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Magnetic Resonance–Derived 3-Dimensional Blood Flow Patterns in the Main Pulmonary Artery as a Marker of Pulmonary Hypertension and a Measure of Elevated Mean Pulmonary Arterial Pressure Gert Reiter, PhD*; Ursula Reiter, PhD*; Gabor Kovacs, MD; Bernhard Kainz, MSc; Karin Schmidt, MD; Robert Maier, MD; Horst Olschewski, MD; Rainer Rienmueller, MD Downloaded from http://circimaging.ahajournals.org/ by guest on May 2, 2017 Background—Pulmonary hypertension is a disease characterized by an elevation in pulmonary arterial pressure that is diagnosed invasively via right heart catheterization. Such pathological altered pressures in the pulmonary vascular system should lead to changes in blood flow patterns in the main pulmonary artery. Methods and Results—Forty-eight subjects (22 with manifest pulmonary hypertension, 13 with latent pulmonary hypertension, and 13 normal control subjects) underwent time-resolved 3D magnetic resonance phase-contrast imaging of the main pulmonary artery. Velocity fields that resulted from measurements were calculated, visualized, and analyzed with dedicated software. Main findings were as follows: (1) Manifest pulmonary hypertension coincides with the appearance of a vortex of blood flow in the main pulmonary artery (sensitivity and specificity of 1.00, 95% confidence intervals of 0.84 to 1.00 and 0.87 to 1.00, respectively), and (2) the relative period of existence of the vortex correlates significantly with mean pulmonary arterial pressure at rest (correlation coefficient of 0.94). To test the diagnostic performance of the vortex criterion, we furthermore investigated 55 patients in a blinded prospective study (22 with manifest pulmonary hypertension, 32 with latent pulmonary hypertension, and 1 healthy subject), which resulted in a sensitivity of 1.00 and specificity of 0.91 (95% confidence intervals of 0.84 to 1.00 and 0.76 to 0.98, respectively). Comparison of catheter-derived mean pulmonary artery pressure measurements and calculated mean pulmonary artery pressure values resulted in a standard deviation of differences of 3.6 mm Hg. Conclusions—Vortices of blood flow in the main pulmonary artery enable the identification of manifest pulmonary hypertension. Elevated mean pulmonary arterial pressures can be measured from the period of vortex existence. (Circ Cardiovasc Imaging. 2008;1:23-30.) Key Words: hypertension, pulmonary 䡲 magnetic resonance imaging 䡲 blood flow 䡲 blood pressure 䡲 catheterization P ulmonary hypertension (PH) is a disease characterized by an elevation in pulmonary arterial pressure that manifests in its early stages during exercise. The diagnosis of PH is established when mean pulmonary artery pressure (mPAP) measured invasively by right heart catheterization exceeds 25 mm Hg at rest (manifest PH) or 30 mm Hg with exercise (latent PH).1 which is related to mPAP,6 the quantity used to define PH. Parameters that directly correlate with mPAP or pulmonary vascular resistance have been related to the shortened acceleration times of blood flow in the right ventricular outflow tract.2,3,7–11 However, the overall applicability and accuracy of the above-described methods are controversial.12–16 Additionally, various authors10,11,17,18 have observed spatially highly inhomogeneous cross-sectional flow profiles and fractions of retrograde flow during systole and diastole in the main pulmonary artery in patients with PH. This was not observed in normal subjects. Even though no correlation between retrograde flow and the degree of PH was found,10,11 these observations suggest PH-caused flow topologies in the Clinical Perspective see p 30 Noninvasive imaging modalities such as echocardiography and MRI have been used to predict PH. Evaluation of the regurgitant tricuspid jet velocity2,3 and septal bowing4,5 have been used to estimate systolic pulmonary artery pressure, Received January 3, 2008; accepted May 14, 2008. From Siemens Medical Solutions (G.R.), Graz, Austria; University Clinic of Radiology (U.R., K.S., R.R.), University Clinic of Internal Medicine, Department of Pulmonology (G.K., H.O.) and Department of Cardiology (R.M.) of the Medical University of Graz, Graz, Austria; and the Institute for Computer Graphics and Vision (B.K.), Technical University of Graz, Graz, Austria. Clinical trial registration information—URL: http://www.clinicaltrials.gov. Unique identifier: NCT00575692. The online-only Data Supplement is available with this article at http://circimaging.ahajournals.org/cgi/content/full/1/1/23/DC1. Correspondence to Gert Reiter, Siemens Medical Solutions, Strassgangerstrasse 315, A-8054 Graz, Austria. E-mail [email protected] *The first 2 authors contributed equally to this work. © 2008 American Heart Association, Inc. Circ Cardiovasc Imaging is available at http://circimaging.ahajournals.org 23 DOI: 10.1161/CIRCIMAGING.108.780247 24 Circ Cardiovasc Imaging Table 1. July 2008 Study Population: Exploratory Study Manifest PH (n⫽22) Characteristic Latent PH (n⫽13) Patients Without PH (n⫽3) Healthy Volunteers (n⫽10) Sex (female/male), n 10/12 11/2 2/1 6/4 Age, y 61⫾10 66⫾6 55⫾9 26⫾7 mPAP at rest, mm Hg 41⫾13 16⫾4 12⫾2 䡠䡠䡠 39⫾6 23⫾5 䡠䡠䡠 mPAP during exercise, mm Hg 䡠䡠䡠 Values for age and mPAP are given as mean⫾SD. Downloaded from http://circimaging.ahajournals.org/ by guest on May 2, 2017 right ventricular outflow tract. Neither echocardiography nor conventional magnetic resonance (MR) through-plane cine phase-contrast imaging appears to be an appropriate technique for a detailed investigation of this assumption, but the MR phase-contrast method can be used to assess timeresolved 3D velocity information of blood flow.19 Complex cardiovascular flow topologies have been studied with this technique and various adequate visualization tools.20,21 The purpose of the present study was to investigate characteristic differences in 3D blood flow patterns in the main pulmonary artery of patients with manifest PH, patients with latent PH, and subjects without PH to determine the blood flow pattern– related measures for mPAP and PH. Methods important change in drug treatment or disease state occurred between the 2 examinations. Right Heart Catheterization and Patient Classification Right heart catheter examinations were performed with a 7F quadruple-lumen, balloon-tipped, flow-directed Swan-Ganz catheter by the transjugular approach (Baxter Healthcare Corp, Irvine, Calif). Parameters that were obtained included mPAP. Patients with no manifest PH underwent a symptom-limited exercise test on a cycle ergometer in a semisupine position with a right heart catheter in place. A standard protocol with a 25-W increase every 2 minutes was used, and mPAP was measured at each stage of exercise. On the basis of the results of the catheterization, patients were assigned to 3 groups1: manifest PH (clinical classification; see online Data Supplement), latent PH, and subjects without PH. Patients without PH and healthy volunteers were assigned to the control group. Subjects MR Imaging The present study was approved by the local ethics review board, and all subjects gave written informed consent. Subjects with contraindications to MR were not enrolled. Patients with suspected or known PH were sent consecutively to MRI after right heart catheterization was completed. The study was subdivided into exploratory and blinded prospective studies. A total of 42 patients were included in the exploratory study. Thirty-eight patients (Table 1) were investigated by right heart catheterization and MR phase-contrast imaging of the pulmonary artery. Four patients were excluded from evaluation because of air trapping during ergometry (1 patient), missing catheter data during exercise (1 patient), and incomplete MR investigation (2 patients). Patients underwent catheter and MR investigation within 2.8⫾4.1 days. In addition, 10 healthy volunteers with no history of cardiovascular or pulmonary disease (Table 1) underwent MR phase-contrast imaging of the pulmonary artery. Conventional ECG-gated cine MRI was used to exclude valvular regurgitations and to confirm normal left and right ventricular function.22 Sixty patients were included in the blinded prospective study. Five patients were excluded from evaluation because of missing catheter data during exercise (3 patients) and incomplete MR investigation (2 patients). The remaining 55 patients (Table 2) underwent catheter and MR investigation within 6.4⫾6.8 days. Generally, no clinically ECG-gated MR imaging was performed on a 1.5-T field-strength scanner (Magnetom Sonata; Siemens, Erlangen, Germany) with a 6-channel cardiac-array coil. All subjects were investigated in the supine position. Velocity field measurements were part of a comprehensive protocol that included retrospectively ECG-gated cine gradient echo imaging with steady-state free precession in the standard cardiac views (3- and 4-chamber views, right and left ventricular 2-chamber views, right and left ventricular outflow tract, and short-axis planes) to verify in particular the normal cardiac function of healthy volunteers. To acquire velocity field data, the main pulmonary artery was covered with 3 to 5 gapless slices in the right ventricular outflow tract orientation by 2D, retrospectively ECG-gated, spoiled gradient echo– based phase-contrast sequences with a 4-point velocity encoding scheme.19 Velocity encoding was set to 90 cm/s in all directions and adapted in the case of aliasing in the main pulmonary artery. Further parameters of the protocol used in the present study were a 234 to 276⫻340-mm2 field of view, 96 to 114⫻192 matrix (interpolated to 192 to 228⫻384 matrix), 15° flip angle, 89-ms temporal resolution (3 segments, 7.5-ms repetition time), reconstruction of 20 cardiac phases, 4.1-ms echo time, and 451 Hz/pixel bandwidth. GRAPPA (generalized auto-calibrating partially parallel acquisition) with a parallel acquisition factor of 2 and an average of 24 reference lines was used to keep the average imaging time per slice at 22 heartbeats, which allowed the performance of measurements during breath-holds in inspiration. For patients who were not able to hold their breath well, the investigation was performed under free-breathing conditions with 3-fold averaging to suppress breathing artifacts. Table 2. Study Population: Blinded Prospective Study Characteristic Manifest PH (n⫽22) Latent PH (n⫽32) Patients Without PH (n⫽1) Sex (female/male), n 12/10 27/5 1/0 Age, y 67⫾13 56⫾11 51 mPAP at rest, mm Hg 39⫾10 17⫾3 14 40⫾6 25 mPAP during exercise, mm Hg 䡠䡠䡠 Values for age and mPAP are given as mean⫾SD. Image Processing and Analysis in the Exploratory Study Calculation of velocity fields from the acquired phase images, their visualization, and analysis thereof were performed with dedicated software (4D Flow, Siemens).20 –23 This software provides visualization of each velocity vector as a color-encoded vector in 3D space: The length and color of the vector indicate the magnitude of velocity, whereas the direction of the vector represents the direction of the Reiter et al Blood Flow Patterns in Pulmonary Hypertension 25 Downloaded from http://circimaging.ahajournals.org/ by guest on May 2, 2017 Figure 1. Typical flow patterns in the right ventricular outflow tract at different cardiac phases for a patient with manifest PH (A, D, and G), a patient with latent PH (B, E, and H), and a normal subject (C, F, and I). PA indicates main pulmonary artery; PV, pulmonary valve; and RV, right ventricle. At maximum outflow (A through C), flow profiles were distributed homogenously across the cross sections of the main pulmonary artery in the manifest PH group (A), the latent PH group (B), and the normal group (C). In later systole (D through F), a vortex was formed in the manifest PH group (D). No such vortex could be found in the latent PH group (E) or the normal group (F). After pulmonary valve closure (G through I), the vortex in the PH group persisted for some time. In all cases, continuous diastolic blood flow upward along the anterior wall of the main pulmonary artery could be observed. Although this phenomenon disappeared quickly in controls (I), it was observed significantly longer in latent PH (H) and manifest PH (G). velocity. Velocity vectors are projected onto (opaque) corresponding anatomic phase-contrast images. The suppression of noisy pixels (by a signal-to-noise threshold in the anatomic phase-contrast images) and an adjustable thinning out of the velocity vector fields enable interpretation of the blood flow patterns within the anatomic context (Figure 1). In addition to determination of the systolic acceleration time (time difference between maximum and onset of pulmonary outflow), systolic ejection time (time difference between onset and end of pulmonary outflow), maximum blood flow velocity above the pulmonary valve at maximum pulmonary outflow, and maximum velocity above the pulmonary valve at its closure, 3 features of the flow field in the main pulmonary artery were investigated in more detail. First, the existence of vortices in the primary flow direction in the main pulmonary artery was investigated. In general, a vortex is defined as a ring- or spiral-shaped motion of fluid or gas. In terms of the vector field representation of blood flow, this means the formation of concentric ring- or spiral-shaped curves in the main pulmonary artery to which velocity vectors are tangential. A vortex in the primary flow direction in the main pulmonary artery means that there is forward and backward flow through a cross section of the main pulmonary artery through the center of the vortex (Figure 2A). Both the existence of such a vortex and the relative period of existence (tvortex) of a nonvalvular vortex in the main pulmonary artery (number of cardiac phases with vortex divided by the total number of imaged cardiac phases) were determined visually and independently by 2 observers. The second specific feature investigated was the diastolic streamline of blood flow upward along the anterior wall of the main pulmonary artery. In terms of the vector field representation of blood flow, this means that blood moves continuously up the anterior wall of the main pulmonary artery during diastole (Figure 2B). The relative period of existence of diastolic streamlines (tstreamlines; the number of cardiac phases after pulmonary valve closure with streamlines along the main pulmonary artery divided by the total number of imaged cardiac phases) was determined visually and independently by 2 observers. Third, a location index was introduced to characterize the velocity profile of blood flow above the pulmonary valve in the anteriorposterior direction. Depending on whether the maximum velocity through the cross section of the main pulmonary artery appeared in the anterior, middle, or posterior third of the vessel, the location index was set to ⫹1, 0, or ⫺1, respectively (Figure 2C). In case of equal maximum velocities in multiple sections, the location index was set to the average value of the corresponding thirds (maximum velocities in the section thirds were interpreted as being different if their difference exceeded a typical pixel-by-pixel variation of velocities). The location index was determined in the cardiac phase with maximum pulmonary outflow, as well as in the cardiac phase of pulmonary valve closure. Image Processing and Analysis in the Blinded Prospective Study After analogous postprocessing of MR data, the existence of a vortex and its relative period of existence (tvortex) were determined by a single observer blinded to the catheter results. Statistical Analysis Statistical analysis was performed with NCSS (J. Hintze, NCSS, LLC, Kaysville, Utah). Mean values are given together with standard deviations (SDs). Group means of the manifest PH, latent PH, and control groups were compared via 1-way analysis of variance and Tukey-Kramer multiple-comparison test. We generally set the significance level to 0.05. For tstreamlines, we additionally performed an analysis of covariance with age as the covariate. A -coefficient was calculated to specify the interrater agreement with respect to the existence of a vortex. To characterize the diagnostic accuracy of predicting manifest PH via vortex formation, 26 Circ Cardiovasc Imaging July 2008 Results Description of Flow Patterns Downloaded from http://circimaging.ahajournals.org/ by guest on May 2, 2017 Figure 2. Specific flow features in the main pulmonary artery. PA indicates main pulmonary artery; PV, pulmonary valve; RV, right ventricle; a, anterior; and p, posterior. A, Vortex in the primary flow direction in the main pulmonary artery. B, Streamlines of blood flow up the anterior wall of the main pulmonary artery. C, Maximum velocities vmax,a, vmax,m, and vmax,p through a cross section of the main pulmonary artery above the pulmonary valve were determined in the anterior (a), middle (m), and posterior (p) third of the vessel. Depending on which of these velocities was maximal, the location index for the velocity profile was set to ⫹1 (vmax,a maximal), 0 (vmax,m maximal), or ⫺1 (vmax,p maximal). It is 0 in the above example. sensitivity and specificity were determined together with their 95% confidence intervals. Interobserver variability in the determination of relative periods of the existence of vortices and streamlines was specified by withinsubject SDs (calculated by variance component analysis) and intraclass correlation coefficients. Mean values of the data of the 2 observers were used to study differences between group means and to analyze the relationship between periods of existence of vortices and mPAP by correlation and regression analysis. For the blinded prospective study, comparison of mPAP values measured by catheter and calculated by the regression equation obtained in the exploratory study was performed by Bland-Altman analysis. The authors had full access to the data and take full responsibility for the integrity of the data. All authors have read and agree to the manuscript as written. During systolic acceleration of blood flow through the pulmonary valve, the flow patterns in the manifest PH, latent PH, and control groups were similar. Blood flow velocities were uniformly distributed across the cross section of the main pulmonary artery. Their primary direction was parallel to the vessel wall. Velocities increased from one cardiac phase to the next until a maximum was reached (Figure 1A through 1C). Although mean maximal peak velocities did not differ significantly between the groups (79⫾21 cm/s in manifest PH, 74⫾11 cm/s in latent PH, and 77⫾11 cm/s in the controls), the mean acceleration time was significantly shorter in the manifest PH group and was not significantly different between the latent PH and control groups (mean acceleration times of 107⫾25 ms in manifest PH, 133⫾24 ms in latent PH, and 141⫾26 ms in the control group; P⫽0.0006 for F test). After maximum outflow, blood flow velocities gradually decreased until the pulmonary valve closed. No significant differences in total ejection times were observed (374⫾54 ms in manifest PH, 365⫾64 ms in latent PH, and 392⫾60 ms in controls). During the deceleration period, the flow profiles changed from rather homogeneous velocity distributions across the cross section of the main pulmonary artery to profiles with higher velocities at the anterior wall (Figure 1D through 1F): Although the position indexes for velocity profiles above the pulmonary valve were 0.1⫾0.5, 0.2⫾0.3, and 0.1⫾0.3 at maximal outflow, they were 1.0⫾0.1, 1.0⫾0.0, and 1.0⫾0.0 at valvular closure in the manifest PH, latent PH, and control groups, respectively. There was, however, a structure that occurred only in patients with manifest PH: A vortex in the primary flow direction was formed, typically below the right pulmonary artery at the posterior wall of the main pulmonary artery (Figure 1D). In 2 patients with high mPAP, vortex formation had already begun in the acceleration phase. The rotational direction of the vortex was always more distal from the right ventricle from anterior to posterior and more proximal to the right ventricle from posterior to anterior (as drawn in Figure 2A and visible in Figure 1D and 1G). During deceleration of blood flow through the pulmonary valve, the region covered by the vortical motion typically increased, and the center of the vortex moved in the main pulmonary artery. After closure of the pulmonary valve, blood flow in the main pulmonary artery did not stop immediately. Mean maximum velocities above the pulmonary valve were 28⫾9 cm/s in manifest PH, 21⫾6 cm/s in latent PH, and 18⫾5 cm/s in controls, and the differences between manifest PH and both latent PH and controls were significant (P⫽0.0012 for F test). In all subjects, blood flow was observed spatially continuously up the anterior wall of the main pulmonary artery after pulmonary valve closure; in the case of manifest PH, this flow was accompanied by the rotational flow of the vortex (Figure 1G through 1I). The mean relative periods of the existence of these streamlines (tstreamlines) were 0.42⫾0.15 in manifest PH, 0.29⫾0.07 in latent PH, and 0.15⫾0.05 in controls (Figure 3) and differed significantly between all Reiter et al Blood Flow Patterns in Pulmonary Hypertension 27 Downloaded from http://circimaging.ahajournals.org/ by guest on May 2, 2017 Figure 3. Comparison of tstreamlines for the manifest PH, latent PH, and control groups. groups (P⬍0.0001 for F test). Age dependence was not significant (P⫽0.10 in analysis of covariance). Interobserver variability of the measurement of tstreamlines was 0.04, and the intraclass correlation coefficient was 0.93. Vortices and mPAP For all 22 patients in the manifest PH group, the described vortex was found, whereas this flow pattern was not detected in any of the subjects without manifest PH (-index for evaluating twice the existence of vortices was 1.00). The use of the existence of vortices in the primary flow direction in the main pulmonary artery as a diagnostic criterion for the presence of manifest PH resulted in a sensitivity of 1.00 and a specificity of 1.00, with 95% confidence intervals of 0.84 to 1.00 and 0.87 to 1.00, respectively. The correlation coefficient between tvortex and mPAP of patients with manifest PH was 0.94 (95% confidence interval 0.85 to 0.97). The corresponding linear regression equation was mPAP (in millimeters mercury) ⫽ 16.7 ⫹ 58.0 䡠 tvortex, with an SD of 4.8 mm Hg from the regression line (Figure 4A). Interobserver variability of the measurement of the relative period of existence of the vortex (tvortex) in the primary flow direction was 0.03, and the intraclass correlation coefficient was 0.97. In the blinded prospective study, all 22 patients with manifest PH had a vortex of blood flow in the main pulmonary artery, whereas 30 patients without manifest PH had none. In 3 patients with latent PH, a vortex was detected (mPAP at rest of 21, 21, and 23 mm Hg with tvortex of 0.05, 0.05, and 0.25, respectively). Consequently, the vortex criterion for the presence of manifest PH led to the same sensitivity as the exploratory study. Specificity obtained was 0.91 (95% confidence interval 0.76 to 0.98). The comparison of mPAP measured by catheter and mPAP calculated by the regression equation resulted in a nonsignificant bias of ⫺0.2 mm Hg, an SD of differences of 3.6 mm Hg, and 95% limits of agreement of ⫺7.3 and 6.9 mm Hg, respectively (Figure 4B). Discussion The main findings of the exploratory study were as follows: (1) Manifest PH coincides with the appearance of a vortex of Figure 4. A, Correlation and linear regression line (together with 95% confidence bounds) of mPAP of patients with manifest PH and relative period of the existence of a vortex (tvortex) in the primary flow direction in the main pulmonary artery. B, BlandAltman plot of mPAP values measured by catheter and calculated by the regression equation mPAP⫽16.7⫹58.0䡠tvortex (with 95% confidence bounds for bias and 95% limits of agreement) for the blinded prospective study. blood flow in the main pulmonary artery; (2) the relative period of existence of the vortex (tvortex) correlates with mPAP at rest, with a high correlation coefficient of 0.94 in patients with manifest PH; and (3) the relative period (tstreamlines) of continuous diastolic flow upward along the anterior wall of the main pulmonary artery differed significantly between patients with manifest PH, those with latent PH, and controls. Vortex Formation Elevated mPAP in manifest PH is accompanied by an anomalous time course of pulse pressure,2,24 and the pressure gradient between the right ventricle and the pulmonary artery becomes zero and positive earlier during systole.25,26 This fact explains the reduced acceleration time in patients with manifest PH, which is the rationale for attempts to assess mPAP and PH directly by noninvasive methods.2,3,7–11 We also observed reduced acceleration times in patients with manifest PH. Other features of the anomalous time course of the pulse pressure of patients with manifest PH are consistent with the observed vortex formation: The results for the position index 28 Circ Cardiovasc Imaging July 2008 Figure 5. Schematic illustration of flow separation at a boundary (eg, a vessel wall). When the pressure gradient becomes positive, the boundary layer thickens, and a vortex may develop within the boundary layer. Downloaded from http://circimaging.ahajournals.org/ by guest on May 2, 2017 of the velocity profiles above the pulmonary valve indicate that in later systole, generally spatial peak velocities move from a central position toward the anterior wall of the main pulmonary artery. This in turn may be interpreted as an increase in the thickness of the boundary layer at the posterior wall of the main pulmonary artery; in other words, flow separates from the posterior wall of the main pulmonary artery. Flow separation at boundaries is a common physical phenomenon if the driving pressure gradient becomes positive.27 In particular, thickened boundary layers become susceptible to backward flow and the formation of vortices (Figure 5). During the midsystolic period, when the pressure gradient between the right ventricle and pulmonary artery is already close to zero, a short positive wave occurs in the time course of the pressure gradient for patients with manifest PH.25,26 We conjecture that this wave, supported by the present high velocities, triggers vortex formation in the main pulmonary artery. Relation Between the Existence of Vortices and Elevated mPAP A priori, it is not obvious that the relative period of existence of the vortex (tvortex) correlates with mPAP; however, PH is accompanied by increased pulmonary vascular resistance and decreased compliance of the pulmonary vasculature.28 During the ejection period of the right ventricle, higher resistance means that less blood can be released to the peripheral pulmonary vasculature. Less compliance means that the released blood cannot be stored adequately in the pulmonary vasculature by a volume change of the vessels. The vortex appears to be a natural mechanism to preserve a part of the kinetic energy of blood, to release the blood to the periphery during diastole. Because diastolic blood release is again determined by pulmonary vascular resistance and compliance, it is plausible that both the vortex and the upward flow persist longer when mPAP is higher. The correlation coefficient of 0.94 between tvortex and mPAP in the case of manifest PH means that the quantities almost exclusively determine one other. The tvortex enables the noninvasive estimation of mPAP via the linear regression equation (in millimeters mercury: mPAP ⫽ 16.7 ⫹ 58.0 䡠 tvortex) with an SD of 4.8 mm Hg. This SD is small compared with other noninva- sive estimates of pulmonary pressure.29 In addition to measurement errors that resulted from the MR sequence technique and vortex determination, which will be discussed below, deviations between mPAP determined by catheter and values that were calculated may have 2 additional causes: First, catheter and MR measurements were not performed simultaneously, and it has been shown30 that the variation within long-term mPAP measurements is 8%. Consequently, an SD of ⬎3 mm Hg (resulting from 8% of our average mPAP value at rest of 41 mm Hg; Table 1) appears to be explainable simply by the physiological change of mPAP and the variability of its catheter measurements. Furthermore, the linearity assumption for the relationship between mPAP and the relative period of existence (tvortex) of the vortex in the main pulmonary artery is quite likely to be violated, at least for higher mPAPs, especially because the maximal predictable mPAP via the linear regression equation is 74.8 mm Hg. Other model equations with a steeper slope for higher mPAPs could be motivated by a general change of the relation of quantities such as compliance28 or acceleration time7 and mPAP, but a larger group of patients with manifest PH would be needed to compare different model equations statistically. Diastolic Streamlines Apart from the vortex pattern in the main pulmonary artery, the study showed significant differences in diastolic streamlines of blood flow in the manifest PH, latent PH, and control groups. Given the interpretation of the vortex as a “reservoir of kinetic energy,” the difference between manifest PH and the other groups is not surprising. It is, however, surprising that the relative period (tstreamlines) of continuous diastolic flow upward along the anterior wall of the main pulmonary artery differed significantly in an investigation at rest between patients with latent PH and controls and therefore allows identifying latent PH. In accordance with the explanation of the phenomenon for manifest PH, the prolonged tstreamlines reflects changes in pulmonary vascular resistance and compliance of the pulmonary vasculature that are too small to lead to vortex formation, as in manifest PH. A possible limitation of the study is that a portion of the tstreamlines difference between patients with latent PH and control subjects may be attributed to the different age distributions in these groups, although age was not significant as a covariate: Although normal mPAP does not depend significantly on age, normal pulmonary vascular resistance31 and compliance28 do. Retrograde Flow In contrast to previous studies that used MR phase-contrast measurements to study PH,9 –11 we acquired time-resolved 3D flow information in the main pulmonary artery to analyze flow topology–related quantities. For patients with manifest PH, increased retrograde flow at the posterior wall of the main pulmonary artery10,11,17,18 can be explained immediately by the existence of a vortex. We could not define a general rule for the motion of the vortex throughout the cardiac cycles which explains why no relation between the retrograde through-plane velocities and mPAP was found in previous studies.10,11 Reiter et al Error Estimate and Verification by the Blinded Prospective Study Downloaded from http://circimaging.ahajournals.org/ by guest on May 2, 2017 As mentioned, part of the SD of 4.8 mm Hg in the linear regression determination of mPAP via tvortex resulted from the MR sequence technique and the method of vortex determination: We used a moderate time resolution to keep the imaging time short and interpolated the retrospectively acquired data to images of 20 cardiac phases. Consequently, a difference of 1 cardiac phase in the determination of tvortex or tstreamlines corresponded to at least 5% of the RR interval, and the minimal difference in mPAP that could be resolved with this time resolution was 2.9 mm Hg. The color-encoded vector field representation of measured velocity fields was appropriate for the interpretation of blood flow patterns. The existence of vortices and streamlines was determined visually with excellent interobserver agreement, which might decrease if catheter results are unknown to the observers. However, the variability of 3% of the RR interval for the determination of tvortex contributes a further variability of 1.7 mm Hg to the mPAP calculation. Summing up the given error estimates of the physiological change of mPAP, the variability of its catheter measurements, and the variability of the tvortex determination, the SD of 4.8 mm Hg between invasively determined and calculated mPAP values is explained fully. To validate the findings with regard to vortices of blood flow, a blinded prospective study was performed. Within confidence limits, this study reproduced the results of the exploratory study. Nevertheless, the appearance of vortices in 3 patients with latent PH should be discussed. Whereas the large deviation of measured and calculated mPAP for 1 patient was probably due to physiological variability (⫺8.2 mm Hg, Figure 4B), 2 patients with a tvortex of 0.05 illustrate a problem associated with the moderate time resolution of MR measurements: Short-living vortices might be missed, and these vortices might correspond to mPAP values slightly below 25 mm Hg according to the linear regression equation (calculated for mPAP values above 25 mm Hg; Figure 4A). In summary, 3D visualization of blood flow patterns in the main pulmonary artery via MR phase-contrast measurements is a promising tool for noninvasive detection and understanding of PH. It allows the identification of manifest and latent PH. Elevated mPAP can be determined with physical accuracy by measuring the period of existence of the vortex associated with PH. 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More on the noninvasive diagnosis of pulmonary hypertension: Doppler echocardiography revisited. Eur Respir J. 1995;8: 1445–1449. 30. Rich S, D’Alonzo GE, Dantzker DR, Levy PS. Magnitude and implications of spontaneous hemodynamic variability in primary pulmonary hypertension. Am J Cardiol. 1985;55:159 –163. 31. Ehrsam RE, Perruchoud A, Oberholzer M, Burkart F, Herzog H. Influence of age on pulmonary haemodynamics at rest and during supine exercise. Clin Sci (Lond). 1983;65:653– 660. CLINICAL PERSPECTIVE Downloaded from http://circimaging.ahajournals.org/ by guest on May 2, 2017 Pulmonary hypertension is associated with a poor prognosis. Currently, the only established method to diagnose pulmonary hypertension is to directly measure pulmonary arterial pressure on right heart catheterization. We present a new method to measure elevated mean pulmonary arterial pressure noninvasively by magnetic resonance velocity imaging. Our findings suggest that (1) manifest pulmonary hypertension coincides with the appearance of a vortex of blood flow in the main pulmonary artery; (2) the relative period of existence of this vortex correlates in a highly significantly manner with mean pulmonary arterial pressure; and (3) the relative period of continuous antegrade diastolic flow along the anterior wall of the main pulmonary artery is significantly prolonged in patients with latent pulmonary hypertension compared with controls. These findings suggest that flow patterns in the main pulmonary artery allow not only the identification of manifest and latent pulmonary hypertension but also the measurement of elevated mean pulmonary arterial pressures. Magnetic Resonance−Derived 3-Dimensional Blood Flow Patterns in the Main Pulmonary Artery as a Marker of Pulmonary Hypertension and a Measure of Elevated Mean Pulmonary Arterial Pressure Gert Reiter, Ursula Reiter, Gabor Kovacs, Bernhard Kainz, Karin Schmidt, Robert Maier, Horst Olschewski and Rainer Rienmueller Downloaded from http://circimaging.ahajournals.org/ by guest on May 2, 2017 Circ Cardiovasc Imaging. 2008;1:23-30 doi: 10.1161/CIRCIMAGING.108.780247 Circulation: Cardiovascular Imaging is published by the American Heart Association, 7272 Greenville Avenue, Dallas, TX 75231 Copyright © 2008 American Heart Association, Inc. All rights reserved. Print ISSN: 1941-9651. 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