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. 2022 Sep 6;12(9):1390. doi: 10.3390/life12091390

Figure 4.

Figure 4

Figure 4

Fluid movement in normal conditions (A) and abdominal hypertension (B). The physiological movement of fluid is determined by the imbalance between hydrostatic and colloid osmotic pressures. It is best described by the revised Starling equation: Jv = LpA[(PcPi) − σ(IIcIIi)], where Jv is net fluid filtration, Lp the capillary hydraulic permeability, A the capillary surface area (which is available for fluids and small molecule filtration), σ the capillary reflection coefficient, Pc the capillary hydrostatic pressure, Pi the interstitial hydrostatic pressure, IIc and IIi the capillary and interstitial colloid osmotic pressures, respectively. Generally, Pc dependent on the differences between the arteriole hydrostatic pressure (PA) and the venule hydrostatic pressure (PV). This difference strongly corresponds to the hydraulic resistances in arterioles and venule (RA and RV, respectively), which was described by the Pappenheimer Soto-Riviera Equation: Pc = (Pv [RA/RV] + PA)/(1 + [RA/RV]). According to this equation, every increase in PA or PV, as well as an increase in RA/RV (e.g., following intra-abdominal hypertension leading to venous congestion) or increase Pc. Under normal physiological conditions, the sub-glycocalyx colloid osmotic pressure strongly corresponds to interstitial pressure and its value ranges between 70% and 90% of the interstitial colloid pressure. Adapted from Levick et al. [133].