antonio fasano dipartimento di matematica u. dini, univ . firenze iasi – cnr roma
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Antonio Fasano Dipartimento di Matematica U. Dini, Univ . Firenze IASI – CNR Roma. A new model for blood flow in capillaries. FASANO, A. FARINA, J. MIZERSKI. A new model for blood flow in fenestrated capillaries with application to ultrafiltration in kidney glomeruli , submitted. - PowerPoint PPT PresentationTRANSCRIPT
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Antonio FasanoDipartimento di Matematica U. Dini, Univ. Firenze
IASI – CNR Roma
A new model for blood flow in capillaries
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A. FASANO, A. FARINA, J. MIZERSKI.
A new model for blood flow in fenestrated capillaries with application to ultrafiltration in kidney glomeruli, submitted
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• 7% of the human body weight,• average density of approximately 1060 kg/m3
• average adult blood volume 5 liters• plasma 54.3%• RBC’s (erythrocytes) 45% • WBC’s (leukocytes) 0.7%• platelets (thrombocytes) negligible volume fraction
Blood composition
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Volume VRBC 90 μm3
Diameter dRBC 78 m
RBC’s properties
Very flexible
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the available fluid mechanical laws cannot be applied for a better understanding of the microcirculation in the living capillaries, and the hemorheology in the microcirculation requires another approach than regularities of the fluid mechanics
Quoting fromG. Mchedlishvili, Basic factor determining the hemorheological disorders in the microcirculation, Clinical Hemorheology and Microcirculation 30 (2004) 179-180.
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General trend:
Adapting rheological parameters to the vessel size
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Our model ignores fluid dynamics and
considers just Newton’s law
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Driving force
Pressure gradient
drag
Translating sequence of RBCs and plasma elements
The drag is due to the highly sheared plasma film
Translating element
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Driving force
Pressure gradient
drag
Translating sequence of RBCs and plasma
The drag is due to the highly sheared plasma film
Translating element
a/R 1/3 when the hematocrit is 0.45
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If the capillary is fenestrated the plasma loss causes a progressive decrease of the element length
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The renal glomerulus is a bundle of capillaries hosted in the Bowman’s capsule
fenestrated capillaries
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Plasma cross flow is caused by TMP (transmembrane pressure):
TMP = hydraulic pressure difference
minus
oncotic pressure(blood colloid osmotic pressure)
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Element volume Vel = R2a + VRBC
Hematocrit el
RBC
VV
)(1 RHRa
3)(R
VRH RBC
R
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elel pRkuuVdtd
2
The motion of a single element(Newton’s law)
Variable owing to plasma loss
Friction coefficient
Pressure drop
elRBC pRkuudtdV
2
density
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A guess of the friction coefficient
0 Take = 0.45
0uu = 1 mm/s
0xp
0= = 40 mm Hg/mm
in the steady state equation
0k 610 = 8.8 g/s.
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in a 1.5mm capillary there are about 200 of such elements
It makes sense to pass to a continuous model
elp xpLel
)( RBCV
u
xu
t xpRuk
3)(
1
)(1)(
Rh
RH RCBC
elLR
Divide by elL
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0
u
xt
)( RBCV
u
xu
t xpRuk
3)(
1
)(1)(
Rh
RH RCBC
elLR
Conservation of RBCs
Momentum balance
To be coupled with a law for plasma outflow …
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Balance equation for plasma
Starling’s law
C = albumin concentrationRTC = “oncotic” pressure (Van’t Hoff law)
constant
external pressure
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Dimensionless variables
0kk
Lx
(L 1.5mm)
ctt
0u
Ltc convection time 1.5 sec
0uuv
Lpp e
0
)(
)()(0
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vvv
tt
c
k )()(
Momentum balance
0kV
t RBCk
stk
610
inertia is negligible
v)(
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Combining the RBC’s and plasma balance equations
or
baa 0
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Introducing the “filtration time”
we get the dimensionless system
compares oncotic and hydraulic pressures
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can be estimated, knowing that the relative change of during the convection time is 1/3
The case of glomeruli
We are interested in the (quasi) steady state
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Eliminating …
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A second order ODE
Cauchy data:
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Experimenting with various friction coefficients and Os