4. Arterial Wave Speed

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Last updated 10:29 AM on 4/24/26
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40 Terms

1
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What is pulse wave velocity

The speed at which pressure or velocity changes travel through blood in the arteries

2
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What is arterial wave speed directly related to

arterial stiffness

3
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Why is PWV clinically useful

It provides a quantitative surrogate measure of arterial stiffness and risk of cardiac/cerebral events

4
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What are major cardiovascular risk factors that promote arterial stiffness

High cholesterol, high blood pressure, diabetes, smoking, and ageing

5
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What serious consequences can increased arterial stiffness cause

Heart failure and stroke

6
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What are the cardiovascular risk factors that promote arterial stiffness

high cholesterol, high blood pressure, diabetes, smoking and ageing

7
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What are the three separate processes that increase stiffness in the arterial system

Structural Breakdown of Elastin Fibers, Damage to Endothelial Function, Increase in Mean Arterial Pressure

8
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Structural Breakdown of Elastin Fibers

Occurs primarily in the aorta and Age driven

<p>Occurs primarily in the aorta and Age driven </p>
9
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Damage to Endothelial Function

  • Occurs primarily in the smooth muscle conduit arteries

  • Disease driven (e.g. T2DM, hypercholesterolemia, atherosclerosis)

10
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Increase in Mean Arterial Pressure

  • Occurs systematically throughout the arterial system

11
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Wave Speed Definition

The speed by which the changes in the pressure or velocity travel in a certain medium, and in the context of arterial system, the medium is the blood.

<p>The speed by which the changes in the pressure or velocity travel in a certain medium, and in the context of arterial system, the medium is the blood.</p>
12
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Wave speed is a physical property of the arterial wall and can be either…

regional (along an arterial segment) and local (at the measurement site)

13
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What has PWV been widely used in clinical practices as a surrogate marker for

  • cardiac and cerebral events

  • Arterial tree stiffness

14
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How can wave speed be measured

Wave speed can be measured regionally or locally

<p>Wave speed can be measured regionally or locally</p>
15
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What is foot-to-foot (called time-of-flight)

A method for the measurement of regional wave speed and has been used extensively clinically. It relies on measuring either the pressure or flow waveform at two locations that are at a known distance apart

16
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Wave speed equation

c= 𝐿 /∆t

<p>c= 𝐿 /∆t</p>
17
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What is the most commonly used distance for the measurement PWV

carotid-femoral

18
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<p>Sphygmocor</p>

Sphygmocor

instrument for the measurement of the foot-to-foot wave speed.

<p>instrument for the measurement of the foot-to-foot wave speed.</p>
19
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How is the ‘foot’ determined

The minimum pressure of each respective wave

20
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How is the time difference determined

The femoral pressure is reversed backward in time until its foot superimposes the foot of the aorta pressure

21
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How is the distance determined

estimate of the distance between the two measurement locations

<p>estimate of the distance between the two measurement locations</p>
22
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Reimann Equation

c=sqrt(1/pDs)

<p>c=sqrt(1/pDs)</p>
23
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Arterial Segment Distensibility Equation

Ds=Cs/A

24
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Ds (Arterial segment distensibility)

the fractional change of the cross sectional dA/A in response of a change in pressure dP

25
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Moens-Kortweg Equation

c=sqrt(Eh/pD)

<p>c=sqrt(Eh/pD)</p>
26
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Assumptions in Moens-Kortweg Equation

  • h is very small with respect to D; h«D

  • The tube is perfectly elastic

  • The fluid is incompressible

27
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Jokowsky Equation

∆𝑃 =𝜌𝑐∆𝑈

<p>∆𝑃 =𝜌𝑐∆𝑈</p>
28
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Otto Frank Equation

c=sqrt(k/p) ; K=A(dP/dA)

<p>c=sqrt(k/p) ; K=A(dP/dA)</p>
29
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Bramwell-Hill equation

c=1/sqrt(pDs) ; Ds=1/A(dA/dP)

<p>c=1/sqrt(pDs) ; Ds=1/A(dA/dP)</p>
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Richard Skalak equation

d𝑃±=𝜌𝑐 𝑑𝑈±

<p>d𝑃±=𝜌𝑐 𝑑𝑈±</p>
31
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Nico Westerhof Equation

Z0=𝑃̅ / 𝑈̅

<p>Z0=𝑃̅ / 𝑈̅</p>
32
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Pressure-velocity loop (PU-loop) equation

A PU-loop which provided a graphical as well as quantitative value of the wave speed. The method relied on the water hammer equation in the forward direction

d𝑃+ = 𝜌𝑐 𝑑𝑈+

d𝑃+ and 𝑑𝑈+ are the changes of the measured P and U in the forward direction

Integrating this equation gives

d𝑃+ = 𝜌𝑐 𝑑𝑈+ + P0

P+ are the pressure in the forward direction

𝑈+ are the velocity in the forward direction

P0 is an integration factor (reference pressure)

p is the blood density

c is the wave speed

This is an equation of a straight line, indicating during that during early part of systole when the relationship between P and U is linear, due to the absence of reflected waves

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Wave Speed equation

c=+- 1/p (dP+/dU+)

34
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<p>Why can obtaining simultaneous measurement of pressure and velocity be a challenge</p>

Why can obtaining simultaneous measurement of pressure and velocity be a challenge

Due to the difference in the frequency response of the equipment used for obtaining the measurements.

<p>Due to the difference in the frequency response of the equipment used for obtaining the measurements.</p>
35
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<p>Diameter-velocity loop (InDU-loop)</p>

Diameter-velocity loop (InDU-loop)

c=±1/2 *(𝑑𝑈± /d𝑙𝑛𝐷 ±)

<p></p><p>c=±1/2 *(𝑑𝑈± /d𝑙𝑛𝐷 ±)</p>
36
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tube law

relating arterial pressure with the luminal cross-sectional area is called the tube law

P = 𝛽 𝐴0 (√𝐴 −√𝐴0 ) + Γ (𝜕𝐴 /𝜕t)

Where 𝛽 = 4 3 ⁄ √𝜋 ℎ𝐸 and Γ = 𝛾 2 ⁄ √𝜋𝐴0

𝛽 and Γ are assumed to be constant and related to the elastic and visco-elastic properties of the arterial wall. A0 is the lumen cross sectional area at P=0

37
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<p>diameter-pressure loop (D2P-loop) equation</p>

diameter-pressure loop (D2P-loop) equation

c=D0*sqrt(dP/p(dD²))

<p>c=D0*sqrt(dP/p(dD²))</p>
38
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Theoretical determination of wave speed

c=sqrt ((B/2p) (A^1/4/Ao))

<p>c=sqrt ((B/2p) (A^1/4/Ao))</p>
39
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B constant

B=4/3*sqrt(pi) hE

<p>B=4/3*sqrt(pi) hE</p>
40
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wave speed in terms of cross-sectional area and wall properties

c=sqrt(B/2p * A^1/4/A0)

<p>c=sqrt(B/2p * A^1/4/A0)</p>