A dynamic model of saliva secretion
Introduction
Saliva production is an important process for both digestion and oral health. Problems with salivation can cause issues with dental cavities, oral pain and infections. In mastication, an adequate supply of saliva is needed to provide lubrication to the mouth and facilitate swallowing. Humans and most mammals possess three major pairs of salivary glands (parotid, sublingual and submandibular). The parotid gland is the largest of these, and is also the only major salivary gland that produces purely serous fluid, with the other glands producing mucous. The structure of the parotid gland consists of bunches of acini connected by ducts. Each acinus comprises several epithelial parotid acinar cells secreting fluid into a shared lumenal cavity. The salivary fluid passes from the lumen of the acini into a branching network of ducts, where it is collected and travels to the mouth. Dysregulation of fluid secretion from the parotid acinar cells can lead to conditions such as xerostomia (dry mouth), where sufferers experience pain with eating and speech because of a lack of saliva.
Fluid is known to travel through the parotid cells by the process of osmosis. Given a membrane impermeable to ions but permeable to water, water will flow from the area of low ionic concentration to that of high concentration. The parotid gland must maintain an ionic gradient, increasing from the interstitium, to the cytoplasm and then into the lumen, to facilitate water movement through the cell to the duct. Whilst maintaining this gradient the acinar cells must avoid accumulation of too much water in the cell, as the cell membrane is incapable of sustaining any significant pressure difference.
Existing models for fluid flow through the parotid acinar cell place K+ channels exclusively in the basolateral membrane (Gin et al., 2007, Nauntofte, 1992, Turner et al., 1993, Turner and Sugiya, 2002). However, there is building evidence for the existence of K+ channels in the apical membrane (Sørensen et al., 2001 find apical K+ channels in frog skin glands, Catalan and Melvin [Unpublished] in parotid acinar). Cook and Young (1989) looked at adding apical K+ channels to a model with constant ionic concentrations and steady state currents. We aim to investigate how the distribution of K+ channels changes the saliva production of the parotid acinar cell in a dynamic model where salivation is initiated by Ca2+ signalling.
We use the currently accepted model for saliva production (see Nauntofte, 1992 for a review) where the movement of Cl− into the cytoplasm and then into the lumen creates a concentration gradient which water follows by osmosis. In this model the basolateral membrane contains a Na+–K+–2Cl− cotransporter (NKCC), a Na+–K+–ATPase (NaK) and a K+ ion channel. Cl− moves into the cell via the NKCC and then moves through Ca2+ sensitive apical Cl− channels into the lumen. The Na+ and K+ ions are removed from the cell by K+ channels and the NaK pump. See Fig. 1 for a diagram of the model used.
Calcium (Ca2+) plays a critical role in epithelial tissue as a second messenger activating fluid flow. Previous models have investigated Ca2+ signalling in a variety of epithelial tissues including airway epithelium (Sneyd et al., 1995, Warren et al., 2009, Warren et al., 2010). As Ca2+ concentration increases in parotid cells the ionic channels at the basal and apical membrane open and fluid production is seen to increase. The salivation process is initiated in the otic ganglion parasympathetic nerve which runs from the brain to the parotid gland. When stimulated, for example when we smell food, these nerves release acetylcholine, which binds to receptors on the cell surface, leading to the production of inositol (1,4,5)-trisphosphate (IP3) in the cytoplasm. The raised IP3 concentration releases Ca2+ from internal stores in the endoplasmic reticulum (ER). As Ca2+ concentration increases in parotid cells the ionic channels at the basal and apical membrane open and fluid production is seen to increase. We create a model for intracellular Ca2+ using recent results relating to the release of Ca2+ from internal stores via the inositol (1,4,5)-trisphosphate receptor (IP3R) and the dynamics of IP3. Feedback of Ca2+ on the degradation of IP3 is the mechanism which our model uses to recreate Ca2+ oscillations.
Insight into the role of the K+ channel distribution in determining the rate of water transport in the parotid cell is gained by observing the apical and basolateral membrane potentials during simulations with and without the addition of apical K+ channels.
Section snippets
Model assumptions and notation
We introduce a subscript notation for ionic concentrations, with [x]i, [x]l, [x]e, [x]er denoting, respectively, cytosolic, luminal, interstitial and ER concentrations of an ion x. We assume the ionic concentrations in the interstitium stay constant, while the concentrations in the cytoplasm and lumen change as a result of the ion movements seen in Fig. 1. Stepwise increases in total ionic concentrations from the interstitium to the cytoplasm and then to the lumen result in fluid flow by
Calcium model results
We aim to reproduce experimental traces found by Bruce et al. (2002) using the unconstrained Ca2+ flux density parameters, kIPR, kRyR, VSERCA, and the constant IP3 dephosphorylation rate k5p to fit the model to the data. In simulating the experimental procedures we hold the cell volume constant, this demonstrates that the model Ca2+ oscillations are not dependent on cell volume oscillations.
In experimental recreation of the salivation process carbachol (CCh) is added to the parotid cells. CCh
Discussion
The model we have developed here with intracellular Ca2+ oscillations driving secretion via secondary chloride transport we have shown to be consistent with a range of experimental data and extends previous parotid acinar cell models by Gin et al. (2007) and Cook and Young (1989). Ca2+ oscillations that previously depended on volume oscillations (Gin et al., 2007) or were altogether absent (Cook and Young, 1989) are now based on physiological models of the IPR and IP3 dynamics. Independent
Acknowledgments
Thanks to Kate Patterson, Ivo Siekmann, Oliver Maclaren at the University of Auckland and Ted Begenisich and James Melvin at the University of Rochester for their comments on an earlier version of this manuscript. We also thank Bill Holmes at Indiana University for his help with simplifying the NaK. This work was supported by National Institutes of Health (NIH) Grant R01-DE19245.
References (38)
- et al.
Phosphorylation of inositol 1,4,5-trisphosphate receptors in parotid acinar cells. a mechanism for the synergistic effects of cAMP on Ca2+ signaling
Journal of Biological Chemistry
(2002) - et al.
Severe impairment of salivation in Na+/K+/2Cl-cotransporter (NKCC1)-deficient mice
Journal of Biological Chemistry
(2000) - et al.
A mathematical model of fluid secretion from a parotid acinar cell
Journal of Theoretical Biology
(2007) - et al.
A kinetic model of the inositol trisphosphate receptor based on single-channel data
Biophysical Journal
(2009) - et al.
Ryanodine receptor adaptation and Ca2+(-)induced Ca2+ release-dependent Ca2+ oscillations
Biophysical Journal
(1996) - et al.
Dopamine-induced epithelial K+ and Na+ movements in the salivary ducts of periplaneta americana
Journal of Insect Physiology
(2001) - et al.
Functional comparisons between isoforms of the sarcoplasmic or endoplasmic reticulum family of calcium pumps
Journal of Biological Chemistry
(1992) - et al.
Defective Secretion of Saliva in Transgenic Mice Lacking Aquaporin-5 Water Channels
Journal of Biological Chemistry
(1999) - et al.
Models of IP3 and Ca2+ oscillations: frequency encoding and identification of underlying feedbacks
Biophysical Journal
(2006) - et al.
Metabolism of inositol 1,4,5-trisphosphate and inositol 1,3,4,5-tetrakisphosphate by the oocytes of xenopus laevis
Journal of Biological Chemistry
(1998)
Development of models of active ion transport for whole-cell modelling: cardiac sodium-potassium pump as a case study
Progress in Biophysics and Molecular Biology
A mathematical model of calcium-induced fluid secretion in airway epithelium
Journal of Theoretical Biology
Activation of calcium-dependent chloride channels in rat parotid acinar cells
The Journal of General Physiology
A quantitative description of the Na–K–2Cl cotransporter and its conformity to experimental data
AJP-Renal Physiology
Transepithelial potential changes during stimulation of isolated salivary glands with 5-hydroxytryptamine and cyclic Amp
Journal of Experimental Biology
Water permeability and pathways in the proximal tubule
The American Journal of Physiology
Calcium dependence of calcium extrusion and calcium uptake in mouse pancreatic acinar cells
The Journal of Physiology
Effect of K+ channels in the apical plasma membrane on epithelial secretion based on secondary active Cl-transport
Journal of Membrane Biology
Activation of salivary secretion: coupling of cell volume and [Ca2+]i in single cells
Science
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