Ciência/Science
CEREBROSPINAL FLUID DRAINAGE DEVICES:
EXPERIMENTAL CARACTERIZATION
C. Bima,
ABSTRACT
a
M. Pinotti ,
J. R. Camilob,
A. L. Masetb,
S. S. Mansurc,
and E. D. R Vieirac
a
UFMG – Universidade Fed. de Minas Gerais
Av. Antonio Carlos, 6627,
Belo Horizonte, Minas Gerais
b
Ventura Biomédica
Av. Francisco Chagas de Oliveira, 1100,
São José do Rio Preto, São Paulo
c
UNESP – Ilha Solteira Av. Brasil Centro, 56,
Ilha Solteira, São Paulo
Hydrocephalus is a pathophysiology due to the excess of cerebrospinal fluid
in the brain ventricles and it can be caused by congenital defects, brain
abnormalities, tumors, inflammations, infections, intracranial hemorrhage
and others. Hydrocephalus can be followed by significant rise of
intraventricular pressure due to the excess of production of cerebrospinal
fluid over the absorption, resulting in a weakening of intellectual functions,
serious neurological damage (decreased movement, sensation and
functions), critical physical disabilities and even death. A procedure for
treatment involves the placement of a ventricular catheter into the cerebral
ventricles to divert/drain the cerebrospinal fluid flow to a bag outside of the
patient body – provisory treatment known as external ventricular drainage
(EVD). Another option is the permanent treatment, internal ventricular
drainage (IVD), promoting the cerebrospinal fluid drainage to other body
cavity, being more commonly the abdominal cavity. In both cases, EVD
and IVD, it is necessary to use of some type of neurological valve in order
to control the flow of cerebrospinal fluid. In the present work is proposed
an experimental procedure to test the hydrodynamic behavior of a complete
drainage system, or parts of them, in order to verify its performance when
subjected to pressure gradients found in the human body. Results show that
the method is well adapted to quantify the pressure drop in neurological
systems.
Received: October 25, 2013
Revised: November 20, 2013
Accepted: December 30, 2013
Keywords: Hydrocephalus, Cerebrospinal fluid, Ventricular drainage.
NOMENCLATURE
D
f
fexp
fL
g
Ke
Kv
L
Re
V
z
pipe diameter, m
friction factor for pipes
experimental friction factor
Hagen-Poiseuille friction factor
local gravitational acceleration, m/s2
loss pressure coefficient for pipe entrance
loss pressure coefficient for valves
pipe lenght, m
Reynolds number
mean flow velocity, m/s
vertical coordinate in upward, m
stable ionic composition. About 20% of all CSF of
the body is found in ventricles – intracerebral
spaces – and in foramens – very small channels
connecting the ventricles –, while the other 80% is
located in areas outside the brain, in the brain
surroundings and in the spinal cord, as depicted in
Figure 1.
Greek symbols
α
ρ
µ
kinetic energy coefficient,
water density, kg/m3,
water viscosity, N s/m2,
INTRODUCTION
Cerebrospinal fluid, also known as CSF, is an
aqueous colorless odorless fluid, with a low
concentration of cells and proteins. According to
Adam et al. (2001), the cerebrospinal fluid fills all
internal and external spaces of the brain showing a
Figure 1. Structure of the brain and spinal cord in the
human body (Adapted from Waxman, 2010).
According to Adam et al. (2001) and
Irani (2009), the main functions of the cerebrospinal
fluid are to protect the brain and the spinal cord from
mechanical shocks, and to regulate the ionic
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Bim, et al. Cerebrospinal Fluid Dreinage …
composition. CFS also plays an important role in the
biological protection of the nervous system,
distributing nutrients, proteins and agents of defense
against infections and carries away metabolites
residues.
Healthy adult presents about 150 ml of CSF
total volume flowing throughout its body and a
continuous daily production rate between 400 and
500 ml (Carlotti Jr, et al., 1998).
In accord to Camilo (2005), the cerebrospinal
fluid is continually produced by a tissue called the
choroid plexus situated in the lateral cerebral
ventricles.
Most of the cerebrospinal fluid is
produced by first and second ventricle (called lateral
ventricles – one in each hemisphere of the brain). The
Fig. 2 illustrates the path of the cerebrospinal fluid.
After being produced and fill the lateral ventricles,
CFS is conducted to the third ventricle through a
small aperture called foramen of Monro (a very small
brain orifice). Thus, the third ventricle (single cavity
situated in the center of the brain) is filled with liquid
deposited and joins a small volume produced locally.
Continuing its path, CFS flows into the aqueduct of
Sylvius to the fourth ventricle (small cavity on the
back of the brain). The fourth ventricle also has a
very low account of choroid plexus tissues.
Donwstream the fourth ventricle, all CFS produced in
the brain is drained out through Lushka and
Magendie foramens. Following, the CSF bathes the
outer surface of the brain (with its several cavities)
and spinal cord. After this long way, from the
interior to the surface of the brain, the fluid is
absorbed in small structures called arachnoid
granulations (venous absorption).
Figure 2. Path of Cerebrospinal Fluid (Adapted
from Rohkamm, 2004).
the excess of cerebrospinal fluid in brain ventricles
(Souza et al., 2007).
Hydrocephalus is a pathophisiology that affects
both adults and childrens, and it can be caused by
congenital malformations, brain anomalies, tumors,
inflammations, infections, encephalitis, intracranial
hemorrhages, subdural or epidural hematoma,
abscess, traumatisms and others (Camilo, 2005).
The hydrocephalus may result in a weakening of
intellectual functions, serious neurological damage
(decreased movement, sensation and functions),
critical physical disabilities and even death.
After the diagnosis of hydrocephalus, there are
some surgical options for treatment. One of those
procedures involves the placement of a ventricular
catheter into the cerebral ventricles to divert/drain the
cerebrospinal fluid flow to a bag outside of the
body – provisory treatment known as external
ventricular drainage (EVD). Another option is the
permanent treatment, internal ventricular drainage
(IVD) that promotes the cerebrospinal fluid drainage
to another body cavity, being more commonly the
abdominal cavity. In both cases, EVD and IVD, it is
necessary to use a neurological valve to control the
flow of cerebrospinal fluid in acceptable levels. An
excessive drainage (or over drainage) can occur after
shunting, but it must be avoided because only a few
seconds in this adverse condition can produce an
irreversible cerebral damage in the patient (Kremeer
et al. 1994).
According to Sood, et al. (1999), since 1960,
when the shunt (drainage procedure of cerebrospinal
fluid) was created, the mortality rates by
hydrocephalus suffered a decline of 54% to only 5%,
while the loss of brain skills of patients decreased
from 62% to 30%.
In the present work a test procedure is proposed
for hydrodynamic characterization of neurological
valves. Additionally, a study of a one-way
neurological valve, known as membrane valve,
designed to work outside the body – external
ventricular drainage – is made. Since the hydraulic
resistance influences directly the valve performance,
it is necessary to study its system behavior as
submitted to different pressure gradients. In this way,
it is possible to determine the pressure loss
coefficients of the valve, in order to evaluate its
performance in a possible application as drainage
system.
EXPERIMENTAL APPARATUS
Normally, there is a natural balance between
production and absorption of cerebrospinal fluid. In
other words, the same volume which is produced in
one part of the brain should match that is absorbed
elsewhere. The hydrocephalus occurs when there is a
disturbance in cerebral spinal dynamics (lock in your
flows, decreased ability to absorb or overproduction)
implying, in general, the accumulation of CSF in the
ventricles. The hydrocephalus can be followed by
significant rise of intracerebral pressure (ICP) due to
60
There are an extensive number of publications
available in technical literature showing several
experimental apparatus for testing neurological
valves, from very sophisticated to simple conceptions
that provide reliable data.
Drake and SainteRose (1994) show several conceptions of devices to
performing test in valves shunts utilizing infusion
pumps and electronic measurements of pressure and
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Ciência/Science
volumetric flow. In many other works, the
construction details of test devices of valves for CSF
drainage are not available, as examples, Horton and
Pollay (1990), Sood et al. (1998) and Kremeer et
al. (1994). Infusion pumps are precise pumps of
positive displacement. A positive displacement
devices remain constant the flow rate. Positive
displacement infusion pumps show an extensive
utilization in neurological valves tests, but the ICP
produced by cerebral ventricles produces a CSF flow
dynamics more close than a non positive
displacement pump than a positive displacement
pump. Mariotte bottle is an ingenious device which
remains the exit pressure constant regardless of the
level of the liquid in the delivery vessel. Utilization
of Mariotte siphons is very adequate for testing
neurological valves since the inlet pressure remain
constant during all the runtime.
The Fig. 3 depicts a simplified sketch of the
experimental apparatus utilized in this work, which
consists of: a Mariotte bottle (A) made in Plexiglas,
adequately placed on a digital balance (B) – Marte
balance model AS 2000 – with ± 0.005 g of accuracy
and measurement up to 2000 g. An electronic digital
chronometer made by Cronobio model SW2018 with
an uncertain of ± 0.01 s directly coupled in the
balance permits to determine the instantaneous mass
flow rate. The liquid inside the Mariotte bottle is
continuously drained to the reservoir (D) through a
stainless steel tube with 2.5 mm of internal diameter
and 4.0 m of length, where the valve under study (F)
is located in one of its ends. Throughout the process
of data acquisition the temperature of the fluid is
continually measured by means of a digital
thermometer (E) Minipa MT 40IA with ±0.5oC of
dial indicator uncertain with a range from 50oC to
750oC. A constant flow rate is produced by using the
Mariotte bottle, since the exit pressure not changes,
regardless the level variations of liquid inside the
bottle.
Experimental uncertainties have been properly
estimated, in order to provide reliable data. The
balance has been evaluated using ABNT standard
mass. Stainless steel tube used in this work has been
produced for pharmaceutical industry for hypodermic
needles production.
Bim, et al. Cerebrospinal Fluid Dreinage …
RESULTS
Initially tests were performed out using several
pressure gradients equivalent to (ICP), ranging from
40 to 240 mmH2O, without the valve. Thus, it was
measured the pressure loss of the rigid circular pipe
and, consequently, the friction factor (fexp) for the
tube can be experimentally determined, using the
energy equation for pressure loss of pipes.
g (∆z ) −
V 2
L V 2
V 2
= f exp
+ Ke
2
2
D 2
(1)
For laminar flow, friction factor of pipes (fL)
can be calculated by Hagen-Poiseuille formulation
for a fully developed velocity profile in laminar
steady flow of a Newtonian fluid.
fL =
64
64 µ
=
Re ρ V D
(2)
The results are shown in Fig. 4, where the red
line represents the friction factor of the tube
experimentally determined (fexp) and the blue line
represents the friction factor in accord to HagenPoiseuille formulation – Eq. (2). The graphic shows a
significant difference between the friction factors
obtained by means of the two equations. This is due
to the fact of Eq. (2) be only valid for steady laminar
flow (Reynolds numbers less than 2100) of
Newtonian fluids having a fully developed velocity
profile (Fox and McDonald, 1995). Thus, it was
chosen to work with the experimental friction factor
(fexp).
f
f exp
fL
Re
Figure 4. Friction factor of a pipe in function of Re.
Once determined the coefficient of friction of
the tube (fexp), a valve neurological can be coupled in
the free end of the stainless steel tube. In this case,
Eq. (1) must be rewritten in order to consider the
pressure drop produced by the neurological valve.
g (∆z ) −
Figure 3. Schematic of experimental apparatus (Bim
et al., 2010).
V2
L V2
V2
V2
= f exp
+ Ke
+ KV
2
D 2
2
2
(3)
Results for pressure gradients from 40 up to
240 mmH2O for a typical membrane valve is shown
in Fig. 5.
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Bim, et al. Cerebrospinal Fluid Dreinage …
Figure 5. Loss of pressure coefficient for a valve.
CONCLUSIONS
Humans are estimated to produce continually
about 0.5 ml/kg per hour, or approximately 500 ml of
CSF each day. A discrepancy in CSF production and
absorption cumulates an excess of fluid in the brain.
Elevated levels of CSF are associated with traumatic
brain injury, meninge infections (meningitis) and a
pediatric disease known as hydrocephalus. In all of
these cases, an increase fluid pressure (intracranial
pressure) can be observed resulting in permanent
brain injury and death.
If diagnosis of hydrocephalus has been obtained
there are rarely options other than surgery for
treatment. Most surgeons use various types of
systems called shunts to channel the fluid from the
ventricles to other sites in the body such as the
abdominal cavity (internal shunts). CSF drainage can
be realized also for an external reservoir (external
shunts).
In 1999, Aschoff et al. (1999) show 127
different types of neurological valves commercially
available, conceived since 1949, and more than other
70 models in different developing stages. All internal
and external drainage systems (and each individual
component) could be intensively tested in order to
determine its hydrodynamic behavior. In this work, a
new procedure for neurological valve test has been
proposed,
allowing
comparing
hydraulic
characteristics of shunt parts or of a complete system.
The individual measurement of pressure drop in all
the parts of a drainage shunt is very important for a
detailed engineering project of a neurological valve.
Aschoff, A., Kremer, P., Hashemi, B., and
Kunze, S., 1999, The Scientific History of
Hydrocephalus and its Treatment, Neurosurgical
Review, Vol. 22, pp. 67-93.
Bim, C., Mansur, S. S., Vieira, E. D. R.,
Camilo, J. R., and Maset, A. L., 2011, Study about
Duck Bill Check Valves in Neurological
Applications, in: COBEM 2011 – 21th Brazilian
Congress of Mechanical Engineering, Natal, RN.
Camilo, J. R, 2005, Simulação Hidrodinâmica e
Caracterização Experimental de Mecanismos Antisifão em Sistemas de Drenagem Externa de Líquido
Cefalorraquidiano, Master Thesis, Universidade
Estadual de São Paulo – UNESP, Ilha Solteira, SP.
(in Portuguese)
Carlotti Jr, C. G., Colli, B. O., and Dias, L. A.
A., 1998, Hipertensão Intracraniana, in: Simpósio
Medicina Intensiva, Ribeirão Preto, SP. (in
Portuguese)
Drake, J. M., and Sainte-Rose, C., 1994, The
Shunt book, Blackwell Science, 228 p.
Fox, R. W., McDonald, A. T., and Pritchard, P.
J., 1995, Introduction to Fluid Mechanics, 6th
Edition, John Wiley.
Horton, H., and Pollay, M. P., 1990, Fluid Flow
Performance of a New Siphon-control Device for
Ventricular Shunts, Journal of Neurosurgical, Vol.
72, pp. 926-932
Irani, D. N., 2009, Cerebrospinal Fluid in
Clinical Practice, Elsevier.
Kremeer, P., Aschoff, A., and Kunze, S., 1994,
Risks of Using Siphon-Reducting Devices, Child’s
Nervous System, Vol. 10, pp. 231-235.
Rohkamm, R., 2004, Color Atlas of Neurology,
Thieme.
Sood, S., Canady, A. I., and Ham, S. D., 1999,
Adjustable Antisiphon Shunt, Child’s Nervous
System, Vol. 15, pp. 246-249.
Souza, H.,
Doutel, F.,
Borge, C.
A.,
Azevedo, R. G., Walter, R., and Ribeiro, C. H., 2007,
Hidrocefalia Aguda Essencial, Arquivos Brasileiros
de Neurocirurgia, Vol. 26, No. 2, pp. 53-59. (in
Portuguese)
Waxman, S. B., 2010, Clinical Neuroanatomy,
26th Edition, McGraw-Hill.
ACKNOWLEDGEMENTS
This work has been developed by FAPESP,
CNPq and FUNDUNESP grants. VENTURA
BIOMÉDICA supplied all materials to manufacturing
the test apparatus and provides funding for this work.
REFERENCES
Adam, P., Táborský, L., Sobek, O., Hildebrand,
T., Kelbich, P., Prucha, M., and Hyánek, J., 2001,
Cerebrospinal fluid, Academic Press.
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