulted in a sustained depolarization of Em, confirming that a Ba2+-sensitive K+ conductance normally contributes to the resting Em of the syncytiotrophoblast. Thus in 170-hyposmotic solution, Ba2+ appears to inhibit both a volume-activated and a basal K+ conductance.

Ba2+-sensitive K+ conductance or 86Rb efflux has been shown to play an important role in volume regulation during hyposmotic challenge in a number of cells and tissues (e.g., Refs. 10, 12, 13, 23, 30). Ba2+ also inhibits volume-activated 86Rb loss and RVD in cytotrophoblast cells, which are the cytological precursors of the syncytiotrophoblast (15, 17). The observation in this study that Ba2+-sensitive conductances are activated in the MVM of the intact syncytiotrophoblast in response to hyposmotic solutions is consistent with the hypothesis that the syncytiotrophoblast achieves volume regulation, at least in part, by extrusion of K+ from the cytosol over the MVM into maternal blood.

Effect of DIDS. The hyperpolarization of Em observed in response to 170-hyposmotic solution was potentiated in the presence of DIDS. These data suggest that a DIDS-sensitive Cl- conductance is activated in the syncytiotrophoblast MVM in response to hyposmotic challenge. When applied in control solutions, DIDS also hyperpolarized Em, indicating that a DIDS-sensitive Cl- conductance normally contributes to the resting Em of the syncytiotrophoblast. When applied in 170-hyposmotic solution, DIDS thus appears to inhibit both a volume-activated and a basal Cl- conductance.

DIDS-sensitive Cl- currents and 125I/36Cl efflux contribute to hyposmotically induced RVD in many cell types (see Ref. 25). In keeping with these observations, DIDS has been shown to inhibit volume-activated 125I loss and volume-activated whole cell chloride currents in cytotrophoblast cells (7, 37). Thus the activation of DIDS-sensitive conductances in the MVM of the intact syncytiotrophoblast in response to hyposmotic solutions that was observed in this study suggests that the syncytiotrophoblast loses Cl- from the cytosol over the MVM to maternal blood to effect RVD.

In conclusion, the data from the present study imply that both K+ and Cl- are lost from the syncytiotrophoblast across the MVM to the maternal circulation during (or as part of) a volume-regulatory response to hyposmotic challenge, via Ba2+ and DIDS-sensitive conductances, respectively. At present we are unable to assess volume-regulatory changes in the syncytiotrophoblast of the intact villus. However, multinucleated cytotrophoblast cells isolated from term placenta and maintained in culture exhibited Ba2+-sensitive volume-regulatory decreases over 15-30 min in response to 138 mosmol/kgH2O solution (17). These data support our hypothesis that ion channel activation forms part of the volume-regulatory response to hyposmotic challenge in placental trophoblast. Our experiments also demonstrate that a Ba2+-sensitive K+ conductance and a DIDS-sensitive Cl- conductance contribute to maintaining the resting Em of the syncytiotrophoblast; this has not previously been shown.

The lack of specific channel inhibitors complicates identification of the channels involved in volume-activated and resting membrane conductances. For example, DIDS, at the concentration used in this study, not only inhibits Cl- channels but also other anion transport processes, e.g., HCO-3/Cl- exchange; inhibition of this exchange will affect intracellular pH, which might have secondary effects on K+ and Cl- channels and Em. Direct study of the K+ and Cl- channels using the patch clamp technique is therefore likely to be the most productive approach in future studies to reveal the single-channel basis for both the volume-activated and basal Ba2+ and DIDS-sensitive conductances.

Perspectives

Em is an important driving force for transport of solutes across the syncytiotrophoblast and thus for maternofetal exchange. However, measurement of Em in intact villi is technically very challenging (6), and to date there have been only four reports of placental villus Em in the literature (4, 6, 9, 14), none of which has addressed the contribution of Ba2+-sensitive K+ conductances and DIDS-sensitive Cl- conductances to the resting Em of the syncytiotrophoblast.

In this study we also show a hyperpolarization of the syncytiotrophoblast Em in isolated placental villi exposed to hyposmotic solutions, apparently caused by a differential loss of K+ vs. Cl- over the MVM. Hyposmotic challenge is used as a reproducible means of altering cell volume and has been used in this way in many studies in both placenta and other cell types (17, 18). The physiological equivalent to this experimental manipulation is likely to be accumulation of intracellular solute resulting in intracellular hypertonicity, water influx, and cell swelling (19). Indeed, exposure to hyposmotic solution or amino acids has been shown to induce similar volume-regulatory responses in cytotrophoblast cells (27, 28).

Clearly, understanding the interaction between solute transport and changes in electrical driving force will be important for a complete understanding of the mechanisms of maternofetal exchange.


    ACKNOWLEDGEMENTS

We thank the staff at St. Mary's Hospital for assistance in obtaining placentas.


    FOOTNOTES

This study was supported by The Wellcome Trust Grant 04023/2/95/Z/MP.

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. §1734 solely to indicate this fact.

Address for reprint requests and other correspondence: T. J. Birdsey, Dept. of Obstetrics and Gynaecolgy, Univ. of Sheffield, Northern General Hospital, Herries Road, Sheffield, S5 7AU United Kingdom (E-mail: t.j.birdsey{at}sheffield.ac.uk).

Received 1 July 1998; accepted in final form 18 January 1999.


    REFERENCES
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
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Am J Physiol Regul Integr Compar Physiol 276(5):R1479-R1488
0002-9513/99 $5.00 Copyright © 1999 the American Physiological Society



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