Robert K. Zeman, MD Wendelin S. Hayes, DO Cirrelda J. Cooper, MD
#{149} William #{149} Paul
Cavitation Part
effects
lithotripsy
can
cally
visible
Davros, L. Cattau, M. Silverman,
Effects
II#{149} Clinical
Cavitation
during produce
The
fragmentation Microbubble
re-
in 31 of forma-
tion in the liver correlated with transient hepatocellular damage (as indicated by a twofold rise in serum transaminase levels) immediately after seven of 10 treatments. Advancing the focal volume of the deeper
(placing the stone point of the focal useful strategy for cavitation effects, be responsible for tocellular damage.
into
during
C
biliary sonographi-
microbubbles.
lithotriptor
terms:
the
patient
at the proximal zone) may be a reducing hepatic which appear to temporary hepa-
Gallbladder, 762.1299
#{149} Lithotripsy,
interventional
Radiology
1990;
calculi,
762.289
procedure. 762.1299
177:163-166
is increasingly clear that cavitation contributes to stone fragmentation (1,2) and perhaps even to tissue injumy (3), clinical data linking stone fragmentation, tissue injury, and the presence of sonogmaphically visible microbubbles during lithotnipsy are sparse. To obtain such data, sonographic evidence of the location, intensity, and power level at onset of it
cavitation bbes were outcome treatments.
MATERIALS
AND
in
during
The
13 men
years. two
for
more
three than
stone
mm
for
From the Departments of Radiology (R.K.Z., W.J.D., JAG., B.S.G., W.S.H., S.C.H., CC., P.M.S.) and Medicine, Gastroenterology Division (E.L.C.), Georgetown University Medical Center, 3800 Reservoir Rd NW, Washington, DC 20007. From the 1989 RSNA scientific assembly. Received February 5, 1990; revision requested March 16; revision received April 4; accepted April 17. Address reprint requests to I
in age
stone,
three
diameters stones
4
22 to 71 initially
ranged
more
in-
from
The
than
R.K.Z. 1990 by Zeman et al (pp 157et al (pp 147-151), and Shapiro (pp 153-156) in this issue.
and
treatment. probe
top)
real-time
diame-
is also position
the for
imaging
is used
22,
left the
used. was
The used
posterior supine
an
for two,
for
taken
to 1ev-
patient
data.
and
recorded.
the
procedure
were
used
The
formation
targetable Real-time
procedure
were
during
and
to gener-
locations
of mi-
(subcutaneous
tis-
bile, vessels, and were recorded.
bubbles,
2
city, city, city 5 =
moderate
3 = 4 = with
others) and Microbubble
tar-
25 treat-
(to table
microbubble
echogeni-
microbubble
persistent
shadowing
beyond was divided microbubble
We called this the If no microbubble maximum
echogeni-
and
prolonged
30 seconds). by the power formation
“cavitation formation
energy
was
The level appeared.
quotient.” occurred,
achieved
used
at
as the
for
that
denominator
for
the quotient calculation. The cavitation quotient differs from the microbubble intensity index used in our previous in vitro work in that it is depen-
dent
on the
power
increases
during
level in
fact
that
were
proapplied
the quotient stones
re-
exposed
level
at
ex-
power
level
(low
to long
cavitation onset) may undergo different degrees of fragmentation than stones posed to shorter periods of cavitation (high
of cavitation
(1). Because
power
the treatment, the
periods
de-
faint
=
intense microbubble echogeniintermittent shadowing, and intense microbubble echogenicity
which
flects
lateral
and
entire
of videotapes
gnessive
during
oblique for
mo-
out-line left
by
unless no was visible.
images
cavitation
the
during
viewing
tolerated
of the
treatment
presto 7.5 as a
unit has sector-scan
imaging
tangential
treatment ments,
1 to 9. The
A 3.5- or 5.0-MHz for
cubitus
be
shock waves on fragment
grade
performed with the Plus (Siemens Medical
mechanical probe that
to let de-
the
could
dissipation
7 to 45 in
suspend-
case
el that
with
cumula-
from 5 mm
was
in each
intensity was graded by consensus of two observers (R.K.Z., W.J.D.) who did not know treatment outcome (1 no micro-
22 treatments
stones.
Treatment
dissipate power
crobubble
were and
was to target the more than 5
bnis settle and microbubbles assist in targeting. The highest
ate
10 treatments
stones,
linear scale from in-line, 3.5-MHz ultrasound (US) geting
diameter.
Notes
16 women
treatments
for one or
tive
in
strategy on fragment
ed up to 5 minutes
review
at our
were
ranging
performed
initial
operation
patients
Eighteen
for
mm
to release excessive hair shaved to en-
contact.
treatment stone
freeze-frame
29 patients
the
of lithotnipton
stitution. and
good
The largest
US
METHODS
of 50 treatments
performed
months
sure
sues, liver, its intensity
Systems, Iselin, NJ). The “overhead dule” used for treatment generates sures from 220 to 750 bar (2.2 X i0 x iO Pa). Power levels are expressed
161), Khouri and Winsberg
MD
contact pressure was required shock waves. Patients with over the coupling site were
4,000 stone
manifesting as microbubcorrelated with the clinical of 50 gallstone lithotnipsy
Lithotnipsy was Siemens Lithostar
RSNA.
S. Garra,
was achieved by progressively increasing the setting at intervals of 50 shock waves. Treatment was extended to a maximum of
ten.
See also the articles
#{149} Brian
Lithotripsy
effects produced by shock waves occur in a variety of media (1). In the laboratory, stones surrounded by fluid capable of supporting cavitation appear to fragment more thoroughly than stones embedded in a solid medium (1). Although
A total
Gallbladder,
RN MD
AVITATION
were Index
PhD #{149} Jo Anne Goldberg, Jr, MD #{149} Steven C. Horii, MD
Observations’
lationship between microbubble formation and clinical outcome of gallstone lithotripsy performed with a commercial lithotriptor was studied in 50 treatments in 29 patients. Microbubble formation in bile was a useful predictor of successful stone 34 treatments.
J.
#{149} Edward
at cavitation
power
onset).
A
the
semierect for one. The largest coupling surface that was anatomically possible was used. A minimum of 9 lb (4.1 kg) of
Abbreviation: oxaloacetic
SGOT
serum
glutamic
transaminase.
163
large cavitation quotient microbubble formation tively
low
power
implies
violent
occurring
levels,
at rela-
while
a small
quotient implies meager bubble formation despite relatively high power levels. The cavitation quotient for bile was correlated with the occurrence of stone fragmentation. A 50% reduction in stone diameter was required to label fragmentation successful. A hepatic cavitation quotient was also calculated when microbub-
a.
bles
Figure
were
seen
to accumulate
parenchyma. tient was
The hepatic correlated with
in
glutamic
serum
in
the
liver
cavitation quothe difference
oxaloacetic
transami-
nase (SCOT) levels immediately before and 2 hours after lithotnipsy. Subjective procedural observations were also recorded as they related to attempts to manipulate cavitation effects.
RESULTS Successful fragmentation (50% reduction in stone size) occurred in 34 of 50 treatments. Of the 16 treatments with unsuccessful fragmentation, five produced no fragmentation. Because the treatments were consistently structured to target the largest stone and success was determined by a 50% reduction in the size of that stone, there was no significant difference in stone burden for the fragmentation group versus the group with unsuccessful fragmentation. The mean number of stones was 3.0 ± 2.0 in the fragmentation group and 3.1 ± 1.9 in the unsuccessful fragmentation group. Similarly, the cumulative diameters of the stones in each group did not differ significantly (23 mm
±
8.8
vs
24
mm
±
11,
b.
ing
1.
Cavitation
lithotnipsy
illustrate
c.
the rapid
gallbladder. development
sipated. rolling
A small fragment the patient and
(arrow) separating
has the
time
ranging
utes.
No
were
seen
from
40 seconds
residual
in the liver
patients. An elevation el to twice the baseline in
seven
of
of these
of the value
SCOT 1evwas seen
10 treatments
that
one
of 40. In Figure
tation
quotient
5, the hepatic
is plotted
in SCOT
Figure
gree
of microbubble
SCOT
level
with
a coefficient suggests
shock
and
the
formation
164
#{149} Radiology
by
damage.
In seven
2 weeks
after
three, bles
of the eight
were seen in hepatic patients (Fig 6). In all
concomitant were
between
hepatic
present.
A clear
the hepatic
focus
microbubbles
traveled
images
showed
entered
as a parabolic
(arrow)
wave
path
bubbles
appeared
became
barely
shock
wave
forming
to the
a dense along
visible was
each
These
shock
by the time
of
the
in the gallbladder. with
shock
band
wave
and
the next
applied.
QUOTIENT
CAVITATION
Figure 3. cavitation tionship
RANGE
Histogram displays gallbladder quotient ranges and their relato fragmentation (FRAG).
connection
of bubbles
that
the
shows
microbub-
and the vessel was identified in two of the three cases. On the basis of their distribution, the vessels were branches of the portal vein in two cases and of the hepatic vein in one case. Review of
videotape
confined
US image
patients
lithotnipsy.
Microbubbles vessels in three
Cavitation
de-
with elevated SCOT values, the values returned to within 10 U of baseline by
ments and sludge. They could be distinguished because, with pauses in treatment, microbubbles tend to rise to the nondependent surface of the gallbladder and then collapse, losing their transient shadow. As they dissipate, bubbles do not form an echogenic layer along the dependent portion of the gallbladder, whereas fragments do. The intensity of microbubble formation and the power level at onset were useful predictors of fragmentation. The cavitation quotient was less than 1.5 in all patients in whom successful fragmentation was not achieved (Fig 3). In patients with successful fragmentation, a broad range of quotients existed, from 0.1 to 5.0. Microbubbles appeared as bright “flashes” within bile, lasting less than 1 second in 29 treatments. In
confirmed
in the
were
frag-
was
of .79.
that
liver and whether it occurs early in the treatment (at low power) are predictive of the extent of transient hepatocellulai
stone
This
The in the
the 36 treatments in which microbubbles occurred, 32 showed bubbles prior to any significant gallstone fragmentation. In four treatments, microbubbles
with
path.
microbubbles
the
before
2.
wave
cavi-
against
values
showed
along
stone.
showed
hepatic microbubbles. In the 40 treatments with no visible hepatic microbubbles, a rise in the SCOT level to twice the baseline value was seen in
correlation
present
the
changes
of any
This
Of
off
to 6 mm-
sonographic
after lithotnipsy for all treatments. quotient correlated with the rise
formation.
been chipped two fragments.
of 50 shock gives rise to indisthe cloud has dis-
seven treatments, progressive buildup of bubbles was seen. The dissipation time of these bubbles ranged from 30 seconds to 3 minutes. Microbubbles were identified within the liver panenchyma during 10 treatments (Fig 4). Temporarily stopping the treatment caused microbubbles to disappear in all 10, with the dissipation
Microbubble formation within the gallbladder was identified in 31 of the 34 successful treatments (Figs 1, 2). Of the 16 unsuccessful treatments, 11
no microbubble
Sequential US images of the gallbladder dunand dissipation of microbubbles. (a) Baseline
image shows a solitary stone targeted in the crosshains. (b) After application waves (1 minute), a cloud of microbubbles (arrow) obscures the stone and tinct shadowing. (c) One minute later (after stopping of the shock waves),
difference
respectively).
within the
vessel,
cluster
once
the
they
in the di-
rection of flow. The bubbles appeared to be tightly clustered as they entered the vessel but spread to fill the vessel as they moved downstream. The rate of bubble travel ranged between 5 and 10
mm per ‘/30-second video frame. After approximately the 40th treatment, concerns that cavitation may be related to temporary hepatocellular injury
and
attenuate attempts
was
found
that
hepatic
microbubbles
may
the shock waves resulted to limit hepatic cavitation.
that
cavitation
in It
in the liver
could be reduced by stopping the treatment, changing the shock wave path, or moving the proximal edge of the focal zone deeper into the patient (ie, placing the stone at the proximal point
October
1990
150
I y=
I R=0.79
-3.9732+40.5781x
a)
U
100
-
-
-
U)
-
0
cn
El-
--
--. -
I-
0 0
.
U)
a.
b.
v
(
A
1’
c.
Figure 4. Microbubble development in the liver, shown on sequential US images. (a) Baseline view shows a solitary stone in the gallbladder. The liver is in the near field and shows no abnormality. (b) After application of 1,000 shock waves, progressive microbubble formation (curved arrow) is seen in the liver. A dense acoustic shadow is cast across the gallbladden (gb), which is filled with sludge, fragments, and cavitation bubbles. (c) After stopping of the shock waves, the hepatic microbubbles dissipated oven 3 minutes.
-
-
-
-
-
0
1
Cavitation Figure rise
5.
Quotient
The relationship
in SGOT
level
and
hepatic
strategy
zone)
reduced
formation eliminated
(Fig
7). The
hepatic
during
two
latter
burden by performing and evaluating success
microbubbbe
treatments
and
it in one.
DISCUSSION It was shown previously that acoustic cavitation may be produced by extracorporeal shock wave lithotnipsy (4). Our work shows that microbubbles resuiting
from
cavitation
are
readily
seen
at neal-time US during clinical gallstone lithotnipsy. Their presence may be noted not only in bile but also in soft tissue such as liven Limited stone size and
previously predictors Our work absence of
been suggested as the only of successful lithotnipsy (5). suggests that the presence or microbubbles in bile during
lithotnipsy
marker
may
that
mentation.
Volume
parenchyma. number have
We
177
be used “factored
#{149} Number
out” 1
majority
of
of our
can be seen
(curved
treatments.
rising
away
arrow),
but spread paraimages was ‘to
The
bubbles
from
the bile-
cavitation
occurs.
50% fragmentation of the largest targeted stone. Although the presence of bubbles does not uniformly predict that stones will break, successful pulvenization is far less likely if intense microbubbles do not form at relatively low power. It should be noted that both in the laboratory and in our clinical expenience some stones broke in the absence of obvious microbubbles (1). Pul-
stone
interface
Once
significant
venization appears less complete, however, when cavitation is not optimized
time sonographic observation will show that bubbles give rise to a rapid sequence of events: a bright echogenic flash that disperses centrifugally and disappears prior to the arrival of the
(1,2). During clinical lithotripsy, ous echoes are seen within recently suggested on the
tro data
that
gallstone
microbubbles
fragments
(1,6).
numerbile. It was basis of in vi-
may This
mimic did
not
of frag-
pose a problem in the calculation of the cavitation quotient, in that microbubble intensity was graded prior to signif-
stone
icant
as an important
can be predictive
our treatments on the basis
the
cavitation
quotient.
Figure 6. Microbubbles within hepatic vessels. The sequence of US images shows a collection of microbubbles in the liver which escape into a branch of the portal vein (straight arrows). The bubbles at first are a dense focus as they enter the vessel bolically to fill the vessel with low-intensity echoes. The direction of flow is to the reader’s left. (The time interval between second.)
of the focal
(Liver)
between
stone
fragmentation
in the
vast
when
numbers
of fragments
and sludge exist within the gallbladder, differentiation of microbubbles is difficult but not impossible. If one temporanily suspends shock wave generation, microbubbles are seen to rise, while the fragments “rain down” to form a layer along the dependent sun-
face of the gallbladder.
next
shock
wave.
Careful
This
was
seen
real-
in all
36 treatments in which there was microbubble formation and is analogous to what is seen during a fireworks display. A fragment would not repetitively
out,
give
and
rise
to an
disappear
intense
every
echo,
spread
0.83
seconds
Radiolotv
#{149} 165
(the
interval
between
the same location. ally at the conclusion
that
microbubble
debris-filled
waves)
is so
crete microbubble identified.
that
dis-
cannot
be
quotients
presented
here represent calculations that unique to our machine. Despite subjective nature of the quotient, provides confirmation who have bile that
that readily
low power
levels
show
more
significant
tation
than
late
cavitation
future
work
tionship targeting
the it at
likely
to
Figure
stone
fragmencavitation at the
with
levels know
only. how
effects
within
may
are
patients cavitates
are more
those
highest power yet specifically
(usu-
in viscous
great
bursts
cavitation
in
are times of a treatment)
persistence bile
The
shock There
shed
We do not to manipubile,
light
on
but
the
rela-
between bile composition for optimal cavitation.
and
Delius et al suggested that cavitation may have been responsible for soft-tissue injury in experimental studies in dogs (3). Similarly, Kuwahara et al showed that hypenechoic foci indicative of micnobubbles correlate with histologic evidence of injury to the canine
kidney
during
(7). On
the
pears
that
experimental
basis tissue
lithotripsy
of these
studies,
tolerates
it ap-
compressive
forces better than rarefactive forces. Our work clinically confirms the expenimental hypothesis of Delius et a! and Kuwahara et a! in liver parenchyma of patients undergoing gallstone
lithotnipsy.
Transient
liver
injury,
as
evidenced by a reversible rise in the SCOT level, was clearly associated with the presence of hepatic microbubbles. The microbubbles were usually shortlived but persisted as long as 6 minutes in liven parenchyma. This dissipation time was greater than in bile and probably related to the solid nature of liver parenchyma. No residual sonognaphic changes were identified in the liver of any patient. Hepatic microbubbles in the near field often cast their shadow across the target zone within the gallbladder. Not only may targeting be impaired but we hypothesize that shock waves may be attenuated. Because of concerns about transient hepatocellular damage and potentially compromised treatments, strategies for
limiting oped. ment
they
liver
cavitation
Temporarily causes bubbles
recur
when
were
devel-
stopping the to dissipate,
treatment
treatbut
is resumed.
Redirecting the shock wave path can shift the location of tissue injury. If the path remains transhepatic, cavitation is not reduced but merely moved. Advancing the center of the focal volume
deepen
into
the
patient
proved
to be the best strategy for reducing liven cavitation. This can usually be accomplished by extending the Lithostar acoustic lens but may at times require
166
Radiology
#{149}
7.
Schematic
shows
how
focal
volume
is advanced
into
patient
to limit
hepatic
cavi-
tation. Although the overall shape of the shock wave beam is that of an hourglass, the twodimensional representation of the focal volume (50% isobar) is cigar shaped (series of dots). With extension of the acoustic lens from the lithotripton, the focal volume may be moved deeper into the patient. This places the stone at the proximal point of the focal volume and the liver in a lower-power portion of the beam. If properly targeted, the stone will attenuate far-zone power, and the beam may be angled to avoid the upper pole of the right kidney. GB = gallbladder, dashed line skin surface, cross-hatched area hepatic cavitation.
the compression pressure at the coupling site. Since the focal volume tends to be cigar shaped, it is pos-
away microbubbles er parenchyma
sible
In conclusion, sonographically visible microbubbles in bile are an important marker of cavitation and enable
varying
to advance
the focus
so that
the
stone resides at the proximal point of the focal zone (Fig 7). The power delivered to the stone in the near-field portion of the focal volume is only slightly reduced compared with that in a more
central
portion
of the focal
volume.
Ad-
vancing the focus leaves the liver antenor to the focal volume, in a wider, less powerful part of the beam, resulting in fewer cavitation effects. This approach to clinical targeting is useful but should be used only if the far zone of the shock wave path can be angled to avoid the kidney. Advancing the focus to spare the liver while jeopardizing
the kidney
is not acceptable.
not be necessary devices
(mainly
small
and
round
with
or elliptic
a
echoes
are
disturbance
caused
The
and
pattern
due by
rate
solely the
of flow
to
shock
flow waves.
foci in the livliver from
stone pulverin liven may
cause transient hepatocellular damage. Advancing the focal zone and altering the shock wave path may be useful in reducing intrahepatic cavitation. U Acknowledgments: The authors acknowledge Karen Kellough and Yvonne Carew for assistance in the preparation of this manuscript.
References 1.
2.
3.
4.
5.
focus.
Vascular microbubbles were seen in three patients. In all three, a focus of hepatic microbubbles was seen near the vessel, and in two, bubbles could be seen entering the vessel. This latter observation makes it unlikely that intravascular
prediction of successful ization. Their presence
at all for low-power piezoelectnic)
the
injury.
Manipula-
tion of the focal zone depth to reduce cavitation in critical organs is possible regardless of the method used to actually generate shock waves. The maneuyen is most useful for devices with cigar-shaped focal volumes that have an axial dimension larger than that of many stones and which may overlap adjacent organs. The maneuver may
from protect
Zeman RK, Davros WJ, Garra BS, Horii SC. Cavitation effects during lithotnipsy. I. Results of in vitro experiments. Radiology 1990; 176:000-000. Delius MK, Brendel W. Mechanisms of action in extra-corporeal shockwave lithotnipsy. In: Ferrucci JT, Delius MK, Burhenne HJ, eds. Biliary lithotnipsy. Chicago: Year Book Medical, 1989; 31-42. Delius M, Jordan M, Eizenhoeffer H, et al. Biological effects of shock waves in dogs: administration rate dependence. Ultrasound Med Biol 1988; 14:689-694. Coleman AJ, Saunders JE, Crum LA, Dyson M. Acoustic cavitation generated by an extracorporeal shockwave lithotripter. Ultrasound Med Biol 1987; 13:69-76. Sackmann M, Delius M, Sauerbruch T, et al. Shockwave lithotnipsy of gallbladder stones: the first 175 patients. N EngI J Med 1988; 318:393-397.
6.
7.
Brink JA, Simeone JF, Saini S. et al. Simulation of gallstone fragments by cavitation bubbles during extracorporeal shockwave lithotnipsy: physical basis and in vitro demonstration. Radiology 1990; 174:787-791. Kuwahara M, loritani W, Kanibe K, et al. Hyperechoic region induced by focused shockwaves in vitro and in vivo: possibility of acoustic cavitation bubbles: J Litho Stone Dis 1989; 1:282-288.
suggested
that the microbubbles were entering venous structures. The vessel distnibution allowed us to confirm that the yessels in two of three patients were branches of patients to ascertain
of the portal vein. is still too small whether vessels
This group to allow us carrying
October
1990