Editorials David
A. Feinberg,
PhD,
MD
Modern Concepts ofBrain Cerebrospinal Fluid Flow’
I
N this
issue
of Radiology,
Poncelet
and
MGH-NMR
co-workers
Center
articles from
of Harvard
by the
Medical
School (1) and Enzmann and Pelc from Stanford Medical School (2) provide exciting new glimpses of brain motion. The findings address a long-standing controversy over the driving force of cerebrospinal fluid (CSF) flow and address the in which
conditions of hydrocephalus flow is impaired. Both articles
display brain velocity with magnetic resonance (MR) phase images. The Haryard study demonstrates a lateral cornpressive velocity component in the thalamic nuclei, while the Stanford study shows
an anterocaudal
motion
of the
cerebellum with the systolic pulse. To present the issues and controversies addressed with these two studies, we must first review prior theories of CSF motion, models of CSF pumps, and earlier MR imaging findings. In 1943,
O’Connell
presented
ful speculations
about
dynamics
on spinal
ments
based
insight-
intracranial tap
CSF measure-
(3):
With each cardiac
systole and during the period before each inspiration there is an increase in the volume of intracranial blood. Now the volume of the cranium cannot increase, and for present purposes the nervous tissues can be regarded as incompressible and undisplaceable. Cerebrospinal fluid must
therefore
be displaced
of the ventricles
and
is diminished nial blood-vessels.
by this .
that the cerebrospinal aided by a vascular
when
the volume
subarachnoid dilation
space
of intracra-
Thus it is believed fluid circulation is pump which drives . .
dynamics,
16.919
Radiology
1992;
Editorials
#{149}
185:630-632
I From the Department of Radiology, New York University Medical Center, 560 First Ave. New York, NY 10016. Received and accepted August 3, 1992. Address reprint requests to the author. 0 RSNA, 1992 See also the articles by Enzmann and Pelc (pp 653-660) and Poncelet et al (pp 645-651) in
this
630
issue.
and
fluid from the ventricles and through the cranial subarachnoid space. There may be a considerable leak back with each stroke of this pump but it is nonetheless considered to be of importance
the transmission
of CSF between
sites at which absorbed
Bering, theory
it is produced
the
through
and
surgical
a
experi-
studies,
duBoulay
argued in favor of a third ventricle pump as the driving force of CSF pulsations and postulated a lateral squeezing of the thalamic nuclei on the third yentricles secondary to brain expansion (5). These two opposing theories of the CSF driving force, brain expansion and choroid plexus expansion, were rooted scientific literature The supporting
since studies,
the however,
had several different sources of experimental error. Intracranial pressure gradients are certainly altered by surgical manipulation of the skull and brain tissue. Pneumoencephalography studies altered brain buoyancy and distorted ventricles by means of air distention. Brain dynamics of interest could not be inferred from distant spinal tap manomeasurements
of CSF
In 1985, a compelling study
from
regions
the
Karolinska
It was demonstrated caudad (antegrade)
all the passageways
systolic
found
pulse
aqueducts
area.
average
The
CSF
normal
demonstrated confirmed ies (10-12).
in
velocity
by its
CSF velocity
patterns
have more recently by several independent Also, circadian variations
been studin
human CSF production have recently been measured with MR velocity imaging (13). CSF motion was not as predicted model,
by the given
third ventricle the MR imaging
the involvement
pump finding
of the lateral
of
ventricles
in ejecting CSF from the brain (9). MR imaging findings also contradicted Bering’s theory, given the compressive mo-
lion of the corpus callosum on the lateral ventricles rather than an outward distention due to choroid plexus expansion. An unexpected finding in our study was an amplified downward
lion
of the brain
stem,
which
to actively drive CSF cisterns and presumably nial cavity. Conservation
was invoked
earlier mo-
appeared
through the basal out of the craof momentum
to explain
the amplified
velocity of the lower brain regions. CSF driving force of the brain stem appears
to be added
volume
expansion
to that
due
This
to net
of the cranial
compartment
The
Institute
It was
(foramen
foramen of Macisterns, while later
vas-
as proposed
by
O’Connell.
MR imaging
demonstrated signal intensity changes of CSF in the aqueduct as a function of cardiac cycle (6). Similarly, the “zebra stripe” method (7) was used at Harvard to detect CSF velocity in the basal cisterns. At this time, Feinberg and Mark (8,9) at the University of California, San Francisco (UCSF), developed a technique of Fourier velocity imaging with which were made the first in vivo measurements of CSF velocity (direction and magnitude) in the cerebral ventrides and passageways. with the arrival of the
brain
the cardiac cycle CSF direction reverses (retrograde), moving into the ventricles and cranial vault. CSF production and flow were measured by multiplying the
cular
pulsation.
of the
caudad, imparting a compressive on all three ventricles and initiat-
ing CSF ejection. that CSF is ejected
in
developed
on animal
encephalography
in the 1950s.
internal
move force
of Monro, aqueduct, gendie) and basal
a neurosurgeon,
based
wave,
ments and claimed that pulsatile expansion of the choroid plexus was the dominant driving force of CSF pulsations (4). Expansion of the choroid plexus within the lateral ventricle should result in a net positive CSF pressure and outward distention of the compliant yentricular walls, differing substantially from an inward compressive force due to brain expansion. To explain pulsatile CSF motion visualized on cine pneumo-
metric Index terms: Brain, hydrocephalus, 10.82 Brain, MR, 13.1214, 15.1214 ‘ Cerebrospinal fluid, MR, 16.1214 . Cerebrospinal fluid, flow
Motion
that
Stanford
study
the dynamics
further
of brain
stem
explains
motion.
sagittally oriented phase images found an anterocaudal motion
cerebellum
and
lower
brain
In
they of the
stem
that
occurs slightly earlier in the cardiac cycle than the caudal motion of the dien-
cephalon readily
and explained
high
brain by timing
stem.
This
is
difference
of systolic arterial pulsation between the anterior and posterior cerebral circulations. The finding is consistent with the slightly earlier onset of CSF caudal motion in the basal cistern than in the aqueduct, initiated by the posterior and
anterior
cerebral
circulations,
respec-
lively. The findings in the Harvard article are important in demonstrating a compressive lateral velocity component at the level of the thalami and third ventricle that is weaker than the caudal velocity component. This is indeed similar to the lateral motion hypothesized by duBoulay, and while it likely contributes to CSF motion at this level, the stronger caudal velocity component covers a larger region of brain parenchyma, affecting all three ventricles. In general, there appears to be a compressive motion of brain parenchyma on the lateral, third, and fourth ventricles. There are some limitations of these
MR imaging
studies.
Phase
imaging
methods, when applied to CSF velocity, are hampered by low spatial resolution, which causes a partial volume effect. Within a voxel containing spins of dif-
ferent velocity, there is destructive interference of the corresponding spin phases (intravoxel incoherent motion), which can greatly reduce the magnitude of the measured velocity. The low spatial resolution on the echo-planar images of the Harvard experiment will suffer such errors in CSF quantitation unless spatial resolution is substantially increased. The Fourier velocity method of UCSF (8) differs substantially from phase imaging by producing a quantita-
live velocity
spectrum.
This
spectrum
separates spin phases of different velocity and is thus immune to the partial volume errors of mixed CSF velocities and brain parenchyma in narrow CSF passageways. The lime-consuming Fourier method, however, is unnecessary for measuring brain parenchyma velocity alone, given its bulk motion and corresponding single spin phase within a
voxel. Accuracy in these MR imaging experiments is determined from velocity resolulion and temporal resolution, the latter being the measurement time in the cardiac cycle. In general, temporal resolution is the lime required for two idenlical gradient pulses that encode a phase shift when spins move parallel to
the direction
of the magnetic
gradient.
Therefore, temporal resolution does not include the lime of spatial phase encoding or signal readout and simply equals 2T + d, where T is the duration of each gradient pulse and d is dead time between the two pulses. The temporal resolulion in the Stanford experiment, 108 msec, however, is more than twice this time, since two consecutive signals are used. The UCSF and Harvard studies used the same spin-echo pulse sequence for velocity encoding, but differed substanlially in temporal resolution (90-120 msec and 45-85 msec, respectively), due to different maximal gradients as discussed below.
Volume
185
#{149} Number
3
Velocity resolution can be defined as the signal phase shift per velocity, 4i/v. The phase shift 4 = k’yT(T + d) Cv, where 4 is phase between -180 and +18f degrees, T and C are the duration and
strength
of the
gradient
pulses,
re-
spectively, and k-y are constants. The above T2 dependence is important in that improvement in temporal resolulion, smaller T, will result in a large loss of velocity resolution unless C is greatly increased (ie, reducing T by haLf requires
more
than
fourfold
increase
in
C). Therefore, the ability to detect subtle timing differences in brain and CSF motion is currently limited by MR imaging
gradient
hardware
rather
than
bio-
logic considerations. The Harvard and Stanford studies were performed with C of 10 mT/m, while the earlier UCSF experiment
used
4 mT/rn,
explaining
its
poorer temporal resolution below tamed with higher mT/rn) provided that are commonly head imaging but
resolution. Temporal 20 msec could be obC values (50-60 by small gradient coils used for echo-planar where fast gradient
switching
not
would
be required,
alley-
ating major technical difficulties. The Harvard experiment also demonstrates the need to isolate brain motion from head motion. Head motion is driven by cardiac pulsations simultaneous with internal brain motion, and so these two velocities are additive in the MR imaging velocity measurement. If the velocity coordinate system can be changed from the external environment to the
moving
coordinate
system
of the
head, then total head motion can be eliminated from the brain velocity measurement. In other words, head velocity must be independently measured and subtracted from brain velocity. The authors
assume
the
scalp,
skull,
and
brain
move together in a rigid fashion in head motion. The skull produces no signal, so head velocity must be measured in the scalp. This correction method appears to have worked well and eliminated what was initially believed to be a net cephalic motion of the cortex during cardiac systole. When considering the Stanford experiment, the cephalic molion of the parietal and frontal lobes might to a large extent be reduced correction for head motion.
In general, intracranial
the pulsatile blood
facilitates
escape
increase
volume
motion. The resulting of brain parenchyma drives CSF out of the downward motion of
with
drives
in brain
compressive force on the ventricles brain, and the the brain stem
of CSF from the cranial
vault. As shown by the Stanford study, the anatomic distribution of expansile arteries and their relative timing of systolic expansion are important determining the directionality and brain motion. All of the
ing velocity
studies
show
factors
in
of CSF MR
uniform
imag-
bulk
motion of large brain regions. While there is perhaps a wafting motion of the cerebral and cerebellar lobes, brain expansion per se, with enlargement of the cerebral hemispheres, has not been demonstrated. MR velocity imaging
studies
consistently
show
large
oscilla-
bidirectional CSF flow, permitting rapid mixing between chambers, as opposed to traditional views of unidireclional flow from the site of production (the choroid plexus) to the site of absorption (the arachnoid villi). Abnormal brain motion in hydrocephalic states is currently being invesligated. A very interesting recent study (14) shows that patients with normalpressure hydrocephalus (NPH) have markedly increased lateral brain molion, while control subjects had weak lateral motion. These findings suggest that abnormal brain motion may be the basis of NPH pathophysiology, as well tory
as providing
a specific
diagnostic
pa-
rameter. It can be postulated that increased lateral brain motion at the level of the third ventricle results in increased CSF pressure, which resists CSF ejection through the foramen of Monro. Alternalively, it can be postulated that at a more distant site, derangement of the caudal motion of the brain stem would reduce and delay the subsequent expulsion of CSF out of the cranial vault, perhaps
blocking
CSF
movement
at the
incisura. With this marked reduction of CSF venting action, pulsatile expansion of the brain’s vascular compartment will not be fully accommodated. A decrease in the global venous drainage would have similar effects. Markedly increased vascular expansile force on brain parenchyma will then be directed centrally toward the ventricular system and, as noted by others (12), an increase in aqueductal CSF velocity may occur. Increased aqueductal CSF flow is consistent with increased ventricular uptake on delayed images of nuclear cisternograms, an accepted diagnostic sign of NPH.
It should
be noted
that
an abnor-
mal inward force on the ventricles differs from the outward force of obstruclive hydrocephalus, as the former would not lead to an immediate expansion of the ventricular system. In either case, however, the increased pressure on periventricular brain parenchyma and blood vessels could cause ischemic damage to the parenchyma and eventually decrease its volume. Evaluation of total brain system dynamics, combining diagnostic parameters of brain motion, CSF velocity, and
vascular
factors
will no doubt
lead to
more specific evaluation of hydrocephalus, useful for guidance and assessment of neurosurgical management. To further define the normal kinematics of brain and CSF motion, MR imaging studies
that
measure
all three
velocity
Radiology
#{149} 631
components,
and
covering
cord,
will likely
the
entire
3.
brain
be needed.
Discrep-
ancies in MR velocity imaging studies may be due to variances in temporal, spatial, and velocity resolutions, as well as findings specific to age-biased popu-
lalions.
4.
In summary, functional MR imof the brain (including these stud-
aging ies of brain and CSF motion, functional mapping of brain activity, and diffusion imaging of acute ischemic events) is re-
shaping
our understanding
physiology
diagnose
and
disease
improving
states.
ability
6. to
#{149}
Enzmann
DR, PeIc
NJ.
7.
Phase-contrast
imaging in measurement of brain Radiology 1992; 185:653-660.
632
Radiology
#{149}
8.
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GH.
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