AME 60676 Biofluid & Bioheat Transfer 3. Body thermo-fluid-mechanics.
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Transcript of AME 60676 Biofluid & Bioheat Transfer 3. Body thermo-fluid-mechanics.
AME 60676Biofluid & Bioheat Transfer
3. Body thermo-fluid-mechanics
Objectives
• Overview of blood behavior as it flows in blood vessels:– Normal (physiologic) flow conditions– Pathophysiologic conditions– Blood flow past biomedical devices
• Overview of the mechanics and mechanical properties of cardiovascular structures
Outline
1. Blood characteristics2. Viscous behavior3. Pressure-flow relationships for non-
Newtonian fluids4. Blood vessel mechanics5. Cardiac muscle mechanics6. Heart valve mechanics
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanics
1. Blood characteristics
Non-Newtonian modelsViscous behaviorBlood characteristics
Blood elements
Plasma ( 55%) cellular elements ( 45%)
water (92%) proteins (7%) others (1%)
albumins (60%) globulins fibrinogen
90% of all proteins
blood
erythrocytes (RBCs)
leukocytes (WBCs)
thrombocytes (platelets)
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsViscous behaviorBlood characteristics
Blood elements
• Erythrocytes (red blood cells)– Involved in transport of O2 and CO2
– Biconcave disc shape (maximizes surface-to-volume ratio)
– Volume: 85 – 90 mm3
– Lifespan: 125 days– Concentration: 5 M/mm3 of whole blood
8 m
1 m2 m
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsViscous behaviorBlood characteristics
Blood elements
• Erythrocytes (red blood cells)
– Production (erythropoiesis)• in bone marrow• requires hemoglobin and iron
– Destruction• destroyed by macrophages• iron recycled in bone marrow into new hemoglobin
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsViscous behaviorBlood characteristics
Blood elements
• Leukocytes (white blood cells)– Involved in phagocytosis and immune responses– Phagocytes
• Removal of foreign bodies• Neutrophils, eosinophils, basophils
– Immunocytes• lymphocytes
– Concentration: 4k – 11k/mm3 of whole blood
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsViscous behaviorBlood characteristics
Blood elements
• Leukocytes (white blood cells)
– Neutrophils• Most abundant leukocyte• Key role in body’s defense against
bacterial invasion• Neutrophil leukocytosis
(> 7500/mm3) results from inflammation, necrosis
Neutrophil and erythrocytes (McGraw-Hill)
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsViscous behaviorBlood characteristics
Blood elements
• Leukocytes (white blood cells)
– Eosinophils• Role in allergic response, defense
against parasites• Detoxification of foreign proteins
Eosinophil, neutrophil, erythrocytes and platelets
(University of Texas)
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsViscous behaviorBlood characteristics
Blood elements
• Leukocytes (white blood cells)
– Basophils• Releases histamine in area of
tissue damage– To increase blood flow– To attract other leukocytes
Basophil, erythrocytes and platelets (University of Texas)
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsViscous behaviorBlood characteristics
Blood elements
• Leukocytes (white blood cells)
– Lymphocytes• Release of antibody molecules• Disposal of antigen• B lymphocytes (20%)
– Produced in bone marrow– Antibody molecules synthesis (humoral
immunity)
• T lymphocytes (80%)– Produced in thymus gland– Attack virus-infected cells or regulate other
immune cells (cell mediated immunity)
Lymphocyte, erythrocytes and platelets (University of Texas)
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsViscous behaviorBlood characteristics
Blood elements
• Thrombocytes (platelets)– Involved in blood clotting
(formation of mechanical plugs in hemostatic response to injury)
• Adhesion, secretion, aggregation, fusion
– Size: 1-2m in diameter– Normal count: 250,000/mm3 of
whole blood
Platelets and erythrocytes(University of Texas)
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsViscous behaviorBlood characteristics
2. Viscous behavior
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
Plasma
• Density: 1035 kg/m3
• Dynamic viscosity: 0.0012 kg/(m.s)
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
Whole blood
• Density: ρ = 1060 kg/m3 (water: 1000 kg/m3)
• Dynamic viscosity: = 0.003 – 0.004 kg/(m.s)(water: 0.001 kg/(m.s))
• Non-Newtonian fluid: : strain rateT: temperatureH: hematocrit (volume percent of blood occupied by formed elements; normal: 40% - 45%)
, ,T H
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
Whole blood
• Nonlinear behavior at low shear rates
• Existence of a minimum yield stress
Shear stress normalized to plasma viscosity vs. rate of shear (Whitmore, 1968)
Square root of shear stress normalized to plasma viscosity vs. square root of shear rate
(Whitmore, 1968)
• Casson’s fluid behavior:
y cK
1.53 2.0p
yield stressyield stress
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
Whole blood
• Apparent viscosity:
• Apparent viscosity increases as shear rate decreases
• Asymptotic behavior as >>1
2
2.01.53app p
Apparent viscosity vs. shear rate(Whitmore, 1968)
0.035
1.53 2.0p
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
Whole blood
• Effect of hematocrit– Blood viscosity increases
with hematocrit
– Blood viscosity decreases with shear rate
– RBC structure (flexible membrane) minimizes viscosity Apparent blood viscosity normalized to
plasma viscosity vs. hematocrit (Whitmore, 1968)
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
Whole blood
• Effect of plasma protein content– Globulin tends to increase
blood viscosity
– Albumin tends to lower blood viscosity
– Fibrinogen lowers blood viscosity but to a lower extent due to low concentration Apparent blood viscosity vs. shear rate
for different plasma protein contents (Flow properties of blood, 1960)
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
Whole blood
• Yield stress– Mainly dependent on
fibrinogen content and hematocrit
CF: fibrinogen content (g / 100mL)
H: hematocrit (%)
– Normal value: 0.7 dyne/cm2
– Effect on capillary blood flow
Flow initiated when:
Yield stress vs. fibrinogen content and hematocrit (Merill et al., 1965)
0.1 0.5y FH C
2w y
R p
L
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
Fahraeus-Lindqvist effect
• Definition: apparent viscosity of blood increases with the increase in vessel diameter
• Migration of the RBCs from vessel wall to center of the vessel (due to BL effect, spinning)
• Existence of 2 flow regions:– cell-free plasma region near the wall– core region near the centerline of the vessel
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
Fahraeus-Lindqvist effect
• Cell-free marginal layer modelvessel wallred blood cells
flow direction
core region cell-free region
rz1 1,
2 2,
R
4
1 2 8
R pQ Q Q
L
1
1
2
1 4 1app
R
From local flow analysis:
In large vessels:
In small vessels: O R
R
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
Fahraeus-Lindqvist effect
• Sigma effect– For small vessel diameters (capillaries), continuum
hypothesis is not valid– Need to discretize the velocity profile in different
concentric layers
R
24
18i
R pQ Q
L R
2
1app R
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
• More aggregates at lower shear rates
• N cells in a rouleaux will cause a greater disturbance than N individual cells rouleaux increase apparent viscosity
Rouleaux and aggregates
Rouleaux of human red cells(Fung, 1993)
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
• Under high shear rates:– blood aggregate size ↓– viscosity ↓– RBC deformation becomes more evident– RBCs elongate and line up along flow direction
Red blood cell deformation
RBC deformation under shear stress (Caro, 1978)
t = 10 N.m-2 t = 300 N.m-2
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian modelsBlood characteristicsViscous behavior
3. Pressure-flow relationships for non-Newtonian fluids
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsViscous behaviorBlood characteristics Non-Newtonian models
Power law fluid
• n = 1: Newtonian fluid• n < 1: pseudoplastic
(shear-thinning) behavior
• n > 1: dilatant (shear-thickening) behavior
nK K: flow consistency index (Pa.sn)n: behavior index (dimensionless) 0.75 for human whole blood
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsViscous behaviorBlood characteristics Non-Newtonian models
Power law fluid
• Velocity profile:
• Volume flow rate:
nK K: flow consistency index (Pa.sn)n: behavior index (dimensionless) 0.75 for human whole blood
1 1 1
1 2
n n n
n nn pu r R r
n KL
13
3 1 2
nn R R p
Qn KL
02
RQ r u r dr
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsViscous behaviorBlood characteristics Non-Newtonian models
Bingham plastic
y K y: yield stressK: viscosity coefficient
• Velocity profile:
• Radius at which yield stress is attained:
2 2
4yp
u r R r R rKL K
2 yc
LR
p
uc
u(r)
Rc
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsViscous behaviorBlood characteristics Non-Newtonian models
Bingham plastic
y K y: yield stressK: viscosity coefficient
• Volume flow rate:
44 2 24 1
18 3 3
y yR pQ
KL R p L R p L
0
2 2 c
c
R R
RQ r u r dr r u r dr
uc
u(r)
Rc
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsViscous behaviorBlood characteristics Non-Newtonian models
Casson’s fluid(preferred whole blood model)
y K y: yield stressK: viscosity coefficient
• Velocity profile:
• Radius at which yield stress is attained:
2 2 3 2 3 22 2 2
1 4
4 3 2y y pp
u r R r R r R rK L K K L
2 yc
LR
p
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsViscous behaviorBlood characteristics Non-Newtonian models
Casson’s fluid(preferred whole blood model)
y K y: yield stressK: viscosity coefficient
• Volume flow rate:
4 1 24
2
2 2 21 4 161
8 21 3 7y y yR p
QK L R p L p L R p L
0
2 2 c
c
R R
RQ r u r dr r u r dr
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsViscous behaviorBlood characteristics Non-Newtonian models
Whole blood model: summary
• Non-Newtonian behavior (Casson’s fluid)
• Apparent viscosity is high at low shear rates (RBC aggregation)
• Shear thinning behavior (as shear rate , apparent viscosity )
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsViscous behaviorBlood characteristics Non-Newtonian models
Hemolysis
• Blood cell damage (destruction or activation)• Depends on:
• Shear stress magnitude• Exposure time
• RBC hemolysis:– Hemoglobin release in
plasma (anemia)• Platelet activation:
– Adherence of activated platelets to subendothelialstructures (thrombus formation)
Shear stress vs. exposure time for hemolysis of RBCs and platelet
destruction
Heart valve mechanicsCardiac muscle mechanicsBlood vessel mechanicsViscous behaviorBlood characteristics Non-Newtonian models
4. Blood vessel mechanics
Heart valve mechanicsCardiac muscle mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Blood vessel mechanics
Blood vessel components
• Elastin fibers: all vessels but capillaries and venules
• Collagen fibers: stiffer but slack
• Smooth muscle
• Endothelial cells
Heart valve mechanicsCardiac muscle mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Blood vessel mechanics
Blood vessel components• Elastin + collagen function: to
maintain a steady tension within the vessels to act against the transmural pressure
• Smooth muscle function: to provide an active tension by means of contraction under physiological control (vascular resistance regulated primarily in smaller arteries and arterioles)
• Endothelial cells: sensors, no mechanical function
Heart valve mechanicsCardiac muscle mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Blood vessel mechanics
Blood vessel behavior
• Structure contribution to material behavior
• Stress-strain behavior– Individual components: linear elastic materials– Individual fiber combination: bilinear curve– Tissue-level: nonlinear behavior
collagen fiberselastin fibers
Heart valve mechanicsCardiac muscle mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Blood vessel mechanics
Blood vessel behavior• Elastic modulus
– Elastin fiber: 106 dynes/cm2
– Collagen fiber: 109 dynes/cm2
– Smooth muscle: depends on muscle state• Typical stress-strain curve for blood vessel:
collagen
elastin
collagen + elastin collagen fiber icollagen fiber i+1
collagen fiber i+2
Heart valve mechanicsCardiac muscle mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Blood vessel mechanics
Material characterization considerations
• Testing protocol requirements:– Preconditioning over several loading-unloading
cycles (compensate for hysteresis)– Physiological environment
• Controlled ionic content, moisture, temperature, …
• Test on native blood vessels:– long segments to neglect end-effects– compensate for effect of smooth muscle
relaxation/contraction
Heart valve mechanicsCardiac muscle mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Blood vessel mechanics
Material characterization considerations
• Assumptions:– Knowledge of p, R, t E
2pRE
t R
2 2 21 1 1 1 2
2 2 2 22 1 2 1
1 1 1p R p R RrE
u urR R R R
Thin-walled tube
t/R < 0.1Thick-walled tube
t/R > 0.1
2
1 22 22 1 2
2inc
R R pE
R R R
2
2p
RE p
R
Heart valve mechanicsCardiac muscle mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Blood vessel mechanics
increasing E
Material characterization considerations
• Assumptions:– Homogeneity, isotropy, compressibility
• Non homogeneous material (different layers, different components)
• Anisotropic material:
information reported in Poisson’s ratio • Incompressible material ( = 0.5)
longitudinalradial circumferential
Heart valve mechanicsCardiac muscle mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Blood vessel mechanics
Residual stresses• Arterial wall tissue is not stress-free at zero
transmural load
Heart valve mechanicsCardiac muscle mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Blood vessel mechanics
Residual stresses
• Magnitude described in terms of opening angle of sector shape
• Residual strains computed by measuring circumferential lengths of intima and adventia in uncut and cut configurations
• Function of:– Anatomical location– Species– Location of radial cut
Heart valve mechanicsCardiac muscle mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Blood vessel mechanics
5. Cardiac muscle mechanics
Heart valve mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Cardiac musle mechanics
Material characterization
• Diastolic and systolic contractile properties
• Orthotropic material: force-deformation behavior stiffer along fibers than in transverse direction
intercalated disk (sectioned)
mitochondrianucleus
cardiac muscle cell
contractile fibers
intercalated disk
Heart valve mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Cardiac musle mechanics
Material characterization
• Fiber orientation varies along wall thickness
Tests performed on papillary muscles (longitudinal fiber orientation)
intercalated disk (sectioned)
mitochondrianucleus
cardiac muscle cell
contractile fibers
intercalated disk
Heart valve mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Cardiac musle mechanics
Material characterization
• Non linear exponential stress-strain behavior• Effects of contractile properties:
– Muscle contraction muscle shortening
shortening velocity
afterload
maximal isometric
force
Vmax
Heart valve mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Cardiac musle mechanics
Material characterization
• Non linear exponential stress-strain behavior• Effects of contractile properties:
– Effect of preload
shortening velocity
afterload
Vmax
Increasing preload
Heart valve mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Cardiac musle mechanics
6. Heart valve mechanics
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
Motivations
• Mechanical forces influence the remodeling of live tissues
• Changes in the mechanical environment result in pathological responses (e.g., valve calcification)
• Mechanical environment is essential for the design of implants and medical devices
• Tissue engineered heart valve
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
Hemodynamic Environment
Aortic valve Mitral valve
Flow visualization (polymeric valve) Ultrasound Doppler Velocimetry (native valve)
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
Mechanical EnvironmentAortic valve Mitral valve
aorta
left ventricle
pressuretensile stressbending
stress
Diastolic forces Mitral valve leaflet motion
Fluid shear stress, bending stress, tensile stress,pressure, chordal tension, muscular contraction
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
flow
aorta
left ventricle
bending stress
tensile stress
Mechanical EnvironmentAortic valve Mitral valve
Systolic forces Mitral valve leaflet motion
Fluid shear stress, bending stress, tensile stress,pressure, chordal tension, muscular contraction
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
AV Leaflet Structure• Tri-leaflet structure• Tri-layered structure:
– Fibrosa: circumferentially aligned collagen fibers– Spongiosa: loose, watery connective tissue
containing mainly GAG– Ventricularis: radially aligned elastin fibers
intertwined with collagen fibers• Cell population:
– Endothelial cells– Interstitial cells:
• Myofibroblasts: prominent stress fibers and α-SMA• Fibroblasts: synthetic phenotype with synthetic and
secretory organelles• Smooth muscle cells
Aortic valve leaflet structure
Ventricularis
Spongiosa
Fibrosa
left ventricle
aortaendothelial cells
interstitial cells
Dissected and unfolded aortic valve
L R N
coronary ostia
leaflets left ventricle
aorta
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
AV Leaflet Mechanical Response
• Leaflet tissue behaves as other soft tissues:• Anisotropic: Complex structural characteristics
lead to directional response
• Non-homogeneous: material response varies throughout the leaflet
• Non linear stress-strain relationship
• Viscoelastic: hysteresis, creep, stress relaxation, loading rate dependence
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
AV Leaflet Mechanical Response
• Unstressed state: disorganized collagen fibers in unstressed state
• Stressed state: elastin and collagen fibers orientation in circumferential direction
Collagen fiber orientation in AV leaflet (small angle scattering) (Billiar and Sacks, 2000)
25
35
45
55
65
Stress-free state p = 4 mmHg
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
AV Leaflet Mechanical Response
• Anisotropic material
• Greater stiffness in direction of collagen fibers
• Non-linear stress-strain relationship (exponential relationship)
Mean stress-strain response of AV cusps under equibiaxial tension (Billiar and Sacks, 2000)
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
AV Mechanical Forces
0
0.1
0.2
0.00 0.20 0.40 0.60 0.800 0.2 0.4 0.6 0.80
0.2
0.1
20
19
18
17
16
a)
b)
stra
inle
afle
t le
ng
th (
mm
)
time (s)
0
0.1
0.2
0.00 0.20 0.40 0.60 0.800 0.2 0.4 0.6 0.80
0.2
0.1
2020
1919
1818
1717
1616
a)
b)
stra
inle
afle
t le
ng
th (
mm
)
time (s)
Stretch waveform (Thubrikar, 1990)
0 0.2 0.4 0.6 0.8 1-10
-5
0
5
10
15
aortic surface
wall shear stress
(dyn/cm2)
time (s)0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9
0
20
40
60
80
100
ventricular surface
wall shear stress
(dyn/cm2)
time (s)
Shear stress waveform (Sucosky, 2009)
0
0.1
0.2
0.00 0.20 0.40 0.60 0.80
Time (s)
Str
ain
0 0.2 0.4 0.6 0.80
0.2
0.1
20
19
18
17
16
a)
b)
stra
inle
afle
t le
ng
th (
mm
)
time (s)
0
0.1
0.2
0.00 0.20 0.40 0.60 0.80
Time (s)
Str
ain
0 0.2 0.4 0.6 0.80
0.2
0.1
2020
1919
1818
1717
1616
a)
b)
stra
inle
afle
t le
ng
th (
mm
)
time (s)
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
AV Leaflet Mechanobiology:Effects of Shear Stress
• Effects of steady shear stress on collagen and GAG synthesis
• Effects of steady shear stress on cathepsin L expression and activity
Ratio of sGAG
content relative to
control
Ratio of collagen
synthesis relative to
control
1.5
1
0.5
1.8
0.9
0
control
Shear stress (dyn/cm2) Shear stress (dyn/cm2)1 9 25 40 80 1 9 25 40 800
control
Cathepsin L activity (gelatin zymography)Cathepsin L expression
(Western blot)
25 kDa
25 kDa
cont
rol
shea
r
Cathepsin gelatin zymography
Cathepsin gelatin zymography + E-64
cont
rol
shea
r
25 kDa
Den
sito
met
ric
fold
uni
ts
(% o
f con
trol
)
control shear
*150
100
50
0
Xing, 2004
Platt et al., 2006
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
AV Leaflet Mechanobiology:Effects of Shear Stress
Fresh tissue Ventricular surface
Aortic surface
Effect of altered shear stress
Fresh tissue Ventricular surface
Aortic surface
Effect of normal shear stress
Fold
incr
ease
of e
xpre
ssio
n pe
r cel
l vs.
fres
h
Fold
incr
ease
of e
xpre
ssio
n pe
r cel
l vs.
fres
h
0
2
4
6
8 VCAM-1 ICAM-1 BMP-4TGF-beta1
0
2
4
6
8 VCAM-1 ICAM-1BMP-4 TGF-beta1
*
***
Normal condition Altered condition
ventricular surface
aortic surface
Altered condition Normal condition
ventricular surface
aortic surface
Sucosky et al., 2009 Arterioscler Thromb Vasc Biol
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
AV Leaflet Mechanobiology:Effects of Stretch
• Collagen content increased in presence of cyclic stretch
• Cyclic stretch alters fiber composition
0
10
20
30
40
50
60
70
80
90
100
Fresh Static Stretched
Composition of Collagen Fibers in Aortic Valve
Perc
enta
ge o
f par
ticul
arty
pe o
f col
lage
n fib
er (%
)
Increasing Fiber maturity
Colla
gen
amt (
ug/m
g dr
y tis
sue
wei
ght)
0.00
10.00
20.00
30.00
40.00
50.00
60.00
70.00
80.00
Am
ount
(ug
/mg
dry
tissu
e w
eigh
t)
*
* * p<0.05
Fresh Static Stretched Balachandran et al., 2006
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
AV Leaflet Mechanobiology:Effects of Stretch
Static Stretched
Fresh 70 bpm, 48h 120 bpm, 48h
A
V
A
50 μm
A: aortic surface; V: ventricular surface; blue: nucleus; red: MMP-2
• Stretch increases MMP-2 expression
• Stretch increases MMP-2 activityFresh S-48h S-120h 70b/ 70b/ 120b/ 120b/
48h 120h 48h 120h
72 kDa pro-MMP267 kDa MMP2
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
AV Leaflet Mechanobiology:Effects of Stretch
120 h static 70 bpm, 120 h 120 bpm, 120 h
48h static 120 bpm 48 h70 bpm 48 h
A
V
A
100 μm
A
V
A
V
A
V
A
• Cyclic stretch induces cell proliferation
A: aortic surface; V: ventricular surface; blue: nucleus; red: proliferating cellsCardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
MV Leaflet Structure
• Bi-leaflet structure• Tri-layered structure:
– Atrialis: elastin fibers– Spongiosa: GAG– Ventricularis: collagen fibers
Mitral valve leaflet structure
Ventricularis
Spongiosa
Atrialis
left ventricle
left atrium
endothelial cells
Dissected and unfolded mitral valve
anterior marginal chord
anterior strut chord
commissuralchord
posteriormarginal
chord
posterior intermediatechord
basal posteriorchord
papillary muscle
anterior leaflet
commissureposterior
leaflet
Chord structureelastin layer
inner collagen core
outer endothelial layer
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
MV Leaflet Mechanical Response
• Unstressed state: disorganized collagen fibers in unstressed state
• Stressed state: elastin and collagen fibers orientation in circumferential direction
Collagen fiber orientation in MV leaflet (small angle scattering) (Sacks et al., 2003)
25
35
45
55
65
radial direction
circumferential direction
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
MV Leaflet Mechanical Response
• Major principal stretch: radial direction• Early leaflet closure: rapid rise• Valve closure: plateau (collagen fiber locking)• Valve opening: principal stretch drops down to strain free
levels
In vitro assessment of stretch levels on anterior MV leaflet (marker technique)
1
1.1
1.2
1.3
1.4
1.5
0 0.1 0.2 0.3 0.4 0.5
Pri
nci
pal
str
etch
Time (s)
Major principal stretch Minor principal stretch
0.9
1
1.1
1.2
1.3
1.4
1.5
Major Minor
Str
ec
h
Principal stretch
Posterior leaflet
Anterior leaflet
Comparison of the principal stretches on
anterior and posterior MV leaflets
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics
MV Leaflet Mechanical Response
• Early leaflet closure: small p large • Leaflet stiffening: large p small (collagen
fiber locking)
MV5 NNat r=s=0
Areal strain1.0 1.1 1.2 1.3 1.4 1.5 1.6
Tra
ns-
mitr
al p
ress
ure
(m
mH
g)
0
20
40
60
80
100
Physiologic load-strain curve of the MV anterior leaflet
collagen fiber configuration
Cardiac muscle mechanicsBlood vessel mechanicsNon-Newtonian models Viscous behaviorBlood characteristics Heart valve mechanics