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Published byMelinda Fleming Modified over 9 years ago
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Conduits –To conduct blood to the organs and periphery Impedance matching –Minimise cardiac work –Minimise pulse pressure –Control flow according to demand What are arteries for?
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What are arteries made of? Why do large arteries become stiffer with age (and disease)? Why are some people affected more than others? Questions Conduit arteries: large arteries near the heart and their main branches Why are conduit arteries distensible?
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Arteries are distensible because: 80 100 120 1 sec The wheel has yet to evolve in the animal kingdom (bacteria have propellers) Therefore(?) the heart is a pulsatile pump. Its output consists of a pulse wave superimposed on a steady component.
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Systolic pressure Diastolic pressure Average pressure Pulse pressure = systolic pressure - diastolic pressure 80 100 120 1 second Pressure [mmHg] Aortic pulse wave
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Average pressure determined by resistance of peripheral arteries Pulse pressure determined by elasticity of large arteries Pulse pressure = systolic pressure - diastolic pressure Systolic pressure Diastolic pressure Average pressure 80 100 120 1 second Pressure [mmHg]
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The pulse is a wave of dilatation With thanks to Chris Martyn
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Similar to a surface wave
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A heavenly wave
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Speed of the wave is related to the stiffness of the artery it is traveling in The stiffer the artery; the higher the wave speed Wave speed is proportional to the square root of arterial stiffness
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Blood vessel elasticity Inelastic Pseudo elasticity Non linear Large strains Strain energy function/incremental approach Anisotropic Uni-axial expts./circumferential direction Viscoelastic Quasi static experiments }
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Stress, strain and elastic modulus A reminder.
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Stress ( , sigma) –Force per unit area= (F/A) Strain ( , epsilon) –Change in length per unit length= ( L/L 0 ) Elastic (Young’s) modulus (E) –stress/strain= F L0F L0 A LA L = Poisson’s ratio (, nu) –transverse strain /longitudinal strain= - x / y –for incompressible materials
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2001000 Pressure (mmHg) Relative Radius 1.0 1.5 2.0 PP P RR R PP P RR R
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Incremental strain Incremental stress Incremental elastic modulus (structural stiffness) 2001000 Pressure (mmHg) RR 1.0 1.5 2.0 PP RR R P 2001000 Pressure (mmHg) Relative Radius 1.0 1.5 2.0 PP P RR R PP P RR R
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2.62.42.22.01.81.61.41.21.0 R/Ro 0 5 10 15 E inc [Nm -2 x 10 5 ] Variation of E inc with stretch
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Structural & functional stiffness Geometry Structure Functional stiffness Structural stiffness
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Some haemodynamics P Q Steady flow resistance = k p E R 2 = k µl R 4 µ:viscosity l: length R: inner radius k 1 :constant Z c ˆ P ˆ Q Characteristic impedance (pulsatile flow “resistance”)
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Just a touch more Z c cc R2R2 c:pulse wave velocity :tissue & blood density c k E p Measure pulse wave velocity non invasively to estimate functional stiffness = k E p R 2
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Summary The relationship between vessel dimensions, elasticity and blood flow Structural stiffness Functional stiffness Characteristic impedance (a measure of all the factors which combine to limit pulsatile flow due to a pulsatile pressure gradient) Structure & geometry Functional stiffness & diameter
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Electrical analogue R 1 : resistance of large vessels L 1 : inertia of blood C 1 : compliance of large vessels R 2 : peripheral resistance R 3 : source resistance of heart R1R1 L1L1 R3R3 R2R2 C1C1
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Reflections In the arterial system reflections of pressure and flow waves occur wherever there is a change in the local fluid impedance Decrease in diameter or increase in stiffness -> positive reflection of pressure negative reflection of flow If no reflections: pressure and flow waves are the same shape Arterial disease usually associated with increased reflections (except aneurysms) Energy is lost so cardiac output must increase to maintain a given flow
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Wave reflection mean pressure/mean flow pulsatile pressure/pulsatile flow resistance characteristic impedance ∆t Pressure Flow Time
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Fourier analysis H1 + H2 H3 36027018090 -2 0 1 2 H1 + H2 + H3 H4 Mean H1 H2 Measured H1+H2+H3+H4
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Q(t) = q 0 + q 1 Cos( t - 1 ) + q 2 Cos( t - 2 ) + q 3 Cos( t - 3 ) +... P(t) = p 0 + p 1 Cos( t - 1 ) + p 2 Cos( t - 2 ) + p 3 Cos( t - 3 ) +... |Z| = |p n |/|q n |Pressure/Flow F = n - n Pressure - Flow
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