Rheology of blood circulation . Basic physical laws of liquids Law of Pascal Liquid column causes a pressure (hydrostatic pressure) that is directly proportional to the height of the liquid column (h), density of the liquid (p) and gravitational acceleration (g). h ^height p ^density g = gravitational acceleration C^\33,322 Pa = 1 mm Hg^> 760 mmHg= 1 atm = 10.3 m H20 Effect of gravity on arterial and venous pressure CO Per each 10 cm Law of Laplace Relation between distending pressure (P [N/m2]) and tension in the wall of hollow object (T [N/m]) : For vessel: Considering thickness of vesse wall (h [m]): T=P-R/h [N/m2] and R2 are the biggest and the smallest radii of curvature For sphere: R1 = R2 Characteristics of vessels ( P.R h ^ y-' P.R/h vessel P [kPa] radius tension (N/m) wall thickness tension (N/m2) aorta 133 13 mm nebo mene 170 2 mm 85000 | arteries 12 5 mm 60 1 mm 60000 arterioles 8 150-62 |Lim 1.2-0.5 20 |Lim 40000 1 capillaries 4 4 |iim L6.10"2 1 (Lim 16000 venules 2.6 10 Kim 2,6.10"2 2 (Lim 13000 veins 2 200 |Lim a vice 0,4 0,5 mm 800 vena cava 1,33 16 mm 21 1,5 mm 14000 Continuity equation The volume of fluid flowing through a tube (vessel) per unit of time (Q [\/s]) is constant vessel aorta arterioles capilaries venules vena cava v - velocity S - area Average blood velocity in vessels ■ 5.6 l/min diameter - 2.6 cm 20-50 |wn 4-9 |um - 20 [am - 3 cm number 1 ~5x106 ~5x109 32x106 total area -5.3 cm2 ~ 60 cm2 2000 cm2 -100 cm2 ~ 14 cm2 1.5 cm/s ~ 0.04 cm/s ~ 1 cm/s 7 cm/s Relation between total cross-sectional area of vessels and mean flow velocity aorta arteries arterioles capilares venules veins v. cava Individual vessel diameter (cm) 2.6 + 0.8 9 0.3-0.06 0.002 0.0009 Number 1 Increasing 0.16-109 5-109 0.5-109 Decreasing 2 Joint cross-sectional area (cm2) 3500 ^^^ 2700 500/ _ 5.3 20 20 ^^100 30 10 Mean flow velocity Va (cm * s 1) 6 Implication at aortic aneurysm S^Vj = S2v2 a je-li Sf^S,, musi pl&tit: Vj>v, 2* R2 1 2 2 For P2>Pi Poiseuille - Hagen equation co 0 1 r <- -► The flow of liquid \n the cylindrical tube (Q) is directly proportional to the pressure difference between two ends of the tube (AP=PA-PB), to the fourth power of the tube radius (r) and inversely proportional to tube length (I) and to the viscosity of liquid (r|). Limitation: » For stationary flow in Newtonian fluids where viscosity is constant and independent on flow velocity. Vascular resistance (Rv):a consequence of the friction vessel wall. een fluid and Parallel arrangement of vessels Series arrangement of vessels Relation between vessel radius and peripheral resistance Total peripheral resistance (TPR) of vascular system 90 ml/s ,mean 3 mm Hg a,mean AP Pa-Pv Pa ~ Q ~ Q ~ Q ~ 90 93__mmHg s ml For constant Q: tTPR =^> t Pa =^> hypertension,.... 2. Rheological features of blood and vessels Blood viscosity Effect of hematocrit Effect of diameter in small vessels 8 _4—| 6 > 4—> !_ 4 >, -t—» "co C 2 > 1 0 Fahraes-Lindqvist efekt Blood I I Plasma Water cap. arterioles J-L J_L 5 10 50 100 500 1000 Vessel inside diameter Other factors causing increase of viscosity: • decrease of blood flow velocity • elevation of plasma proteins • In small arteries the velocity profile of the flowing blood has a parabolic shape. In the bigger arteries it has a piston shape. • The layer close to vessel wall is poor of erythrocytes. Pathological states causing turbulent flow: aneurisma, stenosis, arteriosclerosis, decreased blood viscosity, . Elasticity of vessels Pulse wave velocity (PWV) I- /v h *• PWV P Einc) - modulus of stiffness Moens-Korteweg (1878) In aorta PWV = 4 - 6 m/s Mechanisms of venous return od circulati plic .kap iláry lie. artérie Low-pressure system (reservoir function) pulmonary 100% circulation systemic circulation 15% 25% skin and other organs ■ / plic. vény 4 velké plieni vény Cardiac output in rest 5 - 6 l/min After load up to 20 l/min 15% (3%) 120/80 mm Hg (50%) aort artérie arterioly (4%) kapiláry 20% (3%) High-pressure system ^jJ (3^b) (supply function) Blood pressure Dependence of blood pressure on cardiac output and vascular parameters Model of blood pressure changes in aorta