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1 Department of Anesthesia, 2 Nuclear Medicine PET and Cyclotron Unit, and 3 Copenhagen Muscle Research Center, Rigshospitalet, DK-2100 Copenhagen; and 4 Department of Medical Physiology C, Panum Institute, University of Copenhagen, DK-2200 Copenhagen, Denmark
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ABSTRACT |
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To evaluate whether electrical
admittance of intracellular water is applicable for monitoring filling
of the heart, we determined the difference in intracellular water in
the thorax (ThoraxICW), measured as the reciprocal value of
the electrical impedance for the thorax at 1.5 and 100 kHz during lower
body negative pressure (LBNP) in humans. Changes in
ThoraxICW were compared with positron emission
tomography-determined C15O-labeled erythrocytes over the
heart. During
40 mmHg LBNP, the blood volume of the heart decreased
by 21 ± 3% as the erythrocyte volume was reduced by 20 ± 2% and the plasma volume declined by 26 ± 2% (P < 0.01; n = 8). Over the heart region, LBNP was also associated with a decrease in the technetium-labeled erythrocyte activity by 26 ± 4% and, conversely, an increase over the lower leg by 92 ± 5% (P < 0.01; n = 6). For 15 subjects, LBNP increased thoracic impedance by 3.3 ± 0.3
(1.5 kHz) and 3.0 ± 0.4
(100 kHz), whereas leg
impedance decreased by 9.0 ± 3.3
(1.5 kHz) and 6.1 ± 3
(100 kHz; P < 0.01). ThoraxICW was
reduced by 7.1 ± 1.9 S · 10
4
(P < 0.01) and intracellular water in the leg tended
to increase (from 37.8 ± 4.6 to 40.9 ± 5.0 S · 10
4; P = 0.08). The
correlation between ThoraxICW and heart erythrocyte volume
was 0.84 (P < 0.05). The results suggest that thoracic electrical admittance of intracellular water can be applied to evaluate
changes in blood volume of the heart during LBNP in humans.
cardiac output; electrical impedance; heart rate; positron emission tomography; technetium-labeled erythrocytes
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INTRODUCTION |
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IN SITUATIONS IN WHICH bleeding, upright positioning, or anesthesia contribute to reductions in venous return, one approach to evaluate filling of the heart is to monitor thoracic impedance (TI; Refs. 5, 6, 11, 12, 17). TI relates inversely to the fluid content of the thoracic region, and, with the use of two frequencies, TI distinguishes between the extracellular water (ECW) and total body water (TBW; Refs. 2, 25, 29). Thus the difference in the reciprocal value of the impedance (the admittance) between a high- and a low-frequency current may reflect changes in the intracellular water volume (ICW; Refs. 2, 9, 26).
During acute changes, we assume, the distribution of erythrocytes accounts for most of the deviation in regional ICW, and electrical admittance reflects the distribution of erythrocytes in the body. To test the hypothesis that thoracic electrical admittance reflects filling of the heart, young subjects were exposed to lower body negative pressure (LBNP). Application of LBNP is associated with redistribution of blood from the thorax to the vascular beds in the abdomen and lower extremities to an extent that presyncopal symptoms may develop (13).
The blood volume of the heart was determined quantitatively by positron emission tomography (PET) based on inhalation of C15O (21, 22, 27). In a separate study, 99mTc-labeled erythrocytes were applied to determine the blood distribution between the thorax and the lower leg during LBNP (12). Plasma atrial natriuretic peptide (ANP) was measured to indicate the filling of the right atrium (11), and cardiac output (CO) was assessed together with central venous O2 saturation (SvO2; Refs. 4, 8).
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METHODS |
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Nine men participated in the PET study and six others in the 99mTc study. Their mean age was 28 (range 23-32) years, height 184 () cm, and weight 78 (71-92) kg with no significant differences between the participants in the two studies. The Ethics Committee of Copenhagen approved the project (J.nr.01-045/98), and informed consent was obtained.
The subjects reported to the laboratory in the morning after an
overnight fast. After instrumentation, they were positioned in the LBNP
chamber, which was sealed at the level of the iliac crest. To reduce
movement of the subject, a bicycle saddle was provided, and the feet
were supported. Thirty minutes of rest were followed by 20 min of
supine control, 10 min of exposure to each of four LBNP pressures
(
10,
20,
30, and
40 mmHg), and 20 min of recovery at
atmospheric pressure. Negative pressure was graded by venting the
output of a commercial vacuum cleaner, and data were collected at the
end of each stage.
A cannula (1.0 mm ID, 19.5 gauge) was placed in the brachial artery of the nondominant arm for the measurement of mean arterial blood pressure (MAP). Another cannula (1.4 mm ID, 14 gauge) was introduced into the superior caval vein via the left basilic vein for central venous pressure (CVP) and SvO2. A three-lead electrocardiogram was used to record heart rate (HR), and pressures were measured by use of Bentley transducers (Uden, the Netherlands) positioned at the level of the right atrium in the midaxillary line and fastened to the subject. The transducers were connected to a Dialogue 2000 monitor (IBC-Danica, Copenhagen, Denmark).
TI and lower leg impedance (LI) were measured with a monitor that uses
200 µA at 1.5 and 100 kHz (C-guard, Danmeter, Odense, Denmark). The
skin was cleaned with alcohol swabs. Pairs of electrodes (Q-10-25,
Medicotest, Denmark) were used for the determination of TI. The
electrodes were placed on the right sternocleidomastoid muscle and the
upper left ribs in the midaxillary line with an internal distance of 5 cm. This electrode placement was also used when the correlation to
changes in the central blood volume was evaluated (6, 12, 18,
19). For determination of LI, a pair of electrodes was placed on
the caput tibiae and another pair on the lateral malleolus of the right
leg. Changes in LI have been calibrated against the volume of the lower
leg as calculated by its circumference (1). For all
electrode placements, the outer two electrodes provided the electrical
field, and the inner pair was sensing. Changes in ICW in the thorax
(ThoraxICW) and in the leg (LegICW) were
estimated as the difference between the reciprocal value of impedance
at 100 and 1.5 kHz (1/Impedance at 100 kHz
1/Impedance at 1.5 kHz) (2, 9, 26).
Stroke volume (SV) and CO were determined by impedance cardiography (Instrumentation for Medicine, Greenwich, CT; Ref. 20) and total peripheral resistance (TPR) was the ratio of MAP to CO. To avoid interaction between measurements, the cardiograph was disconnected when the other impedance values were recorded.
To determine the thoracic blood volume, we used a PET scanner (Advance,
General Electric Medical Systems, Milwaukee, WI; Ref. 3) and
C15O with a half-life of 118 s. PET estimates the
regional concentration of the radioisotope quantitatively
(28). The subject was placed in a supine position, and the
axial imaging field (15 cm) was selected to cover both the heart and
the lungs within 35 imaging planes. Using an external 68Ga
radiation source for 20 min, we used a transmission scan for attenuation correction of the subsequent emission scans. After 2-min
inhalation of C15O and a wait of 1 min to approach
distribution equilibrium, a 5-min emission scan was carried out at each
LBNP pressure. In the first four subjects, we observed a 1- to 3-cm
caudal movement of the heart and lungs during LBNP. To evaluate to what
extent such movement affected the determination of the blood volume in the region of interest (ROI), we applied a 2-min attenuation scan before each emission scan in five subjects. Within ROI, the blood volume is
PET/CB · V, where
PET is the average
tracer concentration (kBq/ml), CB is the assumed "100%" blood
concentration in left heart blood pool with C15O (kBq/ml),
and V is the total volume of the ROI. Thus EV = BV · Hct, where EV is the erythrocyte volume, BV is blood
volume, and Hct is hematocrit (22) in the brachial artery.
To limit the exposure to radioactivity, the distribution of
erythrocytes to the lower legs was evaluated in another group of
volunteers by use of a TCK-11 kit (6) and LBNP. The LBNP protocol was identical to that used for the PET study. Ten milliliters of blood were drawn from a forearm vein in a heparinized syringe and
labeled with 37 MBq 99mTc pertechnetate to an initial
binding efficiency of 98%. The 99mTc sample was then
reinjected intravenously 30 min before the study. For the detection of
99mTc activity, a gamma camera with a rectangular,
low-energy, high-resolution, parallel-hole collimator was used to image
activity from the thorax. The ROI was selected to reflect the heart
region. A relative measure of the erythrocyte activity was calculated
from the mean count (total counts of ROI divided by the area). A
collimated NaI single-probe detector integrating 10-s intervals was
applied. The lower legs were evaluated with the active element 15 cm
below the lateral margin of the patella (6). All
measurements were corrected for decay using the half-life of technetium
(T1/2 = 6.02 h), i.e.,
At = A0e
t, where
= ln2/T1/2, At is the activity to
time t, and A0e is the activity to
time 0; T1/2 is the half life of Tc.
For determination of ANP, 4 ml of arterial blood were taken in ice-cold
polypropylene tubes containing heparin (20 IU/ml blood) and aprotinin
(200 kIU/ml). Blood was kept on ice and, within 10 min of sampling was
centrifuged at 4°C for 15 min at 3,000 rpm. The plasma was
stored at
20°C. ANP was extracted from plasma by means of C18
cartridges (Sep-Pak, Waters) and determined by RIA (11).
Blood samples for Hct and SvO2 were placed immediately on ice and were analyzed within minutes using an ABL 510 apparatus (Radiometer, Copenhagen, Denmark).
Data are presented as means ± SE, and statistical significance was set at a P value of 0.05. LBNP-related changes were assessed by the Friedman test, and the Wilcoxon or Mann-Whitney tests were used for comparisons. Correlations were performed with the Spearman test.
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RESULTS |
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Eleven subjects remained normotensive during LBNP. In four
subjects, presyncopal symptoms (nausea, paleness, and a feeling of
heat) developed, associated with decreases in MAP and HR. In one
subject, presyncopal symptoms developed at
20 mmHg, and in the three
others they appeared at
30 mmHg. The presyncopal symptoms disappeared
immediately after return to atmospheric pressure.
Cardiovascular variables and ANP.
All variables remained stable during supine rest. In normotensive
subjects, MAP was 90 ± 3 mmHg and did not change significantly during LBNP (Fig. 1). HR (57 ± 3 beats/min) increased at LBNP
20 mmHg and reached 79 ± 4 beats/min at LBNP
40 mmHg. CVP (6 ± 1 mmHg) fell at LBNP
10
mmHg to stabilize at 0 ± 1 mmHg. SV (120 ± 6 ml) decreased
at LBNP
20 mmHg and fell to 72 ± 5 ml, and CO was reduced from
7.1 ± 1.2 to 5.1 ± 0.8 l/min. SvO2
(75.7 ± 1.2%) decreased at LBNP
20 mmHg and dropped to
67.9 ± 1.5%. TPR (13.6 ± 1.6 mmHg min/l) increased at LBNP
30 mmHg and reached 18.2 ± 1.6 mmHg min/l.
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40 mmHg, i.e., from a
resting value of 23.9 ± 3.0 to 19.6 ± 2.5 pmol/l
(n = 15; P < 0.01). Plasma ANP
returned to the resting level 10 min after LBNP was terminated.
PET.
At the end of the recovery period, the transmission image was similar
to the one obtained at rest before application of LBNP (Fig.
2), indicating that movement of the
thorax was <4 mm, which was consistent with observation of external
landmarks. During LBNP, the heart and the lungs moved 1-3 cm
caudally (Fig. 3); still, as judged by
the transmission image, both regions remained within the imaging field.
In contrast, the top of the liver moved out of the image and thereby
contributed to overestimation of the reduction in "thoracic" blood
volume.
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20
mmHg, falling from 783 ± 30 to 617 ± 26 ml (21 ± 3%;
P < 0.01) at LBNP
40 mmHg, and there was a similar
reduction for the lung blood volume (22 ± 4%; from 350 ± 30 to 267 ± 36 ml; P = 0.92; Fig.
4). Hct rose from 42.8 ± 0.8% to
44.4 ± 0.9%, indicating that the erythrocyte and plasma volume
of the heart decreased from 335 ± 11 to 271 ± 9 ml (20 ± 2%) and from 448 ± 39 to 338 ± 39 ml (26 ± 2%),
respectively (P < 0.01). The reduction in the thoracic
blood volume, including the heart, lungs, thoracic muscles, and also
the top of the liver, was larger (by 26 ± 3%; from 1,772 ± 96 to 1,299 ± 73 ml) than the blood volume reduction in the heart.
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99mTc-labeled erythrocytes.
Over the heart region, the gamma camera count rate decreased by 26 ± 4% at LBNP
40 mmHg and similarly by 25 ± 3% in those subjects who developed presyncopal symptoms. Hct rose from 41.5 ± 1.3 to 43.2 ± 1.0% at LBNP
40 mmHg and from 41.5 ± 1.7 to 43.2 ± 1.4% in subjects who had presyncopal symptoms. Thus
there was a similar change in plasma volume for two groups of subjects. Conversely, over the lower leg, the 99mTc
count rate increased by 92 ± 5% at LBNP
40 mmHg. The elevated count rate over the lower leg was lower for those who developed presyncopal symptoms (by 60 ± 10%; Fig.
5). Ten minutes after return to
atmospheric pressure, the activity of 99mTc in the heart
and the lower leg was 3.8 ± 1.1% and 1.1 ± 1.2% lower
than the control value, respectively.
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Electrical impedance.
After 30 min of supine rest, TI was 50.3 ± 2.3
at 1.5 kHz and
37.6 ± 1.8
at 100 kHz. There was an increase in TI at LBNP
20 mmHg, and, at LBNP
40 mmHg, TI was elevated by 3.1 ± 0.4
(1.5 kHz) and 2.8 ± 0.4
(100 kHz; P < 0.01; n = 11; Fig. 1). In those subjects who developed
presyncopal symptoms, the increase in TI was similar (4.2 ± 0.8
; 1.5 kHz and 3.3 ± 0.6
; 100 kHz; n = 4).
After 30 min of rest, ThoraxICW was 69.0 ± 5.4 S · 10
4, and it decreased at LBNP
20 mmHg to be
reduced by 6.7 ± 1.9 S · 10
4 at LBNP
40
mmHg (P < 0.01). At the time the presyncopal symptoms developed, the reduction in ThoraxICW was similar (7.0 ± 0.6 S · 10
4).
at 1.5 kHz and
69.7 ± 6.2
at 100 kHz. LI decreased at LBNP
20 mmHg and was
reduced by 8.7 ± 3.2
(1.5 kHz) and by 6.0 ± 3.0
(100 kHz) at LBNP
40 mmHg. The decrease was smaller in those
subjects who developed presyncopal symptoms (3.6 ± 2
; 1.5 kHz
and 2.0 ± 1.8
; 100 kHz). In normotensive subjects,
LegICW tended to increase (from 37.8 ± 4.6 to
40.9 ± 5.0 S; P = 0.08), whereas the change was small in those subjects who developed presyncopal symptoms.
ThoraxICW returned to the control value within 10 min after
LBNP. However, after 20 min of recovery, TI remained 1.1 ± 0.3
(1.5 kHz) and 0.8 ± 0.2
(100 kHz) above the resting
value. Conversely, LI remained 3.5 ± 2.7
(1.5 kHz) and
2.0 ± 2.7
(100 kHz) lower than at rest.
Changes in TI and the heart blood volume were correlated (Table
1). TI at 100 kHz exhibited the
highest median correlation with changes in the blood volume of the
heart [0.85 (0.74
0.95)] and was significant for all
subjects. Changes in ThoraxICW and in the erythrocyte
volume in the heart were correlated in 14 of the 15 subjects [0.84
(0.62
0.96)], and TI at 1.5 kHz had the lowest median
correlation with changes in the erythrocyte volume [0.78 (0.43
0.90)] and was significant in 12 of the 15 subjects.
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DISCUSSION |
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As assessed by PET and by a gamma camera-based determination of
the distribution of labeled erythrocytes, the difference in ThoraxICW between 1.5 and 100 kHz reflected changes in the
amount of erythrocytes within the heart during LBNP in young, healthy subjects. A 10-min exposure to
40 mmHg LBNP reduced the volume of the
heart by ~23%, corresponding to a 20% reduction in the erythrocyte
volume and a 26% decline in the plasma volume, whereas the blood
volume of the lower leg increased by 92%. These changes were reflected
by TI and LI at both 1.5 and 100 kHz.
ThoraxICW and the reduced filling of the heart.
Both C15O- and 99mTc-labeled erythrocytes
demonstrated that the reduction in the count over the heart was by
~20% during LBNP
40 mmHg, and the erythrocyte count returned to
the control value within 10 min after atmospheric pressure was
reestablished. These changes were reflected in the deviation of
ThoraxICW. There is no fluid shift between erythrocytes and
blood plasma during LBNP (7). Therefore, the distribution
of erythrocytes determined the deviation of ICW. The individual
correlation for ThoraxICW and the erythrocyte volume was
significant in 14 of the 15 subjects, and it was never below 0.6.
change in TI corresponded to a 6.8 (1.5 kHz)
and 7.5% (100 kHz) deviation in volume, whereas for a
1-S · 10
4 change in ThoraxICW, the
value was 3%.
Murray et al. (13) reported that, after 10-min exposure to
40 mmHg LBNP, the central blood volume (CBV) was reduced by 19%, as
measured by CO (l/min), determined with a dye dilution, times the
transit time (min). Such a determination of CBV represents the
volume of the heart and lungs and also the blood volume in the arterial
vessels to the distance (in time) of the tip of the arterial cannula.
Thus CBV cannot differentiate between blood in the heart and that in
the lungs. With PET and C15O, we demonstrated that there
was no difference in the reduction of the blood volume in the heart and
lungs during LBNP.
LegICW and venous pooling in the leg.
LBNP induced venous pooling in the vascular beds of the legs, as
verified by the distribution of 99mTc-labeled erythrocytes
and by recording of LI. The increased count rate (60%) was lower in
the presyncopal subjects than in the normotensive subjects (92%) as a
smaller LBNP was reached. The larger decrease in LI at 1.5 kHz (9.0
) than in LI at 100 kHz (7.0
) reflected pooling of plasma and
edema in the leg. LegICW tended to rise and remain elevated
after 20 min of recovery. This was so despite the
99mTc-labeled erythrocytes reestablishing baseline values
immediately after return to atmospheric pressure. This discrepancy is
likely related to LBNP-induced intracellular edema in addition to
changes in the distribution of erythrocytes in the body and an
interstitial edema as indicated by LI at 1.5 kHz.
(12). The present results suggest that, in terms
of the amount of fluid shifted to the leg,
40 mmHg LBNP is similar to
head-up tilt to more than 50°. Musgrave et al. (14)
report that
40 mmHg LBNP is similar to 70° head-up tilt when a
calculation of blood in the leg is estimated by water immersion
technique, whereas Patwardhan et al. (16) indicate that
48 mmHg LBNP corresponds to 50° head-up tilt in terms of change in
calf circumference.
Methodological aspects. Progressive levels of LBNP caused the heart and the lungs to move 1-3 cm caudally. We applied an attenuation scan before each emission scan in five subjects. On the basis of these results, a correction was applied for the four subjects who had only a baseline attenuation scan. This scan was used to calculate an attenuation factor for each detector pair. The factor represented the fraction of photons from an external positron source that was attenuated by the tissue. The factor was used to "scale up" the regional tissue activity data in the subsequent emission scan along the line of projection between two coincident detectors. By doing so, we observed that the thoracic blood volume was reduced more (26%) than the volume calculated both for the heart and the lungs (21%). The difference between the reduction in organ and thoracic blood volume reflected that the top of the liver moved out of the image during LBNP.
We did not correct for the biological decay of the 99mTc tracer (6). After correction for physical decay, 99mTc activity was reduced by 3.8 and 1.1% over the thorax and the lower leg at the end of the recovery period. Thus there was a small overestimate of the reduction in 99mTc activity over the heart and, correspondingly, an underestimate of the lower leg blood volume during LBNP. The biological decay of 99mTc could explain some of the difference in the reduction in heart volume determined by 99mTc and C15O. In conclusion, we found thoracic admittance to correlate with changes of the erythrocyte volume of the heart during LBNP in young, healthy men. This result supports an evaluation of the electrical properties of the thorax for monitoring the intravascular volume in situations in which the erythrocyte and plasma volumes do not vary in parallel, e.g., during sustained head-up tilt or in bleeding patients receiving an isotonic saline infusion.| |
ACKNOWLEDGEMENTS |
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We gratefully acknowledge Mette Secher for assistance in data collection; Helle J. Larsen, Kate Pedersen, Brita Dondera, Bitten Vindberg, and Hanne Jørgensen for technical assistance; and Mikael Jensen and the staff in the cyclotron unit for providing the C15O. We also thank Birgitte Hanel and Tommi Bo Lindhardt for valuable discussion of the implication of the 99mTc tracer instability.
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FOOTNOTES |
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This study was supported by the Danish National Research Foundation (504-14), and the John and Birthe Meyer Foundation is gratefully acknowledged for the donation of the cyclotron and PET scanners.
Address for reprint requests and other correspondence: Y. Cai, Dept. of Anesthesia, Rigshospitalet 2041, Blegdamsvej 9, DK-2100 Copenhagen Ø, Denmark (E-mail: caiyan{at}yahoo.com).
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
Received 15 October 1999; accepted in final form 5 May 2000.
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