arterial system & hemodynamics arterial system pressures in the circulation arterial pressure...

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Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics is the study of the physical principles that govern blood flow in the cardiovascular system. Factors affecting resistance to flow Laminar & turbulent flow Tension, pressure and radius

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Page 1: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Arterial System & Hemodynamics

Arterial system

Pressures in the circulation

Arterial pressure during diastole

Pulse pressure and work of the heart

Hemodynamics is the study of the physical

principles that govern blood flow in the

cardiovascular system.

Factors affecting resistance to flow

Laminar & turbulent flow

Tension, pressure and radius

Page 2: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Arterial system

The arterial system consists of:

Elastic arteries: major distribution vessels with a large component of elastic

tissue and low resistance: aorta, brachiocephalic, common carotid, subclavian

and pulmonary arteries.

Muscular arteries: distributing branches with more muscular tissue and less

elastic tissue: radial, femoral, coronary and cerebral arteries.

Arterioles: terminal branches that supply the capillaries.

Page 3: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

= MAP Mean & pulse pressures in the circulation Systolic pressure

80

100

120

60

40

20

L ve

ntr

icle

Art

erie

s

Cap

illa

ries

Art

erio

les

Art

erie

s

Rt a

triu

m

Rt v

entr

icle

Ve

ins

Cap

illa

ries

Ve

ins

L a

triu

m

L ve

ntr

icle

Ve

nule

s

PulmonarySystemic

Pu

lse

pre

ssu

re

Pre

ssur

e, m

m H

g

Shaded area = systolic pressure - diastolic = pulse pressure

Diastolic pressure

Page 4: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Pulse pressure depends on stroke volume and aortic compliance

Peak systolic pressure & pulse pressure are determined by stroke volume & aortic compliance.

Compliance depends on the elastic tissue of the aorta.

Pulse pressure = peak systolic minus diastolic pressure.

A decrease in aortic compliance will result in a higher peak systolic pressure & pulse pressure (assuming stroke volume is unchanged).

Stroke volume

Pulse pressure Mean arterial pressure

Aortic compliance

Aortic valve closure

Page 5: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Arterial pressure is maintained during diastole by recoil of the aorta

The stroke volume is ejected during the rapid ejection period & is accommodated by expansion of the aorta.Aortic pressure is maintained during diastole by recoil of the aorta as blood flows to the periphery.Because of the elasticity of the aorta and large arteries, the pulsatile pressure signal is gradually dampened so that flow is steady (not pulsatile) in the venules.

During diastole the aortic valve is closed and recoil of the elastic aorta drives blood to the periphery

systole

diastoleLeft Ventricle

Aorta

pre

ssur

e

Page 6: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Central and peripheral aortic pressures

Simultaneously recorded pressures from the aortic root (Ao) and femoral artery (FA) demonstrate delayed transmission and a higher systolic pressure in the femoral artery.

Although peak pressure is higher in the femoral artery than the aorta, average driving pressure (MAP) is higher in the aorta than the femoral artery.

There is smoothing of the pressure waveform and loss of the dicrotic notch between the aorta and femoral artery.

UpToDate®

Page 7: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

The work of the heart consists of pumping volume against pressure

Work = force (f) operating over distance (dl): W = (f)( dl)

For work done by a piston with area A moving against pressure P,

For the left ventricle:

P = afterload = arterial pressure when the aortic valve is open &

V = stroke volume, so

cardiac work = stroke volume x afterload

A

dl

P

VPW

so(V)volumedlA

dlAPW

APfA

fP

Page 8: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Age

Art

eria

l pre

ssu

re

100

150

50

20 40 60 80

mean

diastolic

systolic

Systolic and pulse pressures increase with age

Determinants of pulse pressure:Stroke volumeAortic compliance

Aging & atherosclerosis aortic compliance systolic pressure & pulse pressure cardiac work due to systolic pressure

Page 9: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

A decrease in aortic compliance or an increase in afterload increase cardiac work

Cardiac work = stroke volume x afterload.

Cardiac work stroke volume x systolic BP.

Increasing systolic pressure increases cardiac work.

Compliance of the aorta minimizes peak systolic pressure & cardiac work.Cardiac work increases with age, & in hypertension, aortic stenosis or coarctation.

% in

crea

se in

vol

ume

10060 140 180

Pressure, mm Hg

22 y

ears

old

75 years old

C = DV/DP

150

200

250

100

50

Difference in aortic compliance in young versus old subjects

Page 10: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Arterial, arteriolar & capillary resistance

The resistance of an individual vessel is inversely proportional to radius so

R artery < R arteriole < R capillary

The total resistance of a category of vessels is determined by the total cross

sectional area of all the vessels and the radius of the individual vessels.

Comparing arteries & arterioles supplying an organ, the total resistance of the

arterioles is greater than the resistance of the arteries.

Comparing arterioles & capillaries, the total cross sectional area of the capillaries

is so much greater than the area of the arterioles that the total resistance of the

capillaries is less than the resistance of the arterioles.

The greatest pressure drop in the circulation is across the arterioles.

Page 11: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Series & parallel resistances

Resistances in series are additive; total resistance equals the sum of individual resistances.

Resistances in parallel add as the inverse sum, like parallel electrical circuits:

Most vessels of a given category are arranged in parallel.

...R

1

R

1

R

1

R

1

321total

Conductance is the inverse of resistance.

For Parallel circuits conductances are additive

Ctotal = C1 + C2 + C3

P

F

R

1cetanConduc

Series and parallel resistance

Page 12: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Parallel resistances in the systemic circulation

Aorta

Arteries to stomach, spleen, pancreas, gut

Arteries to CNS

Hepatic artery

Arteries to limbs & trunk

Renal arteries

Coronary arteriesArterial beds are arranged in parallel

Venous pressure is small compared to arterial pressure.

Blood pressure is nearly the same in all large arteries, so DP is the same in all vascular beds:

DP = MAP – VP MAP and

MAP = CO X TPR

The resistance of each arterial bed is set by its own arteriolar tone

TPR is less than the resistance of any single arterial bed.

For example:

TPR = MAP/CO

Renal resistance = MAP/renal flow

And renal flow < CO so

Renal resistance > TPR

There are multiple parallel paths for blood flow so total peripheral resistance is less than resistance in any one bed.

Page 13: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Laminar & turbulent flow

Normal flow in the circulation is laminar.

Laminar (or streamlined) flow exhibits maximal velocity at the center of the vessel, and concentric thin layers of plasma with gradually decreasing velocity toward the walls of the vessel. Laminar flow is silent.

Plasma flowing closest to the vessel wall exerts a drag on the wall (shear stress) that influences endothelial function.

Turbulent flow exhibits irregular radial mixing of blood as overall flow occurs in the longitudinal direction.

Turbulent flow usually causes vibrations that are audible with the stethoscope as murmurs or bruits.

The pressure gradient required to drive turbulent flow is greater than that required to drive laminar flow so turbulence increases cardiac work.

Turbulent

Laminar

Page 14: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Causes of turbulent flow

Examples of turbulent flow:Flow across an obstruction (aortic stenosis, coarctation)Abnormally high flow velocity (high CO & reduced viscosity in severe anemia)Regurgitant flow across an incompetent heart valveAbnormal shunt from a high to low pressure chamber (ventricular septal defect)Presence of turbulent flow increases the likelihood of development of blood clots

Flow in the vascular system is normally laminar.Turbulence occurs if Reynold’s number (NR) exceeds 3000:

Factors predisposing to development of turbulence in flowing fluid include:Greater density (r)larger vessel diameter (D)High velocity (v)Low viscosity (h)

In addition, turbulence is likely in the presence of abrupt changes in vessel diameter or irregularities in vessel walls as may occur with atherosclerosis or other pathology.

Dv

NR

Page 15: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Viscosity and hematocrit

Viscosity of a fluid is its resistance to flow resulting from molecular cohesion.Blood is a complex mixture of fluid and cells; blood viscosity increases with hematocrit.

Resistance to blood flow is proportional to viscosity ():

4πr

8LηR

10 30 50 70

Hematocrit

Normal hematocrit

visc

osi

ty

anemia

polycythemia

Viscosity of whole blood (solid line) relative to plasma (dashed line) as a function of hematocrit

Page 16: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Vessel diameter and viscosity of blood

0.1 0.20.3 0.4 0.5

Rel

ativ

e vi

sco

sity

Vessel diameter, mm

Blood viscosity decreases in vessels with diameter < 0.3 mm (300 mm)

Mechanism is complicated but the effect reduces resistance to blood flow.

Most of the resistance in the systemic circulation is from arterioles with small

diameters. Lower resistance reduces the work of the heart.

Viscosity increases at low temperature, & may reduce blood flow in the

extremities & contribute to frost bite.

Page 17: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Law of Laplace

The law of Laplace states that tension (T) in the wall of a blood vessel equals the product of transmural pressure (P) and radius (r):

Tension is a force acting tangential to the surface of a cylinder.

P is transmural pressure (internal pressure minus external)

Transmural pressure equals blood pressure minus tissue pressure. Extravascular tissue pressure is small & can be ignored so

P T

)r)(Palminralu(intT

PrT

Page 18: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Law of Laplace and tension in blood vessel walls

Radius Tension Amount of

mm Hg dynes/cm2 dynes/cm. Elastic tissueElastic arteries I00 130,000 1.3 cm 270,000 ++++Distributing arteries 90 120,000 0.5 cm 60,000 +++Arterioles 60 80,000 0.15 mm - 62 mm 1,200 - 500 elastic intima Capillaries 30 40,000 4 mm 16 None Venules 20 26,000 10mm 26 None Veins 15 20,000 200 mm 400 + Vena cava 10 13,000 1.6 cm 21,000 ++

Intravascular Pressure

T = Pr

The amount of elastic tissue in the vessel wall correlates with the wall tension.

Elastic tissue maintains wall integrity against the outward force of the pressure.

The table shows that a very small tension in the wall of the capillaries suffices to withstand the intraluminal pressure. For comparison, the breaking strength of a strip of Kleenex one cm wide is about 50,000 dynes per cm, over 3000 times as great as the tension required to maintain a capillary wall.

Page 19: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Compliance of the aorta as an example of an elastic artery

In this figure smooth muscle is relaxed pharmacologically so the vessel’s compliance is due primarily to the compliance of the elastic tissue. Compliance of elastic arteries is nearly constant over the physiological range of pressure.

Rel

ativ

e vo

lum

e, %

Pressure, mm Hg

200

300

400

100

150 20010050

Compliance decreases slightly at higher pressures

Slope = Compliance = DV/DP

Page 20: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Compliance in the vena cava as an example of a large vein

In this figure smooth muscle is relaxed; the compliance is due primarily to the changes vessel geometry.

Slope = Compliance = DV/DP

Maximal physiological pressure

Rel

ativ

e vo

lum

e, %

Pressure, mm Hg

200

300

400

100

15010050

Compliance decreases as cross section becomes circular

Page 21: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Contribution of collagen & elastic fibers to passive tension development

Ten

sio

n, d

ynes

/cm

x 1

03

Relative radius, %

80

120

160

40

Collagen fibers only

140 160120100 180

T= Pr

elastic fibers only

Intact artery

Passive tension development (smooth muscle relaxed) with increasing radius in

an intact artery or an artery with only collagen fibers (elastic fibers digested) or

only elastic fibers (collagen fibers digested).

Arterial segment studied in vitro by injecting fluid & measuring radius & tension.

Collagen fibers are least compliant, develop greatest tension for a given radius.

Page 22: Arterial System & Hemodynamics Arterial system Pressures in the circulation Arterial pressure during diastole Pulse pressure and work of the heart Hemodynamics

Wall tension and pathological changes

T = Pr

Arteries: If weakening of the wall causes dilatation (aneurism) , as the radius

increases the tension required to maintain wall integrity increases. If the wall is

too weak to maintain the tension, it will rupture.

The heart: Pathological dilation of the heart as occurs in heart failure increases

the radius of the ventricles. As a result, more tension must be generated to

create a given pressure, increasing the work of the heart & causing

progression of heart failure.