(Circulation. 1995;91:2955-2960.)
© 1995 American Heart Association, Inc.
Articles |
From the Departments of Internal Medicine (Cardiovascular Division) (W.G.H., R.A.L., B.M.M., J.E.W., C.L., D.W., L.D.H., R.M.P.) and Radiology (H.F.L., D.P.P., R.M.P.), University of Texas Southwestern Medical Center at Dallas.
Correspondence to Ronald M. Peshock, MD, Mary Nell and Ralph B. Rogers Magnetic Resonance Center, University of Texas Southwestern Medical Center, 5801 Forest Park, Dallas, TX 75235-9085. E-mail Peshock@rad-rogers.swmed.edu.
| Abstract |
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Methods and Results Twenty-one subjects (15 women and 6 men; age
range, 15 to 72 years) underwent velocity-encoded, phase-difference MRI
measurements of flow in the proximal aorta and pulmonary artery,
followed immediately by cardiac catheterization. The presence of
left-to-right intracardiac shunting was assessed with hydrogen
inhalation, after which shunt magnitude was measured by the oximetric
and indocyanine green techniques. Of the 21 patients, 12 had
left-to-right intracardiac shunting detected by hydrogen inhalation.
There was a good correlation (r=.94) between the invasive
and MRI assessments of shunt magnitude. In comparison to oximetry and
indocyanine green, MRI correctly identified the 12 patients with a
ratio of pulmonary to systemic flow (Qp/Qs) of <1.5 (9 without
intracardiac shunting and 3 with small shunts) and the 9 patients with
a Qp/Qs of
1.5 (6 with atrial septal defect, 1 with ventricular
septal defect, 1 with patent ductus arteriosus, and 1 with both atrial
septal defect and patent ductus arteriosus).
Conclusions Compared with measurements obtained during cardiac catheterization, velocity-encoded, phase-difference MRI measurements of flow in the proximal great vessels can reliably assess the magnitude of intracardiac left-to-right shunting.
Key Words: magnetic resonance imaging imaging catheterization
| Introduction |
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With magnetic resonance imaging (MRI), the cardiovascular system can be imaged with high spatial resolution.13 Velocity-encoded, phase-difference MR images have been used to measure flow in the carotid artery,14 proximal aorta and pulmonary artery,15 16 and abdominal aorta.17 Phase-difference methods are based on the principle that hydrogen nuclei moving through a magnetic field gradient accumulate a phase shift proportional to their velocity.18 Flow is calculated by multiplying blood velocity by the cross-sectional area of the vascular structure of interest. With this technique, flow can be measured quickly; scans can be performed in less than 2 minutes. This technique has been used to quantify intracardiac shunting in patients with large atrial septal defects,19 but its ability to assess shunt magnitude in patients with small shunts and those with shunts at other locations has not been evaluated. Accordingly, the present study was performed in patients with and patients without intracardiac left-to-right shunting to compare velocity-encoded, phase-difference MRI measurements of shunt magnitude with those obtained by the use of oximetry and indocyanine green.
| Methods |
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Study Design
Each patient underwent (1) velocity-encoded,
phase-difference
MRI measurements of flow in the proximal aorta and pulmonary artery,
followed in 1 to 2 hours by (2) cardiac catheterization. Hydrogen
inhalation was used to assess the presence of left-to-right
intracardiac shunting, as this technique can reliably detect shunts
with a Qp/Qs of >1.01.20 Patients in group 1 had hydrogen
appearance times of >4 seconds, indicating no left-to-right shunting,
whereas those in group 2 had hydrogen appearance times of <4 seconds,
indicating left-to-right shunting.21 During
catheterization, all patients in group 2 underwent a detailed oximetric
assessment, as described previously,4 followed by the
administration of indocyanine green, as described
previously.6 11 The MRI and invasive measurements
were
accomplished in close temporal proximity to ensure that similar
hemodynamic conditions existed during both assessments. During MRI and
catheterization, heart rate and blood pressure were monitored and
recorded.
| MRI Technique |
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Each patient was positioned supine on the MRI table after placement of ECG monitoring leads, a respiratory gating belt, and a brachial blood pressure cuff. All MR scans used prospective ECG and respiratory gating. Multislice coronal, gradient-echo PEG sequences were used to obtain scout images of the proximal aorta and pulmonary artery. These localizing scans were fast-field echo sequences with first-moment compensation in the read-out and slice-select directions, a repetition time (TR) of 20 milliseconds, and an echo time (TE) of 9.4 milliseconds. Eight-millimeter slices were used with a field of view (FOV) of 50 cm, a flip angle of 40 degrees, a 256x256 matrix, and voxel sizes of 3x2x8 mm.
Interleaved, velocity-encoded, phase-difference PEG sequences positioned across proximal vessel segments were used to measure flow in the aorta and pulmonary artery. A PEG size of 2 (yielding 8 to 12 frames per cardiac cycle) was used in 18 of the 23 patients. In 1 patient, a PEG size of 3 (yielding 9 frames per cardiac cycle) was used, and in 4 patients, a PEG size of 1 (yielding 20 to 26 frames per cardiac cycle) was used. These scans were 10-mm-thick slices with 256x256 matrices and had a FOV ranging from 32 to 45 cm (yielding voxel sizes of 1x1.3x10 mm to 1x1.7x10 mm), a flip angle of 40 degrees, a TR of 19.5 milliseconds, and a TE of 11 milliseconds. For the proximal aorta, an oblique slice was positioned from a coronal scout image perpendicular to the course of the aorta, approximately 2 to 4 cm above the aortic valve and distal to the coronary arterial ostia. Except for patients 10 and 13, the slice positions used for the pulmonary artery were selected from the coronal scout images and corresponded to a plane that produced a circular appearance of the pulmonary artery to minimize partial volume effects during image acquisition. The position was distal to the pulmonic valve but proximal to the bifurcation. In patients 10 and 13, echocardiography suggested the presence of a patent ductus arteriosus, and therefore two flow scans (one of each major branch of the pulmonary artery) were performed. The total pulmonic blood flow for these 2 patients was measured as the sum of flow calculated in the two branches.
After acquisition, the first-order, motion-compensated reference scan
and the velocity-sensitized scan were Fourier-transformed to produce
two sets of images (magnitude and corresponding phase image). These
images were transferred to an image-processing workstation for further
analysis. A velocity map was generated by (1) pixel-to-pixel
subtraction of the velocity-sensitized and velocity-compensated phase
images and (2) application of a correction algorithm designed to remove
background phase error. The background correction involved three steps:
(1) an operator identified the stationary pixels on the magnitude image
of the velocity-compensated acquisition; (2) the processing software
fit the background phase onto a two-dimensional plane; and (3) the
estimated linear background phase shift was subtracted from the
phase-difference image. To complete the generation of the velocity map,
we multiplied the background-corrected, phase-difference image by a
constant to create a velocity image where pixel gray-scale intensity is
represented in millimeters per second. Magnitude images and
corresponding velocity maps for the aorta and pulmonary artery in
patient 12 are displayed in Figs 1
and 2
.
After producing the velocity maps, we transferred the digital data to a
second image-processing workstation for flow calculations.
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Flow was calculated by multiplying the cross-sectional area of the vessel lumen by the mean blood flow velocity for each point sampled in the cardiac cycle. The cross-sectional area of the vessel lumen was defined on the magnitude image of the reference scan by a region of interest (ROI), where
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This same ROI was superimposed on the velocity map for each corresponding frame of the cardiac cycle, and the mean velocity was obtained by measuring the average pixel intensity within the ROI. For each frame sampled in the cardiac cycle, Fi=flow per frame of the cardiac cycle (cm3 per frame)=mean velocity (cm/s)xarea (cm2)x2xPEG sizexTR of sequence (seconds per frame), with the TR (pulse repetition time) being multiplied by 2 because the sequence consists of a reference followed by a velocity-sensitized pulse. With prospective gating, images were not acquired during the last 30 to 80 milliseconds of diastole. For this terminal portion of the cardiac cycle, we estimated flow to be half the flow of the previously imaged frame. Thus,
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where Fi equals the flow in frame i, and n equals the number of frames in the cycle plus the last interval of the cycle. By multiplying heart rate by the sum of the flow for all frames of the cardiac cycle, we determined flow per minute through the vessel.
All data, including heart rate, blood pressure, and pulmonic and aortic flows, were compiled, analyzed, and stored without knowledge of the findings during subsequent catheterization. MR images were stored on optical disks for subsequent recall and analysis. To determine the interobserver variability of analyzing the MR images, they were analyzed by two investigators who were blinded to the other's results as well as to the results of catheterization. After completion of the MRI scanning procedure, patients were transferred immediately to the catheterization laboratory.
Cardiac Catheterization
In each patient, an 8F sheath was
inserted percutaneously into
the femoral vein, and a cannula was placed in the femoral artery. A
platinum-tipped pacing electrode was advanced to the main pulmonary
artery and connected to a standard DC amplifier (Electronics for
Medicine) for the recording of an electrical potential. The patient was
administered a single breath of hydrogen, and the elapsed time from
inhalation to the detection of an electrical potential was measured
according to previously described
techniques.21 22 23 The
platinum-tipped electrode was withdrawn from the body, and an 8F
Goodale-Lubin catheter was advanced to the pulmonary artery. In less
than 10 minutes, multiple blood samples were obtained from the
right-side heart chambers, and their oxygen saturations measured and
contents calculated, after which the criteria of Dexter et
al24 were used to determine the location of intracardiac
left-to-right shunting. Subsequently, pulmonic and systemic blood flows
were quantified by using the Fick
principle,4 6 20 and
Qp/Qs was calculated.
Immediately afterward, in the patients who had hydrogen appearance times of less than 4 seconds (group 2), the Goodale-Lubin catheter was readvanced to the pulmonary artery, and 5 mg of indocyanine green was injected through the catheter as blood was withdrawn from the femoral artery through a densitometer cuvette.6 From the inscribed curve, shunt magnitude was quantified in accordance with the equation of Carter et al.5 For all the patients studied, catheterization measurements were completed within 15 to 20 minutes of one another, and no change in heart rate or systemic arterial pressure occurred during this time. The catheterization Qp/Qs value was calculated by averaging the oximetric and indocyanine green measurements.
Statistical Analysis
Without knowledge of the flow data, we
excluded patients from
analysis if there was a substantial change in heart rate or
systemic arterial pressure between the time of MRI and invasive
measurements, specifically, if (1) the patient's heart rate varied by
>15% or (2) mean systemic arterial pressure varied by >20%. All
data are expressed as mean±1 SD. The values for Qp/Qs obtained
invasively were compared with those measured by the use of MRI with a
two-variable linear regression analysis. In addition, the
difference between catheterization and MRI measurements of Qp/Qs were
compared using the analysis of Bland and
Altman.25
| Results |
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15% (range,
0% to 15%), and mean systemic arterial pressure varied by <20%
(range, 1% to 18%) during MRI and catheterization. One subject was
excluded from analysis because an error in acquisition rendered the
flow measurements uninterpretable. The remaining 21 subjects (15 women
and 6 men; age range, 15 to 72 years) formed the study population9
without evidence of intracardiac shunting (group 1) and 12 with
intracardiac shunting (group 2). Twenty patients had normal sinus
rhythm, and 1 (patient 20, group 2) had atrial fibrillation. The
duration of the flow scans was 1 to 3 minutes for those in sinus
rhythm. The patient with atrial fibrillation was scanned with two
averaged acquisitions, thereby lengthening the flow scans to 4 to 6
minutes.
Data regarding the 21 subjects are displayed in Table 1
.
Table 2
summarizes the mean blood flow and Qp/Qs
obtained with catheterization and MRI for all 21 patients. As displayed
in Fig 3
, there was a good correlation between the
measurements of shunt magnitude obtained with catheterization and those
obtained with MRI. Furthermore, MRI reliably determined whether Qp/Qs
was <1.5 or
1.5 in all 21 subjects. The difference between Qp/Qs
measured with MRI and that measured with catheterization was 0±0.3 for
the patients in group 1, -0.2±0.7 for the patients in group 2,
and
-0.1±0.55 for all patients combined (Fig 4
).
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The interobserver variability for the MRI measurements of flow was 3±3% in the aorta and 5±3% in the pulmonary artery.
| Discussion |
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MRI with spin-echo or gradient-echo techniques has been used to detect
and localize atrial and ventricular septal defects with a sensitivity
of 90% to 100% and a specificity of 90%.26 27
Although
velocity-encoded, phase-difference cine MRI scans of the proximal aorta
and pulmonary artery have been used to quantify the magnitude of
left-to-right intracardiac shunting in patients with large intracardiac
shunts,19 no previous study has assessed the usefulness of
this technique in distinguishing patients with no or small intracardiac
shunts from those with large shunts. Data from the present study
demonstrate that MRI can rapidly and accurately quantify shunt
magnitude in patients with intracardiac left-to-right shunting and,
furthermore, that it can reliably differentiate those with Qp/Qs of
<1.5 from those with Qp/Qs of
1.5 (Figs 3
and
4
).
Several features make MRI attractive for evaluating patients suspected of having left-to-right intracardiac shunting. First, it is safe, reasonably comfortable, noninvasive, and easily performed in an outpatient setting without the need for ionizing radiation or intravascular injections. Second, single flow measurements are performed rapidly (in less than 3 minutes), thereby allowing a complete hemodynamic assessment in less than 10 minutes. Third, excellent visualization of the area and velocity profile within the proximal aorta and pulmonary artery is obtained; therefore, impediments presented by body shape and size are of little concern. Fourth, high-resolution tomographic imaging for visualizing the entire thorax can be obtained concomitant with the flow analysis. This information can be used to detect associated anomalies, such as anomalous pulmonary venous drainage or patent ductus arteriosus; to visualize intracardiac structures before and after surgical intervention; and to reconstruct three-dimensional images of the heart and great vessels in patients whose anatomy is complex.
The present study has limitations. First, most of our patients were
in sinus rhythm. None had frequent ventricular ectopy, and only one had
atrial fibrillation. We are uncertain whether this technique provides
reliable results in patients with irregular rhythms. Second, we
excluded patients with aortic or pulmonic stenosis, since they have
turbulent, high-velocity flow jets in the proximal great vessels. As
other investigators have suggested,28 the acquisition of
data in these patients may require careful alignment of the
velocity-encoded slice parallel to the direction of flow and the use of
very short echo times (TE of 3 to 4 milliseconds). Third, we did not
enroll patients with marked pulmonic or aortic regurgitation. With our
method of calculating flow in these patients, negative flow in the
proximal great vessels during diastole would interfere with the
determination of forward flow. Fourth, MRI did not allow discrimination
of patients without shunts from those with small amounts of
left-to-right shunting. The discrepancy in systemic and pulmonary
artery flows in the patients with no shunting could have been caused by
technical factors related to the sensitivity of the MR flow
measurements.29 Finally, in the patients with hydrogen
appearance times of more than 4 seconds (group 1, Table 1
),
Qp/Qs by
catheterization was assumed to be 1. In these patients, the oxygen
saturation of pulmonary venous blood was not measured, and therefore,
Qp could not be precisely quantified oximetrically. In addition, no
prominent early recirculation was seen after injection of indocyanine
green, and therefore the percentage of left-to-right shunting could not
be measured by indicator dilution.
In conclusion, velocity-encoded, phase-difference cine MRI measurements of forward flow in the proximal aorta and pulmonary artery can accurately and rapidly quantify intracardiac left-to-right shunting, thereby providing a reliable, noninvasive method for determining which patients should be considered for surgical correction.
| Acknowledgments |
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Received October 10, 1994; revision received December 19, 1994; accepted December 21, 1994.
| References |
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