Title: Chap 4'
1Chap 4. The Dynamics of the Circulatory System
2I. General Structure, Volumes, and Flow Rates
Approximate Estimate of Blood Distribution in
Vascular Bed of a Man
3Blood Flow to Different Organs and Tissues under
Basal Conditions
4I. General Structure, Volumes, and Flow Rates
Systemic Circulation of a Dog
assuming blood viscosity is 0.03P
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6Systemic Circulation of Man
assuming blood viscosity is 0.035P
7II. Capillary Blood Flow
Let
Capillary diameter 8 mm The number of systemic
capillaries in body 109 Cardiac output 5
liters/min
The linear velocity of blood flow in the
capillaries is
Assuming each capillary is 1mm long, the bloods
residence time is
so little time for exchange
extremely efficient mass transfer in the
capillaries
8III. Rates of Shear in the Circulation
Rates of shear in the circulation
assuming blood viscosity is 0.03P
9IV. Pressure profiles in the circulatory system
10Diagrammatic comparison of the behavior of the
pressure and flow pulses in the systemic arteries
p78
Note that the pressure pulse increases and the
flow pulse decreases.
11Peripheral resistance
Peripheral resistance
Relative resistance to flow in the vascular bed
12V. Interconversion of pressure and kinetic
energy in the circulation
Kinetic energy ? pressure
? 1/2 for laminar ? 1 for turbulent ? 1/2
1 for transition
13V. Interconversion of pressure and kinetic
energy in the circulation
Amount and relative importance of kinetic energy
in different parts of the circulation
14A. Kinetic Energy Effects in Narrowed Arteries
- Stenosis narrowed arteries due to fatty deposits
15A. Kinetic Energy Effects in Narrowed Arteries
Let
Then,
Thus,
By the Bernoullis equation (law of energy
conservation)
Cave in at the stenosis
Due to the significant increase of the peripheral
resistance
Causing the flow to slow down
Decrease in KE
Increase in pressure
Periodic closing and opening flutter
16A. Kinetic Energy Effects in Narrowed Arteries
- Pressure rise in an aneurysm
17Ruptured AAA
Un-ruptured (control) AAA
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19Fluid-Structure Interaction in Aneurysm
20A. Kinetic Energy Effects in Narrowed Arteries
- Pressure rise in an aneurysm
Let
Then,
Thus,
By the Bernoullis equation (law of energy
conservation)
Arterial rupture
21VI. Mechanical Energy Balance
Bernoulli equation
22VI. Mechanical Energy Balance
A. Horsepower of the heart
- Assuming
- Cardiac output 5 liter/min
- (b)
- (c)
- (d) KE can be neglected
6mmHg
15mmHg
95mmHg
0mmHg
13.8 of basal metabolic rate of 72kcal/hr
23Pressure-volume diagram for the left ventricle of
the heart
Work done by the LV on the blood
Work done by the blood on the LV
Net mechanical work of the LV in one cycle
A filling phase B isometric(isovolumetric)
contraction phase C ejection phase D
isovolumetric relaxation phase E complete cycle
24B. Friction losses in the circulation
Inlet and outlet are adjacent
Thus,
- Work is done by the heart in order to overcome
frictional energy losses. - Hearts work total frictional loss
25C. Hydrostatics of the circulation
Hydrostatic pressure
collapsed
26Distensibility of the vein
artery
vein
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28Artery and vein