Summary
To explain how hydrostatic pressure differences between tubule lumen and interstitium modulate isotonic reabsorption rates, we developed a model of NaCl and water flow through paracellular pathways of the proximal tubule. Structural elements of the model are a tight junction membrane, an intercellular channel whose walls transport NaCl actively at a constant rate, and a basement membrane. Equations of change were derived for the channel, boundary conditions were formulated from irreversible thermodynamics, and a pressure-area relationship typical of thin-walled tubing was assumed. The boundary value problem was solved numerically. The principal conclusions are: 1) channel NaCl concentration must remain within a few mOsm of isotonic values for reabsorption rates to be modulated by transtubular pressure differences known to affect this system; 2) basement membrane and channel wall parameters determine reabsorbate tonicity; tight junction parameters affect the sensitivity of reabsorption to transmural pressure; 3) channel NaCl concentration varies inversely with transmural pressure difference; this concentration variation controls NaCl diffusion through the tight junction; 4) modulation of NaCl diffusion through the tight junction controls the rate of isotonic reabsorption; modulation of water flow can increase sensitivity to transmural pressure; 5) no pressure-induced change in permeability of the tight junction or basement membrane is needed for pressure to modulate reabsorption; and 6) system performance is indifferent to the distribution of active transport sites, to the numerical value of the compliance function, and to the relationship between lumen and cell pressures.
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Abbreviations
- A :
-
channel cross-section area, cm2
- A max :
-
maximum channel cross-section area, cm2
- α:
-
volume flow rate, dimensionless
- b :
-
NaCl concentration gradient, (mOsm cm−4)×10−3
- β:
-
NaCl concentration gradient, dimensionless
- C :
-
NaCl concentration, (mOsm cm−3)×10−3
- \(\overline C \) :
-
arithmetic mean NaCl concentration (mOsm cm−3)×10−3
- γ:
-
NaCl concentration, dimensionless
- D :
-
channel NaCl diffusion coefficient, cm2 sec−1
- E :
-
emergent osmolality, (mOsm cm−3)×10−3
- k 1 :
-
channel wall hydraulic permeability, dimensionless
- k 2 :
-
NaCl active transport rate, dimensionless
- k 3 :
-
basement membrane hydraulic permeability, dimensionless
- k 4 :
-
tight junction hydraulic permeability, dimensionless
- k 5 :
-
basement membrane NaCl permeability, dimensionless
- k 6 :
-
tight junction NaCl permeability, dimensionless
- k 7 :
-
NaCl reflection coefficient, tight junction, dimensionless
- k 8 :
-
NaCl reflection coefficient, basement membrane, dimensionless
- L :
-
hydraulic permeability, cm sec−1 mm Hg−1 or NaCl permeability, cm sec−1
- λ:
-
distance, dimensionless
- N :
-
NaCl active transport rate, mOsm cm−2 sec−1
- ζ:
-
compliance parameter, mm Hg−1
- p :
-
hydrostatic pressure, mm Hg
- \(\bar p\) :
-
cell hydrostatic pressure, mm Hg
- II :
-
osmotic pressure, mm Hg
- q :
-
volume flow rate, cm3 sec−1
- R :
-
universal gas constant, mm HgT −1 mol−1
- r :
-
A/A max, dimensionless
- S :
-
channel circumference, cm
- σ:
-
NaCl reflection coefficient
- T :
-
absolute temperature,oK
- Φ:
-
hydrostatic pressure, dimensionless
- X :
-
channel length, cm
- x :
-
distance, cm
- z :
-
pump distribution, dimensionless
- B :
-
basement membrane
- BS :
-
basement membrane, NaCl
- IS :
-
interstitial space
- L :
-
lumen
- o :
-
isotonic
- T :
-
tight junction
- TS :
-
tight junction, NaCl
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Huss, R.E., Marsh, D.J. A model of NaCl and water flow through paracellular pathways of renal proximal tubules. J. Membrain Biol. 23, 305–347 (1975). https://doi.org/10.1007/BF01870256
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DOI: https://doi.org/10.1007/BF01870256