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33 Cards in this Set

  • Front
  • Back
Hemodynamics
Blood flow is driven by a constant pressure along varying resistances
Elements of CV system
Pump, vessels, blood
Blood pressure
Measured as pressure difference between two points
Blood flow
Blood flow = cardiac output = stroke volume x heart rate
Types of pressure difference
Axial, radial, hydrostatic
Circulation evolutionary consequence of:
body size
Circulatory system integrates three organs:
heart, blood vessels, blood
The heart is a dual pump that drives the blood that drives blood in two serial circuits of blood vessels:
systemic and pulmonary circulations
Driving pressure difference
= Flow x Resistance (viscous)
Flow
= delta(V) / delta(t)
= Av (cross section x velocity)
Blood flow is driven by constant pressure head across variable resistances
Left and right heart each maintain a constant pressure head that drives blood flow across a branched system of blood vessels acting as resistors
Total peripheral resistance to blood flow is result of combination of blood vessels in parallel and in series
Parallel:
1/R_total = 1/R_1+1/R_2+1/R_3+...

Series:
R_total=R_1+R_2+R_3+...
Three types of pressure difference in blood vessel:
Driving pressure between arterial and venous ends of the circulation:
(between 2 points along x axis)

Transmural pressure between intravascular and tissue space (between two points along r axis)

Hydrostatic pressure between two points in a vertical column of blood (between two points along h axis)
Total flow of blood delivered by the heart (total mean flow in the circulation) is called the cardiac output
Total flow of blood = Cardiac output = Heart Rate x Stroke volume.

Example:
4.9 L/min = 70 beats/min x 70 mL/beat
Flow in idealized vessel increases with the fourth power of radius:
Hagen-Poiseuille Equation

F = delta(P) * pi*r^4 / (8*nu*l)
Viscous resistance to flow is proportional to the viscosity of blood, but does not depend on properties of the blood-vessel walls
R = 8*nu*l/ (pi*r^4)
Viscosity of blood
Measure of the lack of "internal slipperiness" between layers of fluid

viscosity = nu = shear stress / shear rate
=(Force/A)/(delta(v)/delta(x))
Blood flow is laminar
Distinction between laminar and turbulent flow is clinically very important
Critical quantity concerned in the generation of turbulence
Reynolds number (dimensionless)

Re = v_bar * 2r*rho / nu

v_bar = mean linear velocity
r = vessel radius
pho = density of fluid
nu = viscosity of fluid
Pressure and flow oscillate with each heartbeat
Maximum: systolic
Minimum: diastolic
Gravity
When there is a difference in height, there will be a hydrostatic pressure difference
Low compliance of vessel
Causes transmural pressure to increase when the vessel blood volume is increased
Viscous resistance of blood
Causes axial pressure difference when there is flow
Inertia of blood and vessels
Causes pressure to decrease when velocity of blood flow increases
Whole blood
Whole blood has an anomalous viscosity. Although the viscosity of water and blood plasma are Newtonian, whole blood is non-Newtonian (viscosity varies with rate of shear or flow)
Influence on blood viscosity:
i) Increases with fibrinogen concentration

ii) Increases with hematocrit

iii) Decreases as vessel radius falls belows a certain threshold

iv) Increases at low flows

v) Increases at low temperatures
With progressive branching of vascular tree, several parameters change at each arborization:
i) Number of vessels

ii) Vessel radius

iii) Aggregate cross-sectional area of vessels

iv) mean linear velocity

v) flow through a vessel

vi) relative blood volume

vii) circulation (or transit) time

viii) pressure profile
Physical properties of vessels
Closely follow level of branching in the circuit
Blood volume
Mostly resides in systemic veins
Intravascular pressures
Intravascular pressures along the systemic circuit are higher than those along the pulmonary circuit
Steepest drop in systemic circulation
Under normal conditions, occurs in arterioles, the site of greatest vascular resistance.
Vasoconstriction and vasodilation can steepen or flatten the pressure profile
Local intravascular pressure
Depends on distribution of vascular resistance. Midpoint capillary pressure

Pc = [(Rpost/Rpre)Pa+Pv] / [1+(Rpost/Rpre)]
Blood vessels are elastic tubes
Distensible elastic materials in blood vessels (elastin and collagen) allow blood vessels to distend with increasing pressure, thereby decreasing resistance