MODELLING, 3D FLOW ANALYSIS AND
DEPOSITION
3D models of the upper respiratory tract and
tracheo-bronchial tree
The compartmental model together with the 3D
models of the airways are being developed by the
University of Sheffield with the use of CFX5.4
and SIMULINK from MathWorks.
Detailed geometrical information for flow
analysis is highly desirable for a number of
reasons. While idealised geometries have been
used extensively in flow studies of various parts
of the respiratory tract, their strength lies in
understanding the underlying mechanisms of
transport and mixing in the respiratory tract.
Realistic geometries however allow a more
thorough analysis of actual flow patterns and
corresponding deposition in a geometry that is
highly variable from subject to subject. In
addition to this, simulation of flow can be
carried out for different lung pathologies that
will clearly affect the geometry and
mechanical properties of the respiratory tract in
many different ways.
A volume mesh is generated from the results of
the segmentation in the following way:
- Bitmaps stacks containing the results of
the segmentation algorithms are read into
MATLAB
- An isosurface is created around the
segmented regions of the bitmaps
- The isosurface consisting of tessellating
triangles is imported into a 3rd party
software in the form of nodal coordinates
and connectivity. CFX is currently
modifying the import functions to enable
import of the surface mesh directly into
CFX.5.4.
- Boundary nodes are picked within ANSYS
and the volume mesh generated from the
triangular elements making up the
surface.
- The volume mesh and information about the
boundary nodes are imported into
CFX5.4.
This reconstructed geometry can be rendered in
a number of ways for visualisation purposes as
shown in the animations below. The 3D
reconstruction and mesh generation can be carried
out for individual patients.
The animation below shows the reconstruction
of the oro-nasal cavity. Note that the CT scans
were taken at end inspiration during breath hold.
As a result the larynx closes and the resulting
isosurface creates two separate structures. The
oral cavity is not visible in this example due to
the fact that the subjects tongue may be
touching the roof of the oral cavity.

Play
the AVI video | Play the
RealMedia video
The animation below shows an example of a
reconstructed tracheo-bronchial tree down to the
5th generation

Play
the AVI video | Play the
RealMedia video
Steady flow analysis is carried out in the
tracheo-bronchial geometry shown above. A
velocity boundary condition is set at the inlet,
and pressure boundary conditions (of atmospheric
pressure) are set at the outlets. The figures
below show the result of a simulation for
which the inlet velocity (at the top of the
trachea) is set to 0.05ms^-1. The k-ε turbulence model within
CFX5.4 is used to calculate turbulent flow.
Isosurfaces of equal fluid velocity are shown in
the figure on the left while pressure drop is
shown on the right. The deep blue shows surfaces
with lowest velocity and the red shows surfaces
with the highest velocity. The pressure drop down
the tree can be seen to occur as expected. It may
appear curious that the fluid velocity is greater
in the lower branches. This is simply a
consequence of the fact that each vessel from one
bifurcation point to the next tapers
significantly. The method of visualisation
used here enables one to see the different values
of core flow. An important observation can be
made here that in many senses is intuitive but is
encouraging to see borne out by the flow
analysis: the cross-sectional area of the right
main bronchus (on the left of the figure below)
and of the branches orginating from the right
main bronchus are slightly greater than those of
the left main bronchus (on the right of the
figure below) resulting in a larger proportion of
the flow being directed down the right lung. The
consequences of asymmetry in the airways are
clearly demonstrated in this realistic asymmetric
geometry; in reality it is indeed the right lung
that is known to be larger and receive greater
ventilation.

Click
here for full-sized image
An example of simulated expiratory flow
below shows results for such a simulation with
the pressure at the opening of the trachea set to
atmospheric and fluid velocity boundary
conditions at each ending set to 0.05 ms-1. Again
a k-ε turbulence model
is used to carry out the flow analysis. The
velocity at each ending need not be identical.
Indeed in the final compartmental model this 3D
component will be coupled to the peripheral
airways compartment resulting in different
pressures at these boundaries.

Click
here for full-sized image
While the boundary conditions used here are
not realistic, integration of this model into the
compartmental framework will take into account
boundary conditions at the interfaces with other
compartments and therefore more realistic
pressures here.
The results for a transient flow analysis can
be seen in the animation below. Here the velocity
at the top of the trachea varies sinusoidally as
a function of time, with peak inspiratory
velocity of 0.5 ms^-1 and peak expiratory
velocity of -0.5 ms^-1 over a period of 4
seconds. The animation shows massless particles
in the resulting transient flow field.

Play the
AVI video | Play the
RealMedia video
Device models
Several types of delivery devices and spacers
or holding chambers will be considered, ranging
from ventilator delivered nitric oxide through to
pressurised metered dose and dry powder inhalers
from Aventis Pharma. The following section
concentrates on flow and particle deposition
analysis in the E-haler - a multi-capsule,
unit-dose, dry powder inhaler from Aventis
Pharma. The CAD representation is provided by
Aventis Pharma and the flow analysis has been
carried out at CFX.
There are a number of issues in the
fluid-dynamic performance of delivery devices
which manufacturers face. These include:
- flow rate/pressure drop characteristics
- residence time distribution
- particle trajectories
- deposition and impaction
The CFD models which are being employed and
developed within COPHIT provide detailed
information to the designer on the flow behaviour
within the devices. The CFX-5 software is used
for the flow simulations.
Figure 1 shows the original CAD model of the
Aventis Pharma E-haler, whilst Figure 2 shows the
surface mesh created in CFX-5. CFX-5 uses
mixed-element meshes which can comprise
tetrahedra, hexahedra, pyramids and prisms.
Inflation of the elements adjacent to the walls
of a device allows accurate solution of the flow
in the boundary layers.
In Figure 3, streamlines coloured by the local
flow speed reveal the complex flow patterns
within the device. The flow is driven by the
difference in pressure between the air inlets and
the mouthpiece, which can be made to vary with
time to replicate real inhalation profiles.
Figures 4.1 to 4.4 are plots of the
trajectories of typical drug particles of
different sizes. Smaller particles are seen to
follow the air flow more closely than larger
ones, which due to their inertia, tend to spiral
out towards the outer wall of the device.
Pharmacokinetic models for drug uptake and
clearance
Good pharmacokinetic models of drug uptake are
needed to calculate the concentration of drug in
the blood after it has passed through the lung
and the subsequent clearance from the body.
Pursuit of a satisfactory biokinetics model (at
the University of Shefffield) to describe the
uptake of drugs at the alveolar membrane and via
the oral and infused route has resulted in
the formulation of a simplistic, but robust
three-compartment model. This is designed to be
the simplest system that can accommodate the
parameters of pharmaceutical profiles required
for medical approval (eg. FDA). These are shown
below:
Typical
pharmacokinetic parameters
Elimination half-life
Area under curve
Plasma clearance
Volume of distribution
Distribution half-life
Total body clearance |
Input - Infusion,
oral, inhaled
Output -
Plasma concentration, urine, faecal
samples
|
The pharmacokinetic model is depicted below:
- A first order description of
reaction processes based on Ficks law has
been employed.
- The simplicity of the model ensures that
all relevant rate constants can be
uniquely determined.
- Data has been collected on some well
characterised pharmaceuticals (eg.
Iloprost) in order to test and validate
the model. It has demonstrated
satisfactory description of
pharmacokinetic data (ie. generally to
within 10% - see table...)
| ILOPROST |
Intravenous Dose (ng/kg/min) |
Model |
| |
1
2
3 |
3 ng/kg/min |
Steady state plasma conc (ng/L)
Vol. of distribution (ml/kg)
Half life of distribution (min)
Half life of elimination (min)
Total body clearance (ml/min/kg)
|
46
81
135
679
839
3.8
4
2.8
20.1
31
26.0
21
24
20.1
|
127
800
3
29
19
|
Pharmaceutical data from
. Grant
et al. Drugs 43(6);889-924 1992
- The limitations of this biokinetic model
need to be established, and this is being
pursued by monitoring its ability to cope
with an increasingly wide selection of
pharmaceuticals.
- The model has been constructed in
Simulink to comply with the wider
programming requirements of COPHIT.
- Systemic biokinetics and alveolar
exchange:
- The model has demonstrated
satisfactory description of systemic
biokinetics. Attention must now be
focused on drug transfer across the
alveolar membrane since this is the
primary feed to the systemic biokinetic
model.
|