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Eur J Cardiothorac Surg 1999;16:300-305
© 1999 Elsevier Science NL
a Department of Cardiothoracic and Vascular Surgery, Skejby Sygehus, Aarhus University Hospital, 8200 Aarhus, N., Denmark
b Institute of Experimental Clinical Research, Aarhus University Hospital, 8200 Aarhus, N., Denmark
c MR Center, Skejby Sygehus, Aarhus University Hospital, 8200 Aarhus, N., Denmark
d Institute of Biomedical Engineering, University and E.T.H., Zürich, Switzerland
Corresponding author. Tel.: +45-89-49-5480; fax +45-89-49-6016
e-mail: skejmh{at}aau.dk
| Abstract |
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Key Words: Prosthetic heart valve Magnetic resonance imaging Hemodynamics In vitro Human
| 1. Introduction |
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Due to the importance of this issue the regulatory authorities consider hemodynamic performance of heart valve prostheses as a key area in their essential requirements for approving these devices to be used in humans [5,6]. Traditionally, in vitro and in vivo studies are performed by laser Doppler anemometry and echo Doppler cardiography used in different models and different applications. Therefore, it is often difficult to extrapolate data from the in vitro to the in vivo environment.
Magnetic resonance imaging (MRI) is a relatively new tool in this arena [79], but the beauty of this modality is its applicability to both in vitro and in vivo assessment of blood velocity fields and also for imaging purposes. Numerous studies have shown the reliability of MRI for velocity field and volume flow studies in a variety of settings [916]. Only few studies have reported on evaluation of prosthetic heart valves using this modality. A clinical concern has been raised as to whether heart valve patients can be subjected to MRI scanning at all both from a patient safety point of view and from a signal-to-noise point of view since the valve induce a significant artifact on the MRI image. We hypothesize that MRI can provide complementary hemodynamic data from prosthetic heart valves both in vitro and in vivo.
The purpose of this study was, therefore, to demonstrate the feasibility of using the MRI technique for heart valve studies by a qualitative comparison of velocity field data obtained downstream of a bileaflet prosthetic aortic valve in a pulsatile flow model with similar data from patients.
| 2. Materials and methods |
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The axial fluid velocity component was measured at two levels: 0.25 (0.25DD) and 1 diameter (1DD) downstream of the valve ring in a plane orthogonal to the main flow axis.
In order to obtain maximum performance (high resolution) of the MRI technique, we used a high field strength magnet in vitro accepting the inherent limitation that the measuring object (the flow model) had to fulfil some space limitations in order to fit into the magnet.
The MRI instrument was a 7.0 Tesla SISCO scanner (SIS-300/183, Varian, Palo Alto, CA, USA). The bore diameter of the scanner was 10 cm. Technical details are provided elsewhere [11]. The temporal resolution was 66 ms, the thickness of the slice (pixel size) was 1 mm. A field of view of 80x80 mm and a 256x256 matrix gave an in-plane spatial resolution of 0.31x0.31 mm. A trigger signal from the computer controlled pump allowed data acquisition from the scanner to be synchronized with the pulsatile flow. The MRI data were analyzed on a DEC-Alpha (Digital Equipment Corp., USA) workstation using a dedicated analysis program based on the PV-Wave (Visual Numerics, Boulder, CO, USA) programming language.
Fluid velocities were visualized as three-dimensional surface plots.
2.2. In vivo
Six patients, three male and three female aged 2274 (mean 52.6) years, who had a St. Jude Medical aortic valve inserted volunteered in the study. They all gave written and oral consent and the project was approved by the local ethics committee and conformed with the Helsinki II declaration. Valve sizes were 2127 mm in tissue annulus diameter and all patients were in NYHA class I. Standardization of valve orientation at implantation was not performed. Electrocardiogram was continuously monitored during the entire procedure.
The MRI scanning was performed in a Philips 1.5 Tesla Gyroscan S15/HP whole-body scanner (Philips Medical Systems, Best, Netherlands) with patients lying in supine position. Initially a series of spin echo scouts and coronal cine gradient echo images were made to locate the valve and determine its angulation in relation to the ascending aorta. To minimize signal void due to disturbed flow, blood velocity measurements were accomplished by the low echotime FAcE (Free Induction Decay Acquired Echo) sequence [12] in an image plane perpendicular to the ascending aorta. The image disturbances originating from the moving heart valve did not allow us to measure closer to the valve than 1 valve diameter (1DD) downstream of the valve ring. For reference, blood velocities were also measured 2 valve diameters downstream (2DD).
The image slice thickness was 10 mm. A field of view of 400 mm was applied on a 128x128 matrix giving an in-plane spatial resolution (pixel size) of 3.1x3.1 mm. An image was generated every 40 ms throughout the heart cycle. The time for completing an investigation was approximately 90 min.
The MRI data were reconstructed on the MRI host computer for imaging purposes. Subsequently data were transferred to a SPARC II workstation (Sun Microsystem Inc., Mountain View, CA, USA), where additional compensation for artefacts in the velocity images was performed as previously described [10].
Like for the in vitro data analysis, blood velocity data were displayed as three-dimensional surface plots as seen from a position downstream of the valve.
| 3. Results |
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The blood velocity profiles obtained from the patients had the same overall appearance in all cases. The temporal development of the blood velocity profile in one of the patients one diameter downstream of the valve is displayed in Fig. 3. During the acceleration phase, the highest velocities were disclosed in the two wall near areas of the vessel downstream of the two lateral valve orifices. At top systole and throughout the systolic deceleration phase, the valve features are consistently identifiable although not to the same extent as in vitro. An evident overall skewness of the velocity profile could be seen with the highest velocities toward the anterior right vessel wall. The skewness and contour of the velocity profiles were more enhanced at the 1DD than the 2DD position.
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Estimated cardiac output was 4.35.8 l min-1 (mean 5.2 l min-1) during measurements and heart rate was 6581 min-1 (mean 73.1 min-1).
None of the patients expressed any discomfort during or after the experiment.
| 4. Discussion |
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The advantage of MRI for in vitro fluid and in vivo hemodynamic evaluation of heart valve prostheses is the capacity to study velocity fields across the entire aortic area and with the capacity to measure all three velocity components both in vitro [7] and in vivo [15].
Using the small-bore, high magnetic field strength magnet it is possible to measure fluid velocities very close to the valve with a high temporal and spatial resolution, although not to the extent that allows turbulence analysis.
The in vitro investigations allow us to interpret velocity fields in quite significant detail and thus evaluate the impact of valve design on the flow through the valve.
The present study shows that velocity fields downstream of a bileaflet prosthetic heart valve cannot be extrapolated directly to a predicted outcome in patients. A study valve carefully mounted orthogonally to the long axis of the test tube will inherently provide nice symmetric velocity profiles compared to the clinical situation where this kind of idealized geometry in the left ventricular outflow tract, the aortic root or the ascending aorta is not present. Since the aortic annulus is often not orthogonal to the long axis of the ascending aorta skewed blood velocity profiles in the curved aorta is to be expected.
Furthermore, the 7.0 Tesla magnet used for in vitro studies obviously allows much more detailed display due to the ten times higher spatial resolution than the 1.5 Tesla whole-body MRI scanner.
Evidently, this study needs to be followed up by similar investigations of other valve types using MRI both in vitro and in vivo. Due to the non-invasive character and safety of this procedure such investigations can be accomplished in patients without significant ethical problems.
Newer MRI hard- and software have significantly improved the performance of the MRI techniques in terms of spatial and temporal resolution and shortening of experiment time consumption. Newer techniques such as navigators for respiratory control, combined with valve motion following modalities [16] will reduce the artefacts produced by the valve prosthesis, and allow measurements closer to the valve prostheses.
We conclude that MRI has advantages over the traditional hemodynamic measuring equipment due to its versatile applicability and the reliable outcome. Furthermore, in vitro models need to comprise much more geometrical complexity in order to simulate flow conditions in vivo. On the other hand, geometrical simplicity facilitates the interpretation of flow fields downstream of prosthetic heart valves without modulation from the environment.
| Acknowledgments |
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| Footnotes |
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| Appendix A |
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Dr. Hasenkam: It was not our primary goal to make clinical applicability of the magnetic resonance imaging, but obviously you can have it as a diagnostic tool in order to verify the function of the valve where you can see reflection of the velocity fields downstream of the valve. The purpose was mostly to evaluate the profiles in different types of valves so you can have a basic bank of data describing different types of valves.
Dr. E. Baudet (Bordeaux, France): Could you deduce shear stresses downstream aortic prostheses from velocity profiles assessed by MRI?
Dr. Hasenkam: MRI does not allow us directly to do shear stress measurements, and especially not turbulence shear stress measurements, of course. But if you take the velocity gradients in the profile, you can have indications where in the cross sectional area turbulence is prone to occur. So you can have an indication of shear stresses in that way.
Dr. R. DeSimone (Heidelberg, Germany): You know that MRI has a very slow acquisition rate. Which kind of procedure, or sequences (as they are called) did you use for making the acquisition? This is a very actual subject and perhaps you can explain more details about the sequence used.
Dr. Hasenkam: I am certainly not the technical MRI expert of the group, but we used the so called FAcE technique. You might know that this technique has a very short echo time, allowing us to have a fairly short acquisition time of the data. But, sorry to say, I don't know the precise details about the technical applicability.
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