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3D hydrodynamics and mass transport simulations of ocular drug delivery considering segmental aqueous humor outflow phenomenon in the human eye LOKE CHAI YEE Doctoral Candidate Monash University Malaysia

3D hydrodynamics and mass transport simulations of ocular

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Page 1: 3D hydrodynamics and mass transport simulations of ocular

3D hydrodynamics and mass transport

simulations of ocular drug delivery

considering segmental aqueous humor

outflow phenomenon in the human eye

LOKE CHAI YEE

Doctoral Candidate

Monash University Malaysia

Page 2: 3D hydrodynamics and mass transport simulations of ocular

(AH)

Figure 1

Pathogenesis of glaucoma (Murgatroyd et al., 2008).

normal intraocular

pressure (IOP) ranges

from 9 to 20 mmHg

optic nerve head (ONH)

trabecular meshwork (TM)

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What is GLAUCOMA?

Page 3: 3D hydrodynamics and mass transport simulations of ocular

Circulation of the aqueous

humor (AH)

1. Production and drainage

of AH

2. Thermal-induced

buoyant forces

3

The anterior segment of the human eye: anatomy and physiology

RESEARCH BACKGROUND

Schlemm’s canal (SC)

Figure 2

Production and drainage of the AH.

Page 4: 3D hydrodynamics and mass transport simulations of ocular

The segmental outflow phenomenon

✓ heterogeneity in the TM outflow facility (Chang et al., 2014): active and

inactive outflow regions

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Questions

✓ how does it affect the AH flow?

✓ does it limit the efficacy of the anti-glaucoma drugs delivery?

Figure 3

The non-uniformity of AH outflow across the

TM in previous fluorescent tracer distribution

study (Chang et al., 2014)

Research objective

✓ to investigate the response of the AH flow to outflow segmentation

and its influence towards treatment of glaucoma

RESEARCH BACKGROUND

TM

Page 5: 3D hydrodynamics and mass transport simulations of ocular

HYPOTHESIS

Segmental outflow : Effects on the ocular drug delivery system

✓ hypothesis: it limits the efficacy of the anti-glaucoma drugs delivery

TM

Figure 4

Hypothesized outflow behavior of the

AH and the ocular drugs.

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Major concerns

‘over-treating’ and ‘under-treating’ conditions

Page 6: 3D hydrodynamics and mass transport simulations of ocular

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METHODS & MATERIALS

The geometry

Figure 5

Illustration of the 3D model in COMSOL MULTIPHYSICS 5.3.

Effective permeability, 𝜅𝑒𝑓𝑓

POSTERIOR CHAMBER

ANTERIOR CHAMBER

Iris

Drainage System Permeability, 𝜿

Drainage System

Page 7: 3D hydrodynamics and mass transport simulations of ocular

Navier-Stokes equation coupled with

Boussinesq Approximation,

𝜌(𝐯 ∙ 𝛻𝐯) = −𝛻𝑝 + 𝜇𝛻2𝐯 + 𝜌0𝐠[1 − 𝛽(𝑇 − 𝑇𝑟𝑒𝑓)]

𝛻 ∙ 𝐯 = 0

Stokes-Brinkmann equation,

𝜇𝛻2𝐯 − 𝛻𝑝 −𝜇

𝜿

Boundary Boundary Conditions

Γ1 AH inlet

Γ2 Non-slip/wall condition

Γ3 Non-slip/wall condition

Γ4 Non-slip/wall condition

Γ5 AH outlet

Γ6 Non-slip/wall condition

Γ1

Γ2

Γ3

Γ4

Γ5

Γ6

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METHODS & MATERIALS

Free and porous media flow

Table 1

Hydraulic boundary conditions.

Page 8: 3D hydrodynamics and mass transport simulations of ocular

METHODS & MATERIALS

Thermal and hydraulic boundary conditions

Figure 6

Thermal and hydraulic boundary conditions employed.

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Page 9: 3D hydrodynamics and mass transport simulations of ocular

METHODS & MATERIALS

The drug transport model

Figure 7

Boundary conditions employed on the drug transport model.

vitreousAC

sclera

lens

TM

iris

tear film

cornea

TM

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Page 10: 3D hydrodynamics and mass transport simulations of ocular

METHODS & MATERIALSThe segmental outflow model

Figure 8

(a ) The spatially defined TM permeability in rectangular function, expressed in terms of θ0 , θ1 and θ2 ;

(b) the schematic diagrams illustrating active outflow regions on the TM at N, NE, E, SE and S.

(b)

(a)

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TM

Page 11: 3D hydrodynamics and mass transport simulations of ocular

METHODS & MATERIALSMaterial properties

Table 2 The thermal, hydraulic and transport properties.

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Ooi and Ng, 2008

Emery et al., 1975

Cicekli, 2003

Lagendijk, 1982

Johnson, 2006

Scott, 1988

Scott, 1988

Ferreira et al., 2014

Ferreira et al., 2014

Ferreira et al., 2014

Page 12: 3D hydrodynamics and mass transport simulations of ocular

METHODS & MATERIALSMaterial properties

Table 3 The baseline values for different model parameters.

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Ooi and Ng, 2008

Ooi and Ng, 2008

Ooi and Ng, 2008

Ooi and Ng, 2008

Ooi and Ng, 2008

Ooi and Ng, 2008

Ooi and Ng, 2008

Ooi and Ng, 2008

Ferreira et al., 2014

Ferreira et al., 2014

Ferreira et al., 2014

Ferreira et al., 2014

Ferreira et al., 2014

Ferreira et al., 2014

Ferreira et al., 2014

(W/(m2.K))

Page 13: 3D hydrodynamics and mass transport simulations of ocular

RESULTS & DISCUSSIONSStanding position

Figure 10

Normalized drug concentration across the plane x = 3.75 mm at (a) 10 minutes; (b) 20 minutes after eye drop

instillation at a standing position.

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Page 14: 3D hydrodynamics and mass transport simulations of ocular

Figure 11

Values of mass transport by

convection, Mconv and mass transport

by diffusion, Mdiff across the active and

non-active region of the TM for the

eye in the standing position, after 10

minutes upon eye drop instillation.

Hypothesis

the direction of the acting gravitational

contributes to the preferential outflow of the

drugs through the bottom half of the eye.

RESULTS & DISCUSSIONSStanding position

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g

active region non-active region

Mconv

Mconv

MdiffMdiff

Page 15: 3D hydrodynamics and mass transport simulations of ocular

Figure 13

Normalized drug concentration across the plane x = 3.75 mm at (a) 10 minutes; (b) 20 minutes after

eye drop instillation at a supine position.

RESULTS & DISCUSSIONSSupine position

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TM

g

Page 16: 3D hydrodynamics and mass transport simulations of ocular

RESULTS & DISCUSSIONSTotal mass transport through the TM by convection & diffusion

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Figure 14

Values of Mconv and Mdiff across the active and non-active region of the TM for the eye in the (a) standing

and (b) supine position, after 10 minutes upon eye drop instillation.

active region non-active regionactive region non-active region

Mconv

Mconv

Mdiff MdiffMconv

Mconv

Mdiff Mdiff

Page 17: 3D hydrodynamics and mass transport simulations of ocular

(a)

(b)

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RESULTS & DISCUSSIONSTotal mass transport through the TM by convection & diffusion

Table 4 Convective and diffusive drug transport through the active and non-active regions of the TM in

(a) the standing position; and (b) the supine position, for the first 15 minutes upon eye drop instillation.

supine position

standing position

Page 18: 3D hydrodynamics and mass transport simulations of ocular

CONCLUSION

✓ the hypothesis of ‘over-treated’ and 'under-treated' conditions are tenable

✓ treatment at a supine position may lead to higher drug efficacy

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Page 19: 3D hydrodynamics and mass transport simulations of ocular

THANK YOU

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