Delayed reduction of tissue water diffusion after myocardial ischemia EDWARD W. HSU,1 RONG XUE,1 ALEX HOLMES,1 AND JOHN R. FORDER2 Departments of 1Biomedical Engineering and 2Radiology, The Johns Hopkins University School of Medicine, Baltimore, Maryland 21205-2195 magnetic resonance imaging; apparent diffusion coefficient; myocardial infarction DIFFUSION OF WATER is sensitive to changes in the structural geometry and organization of its molecular environment and can be noninvasively measured by using nuclear magnetic resonance (MR) techniques via the signal attenuation caused by the loss of spin-phase coherence in the presence of magnetic field gradients (30). The MR apparent diffusion coefficient (ADC) of tissue water has been found to decrease dramatically after acute cerebral ischemia (21). The ensuing research, the subject of several reviews (9, 11, 27, 32), suggests that the rapid decrease and reversal of the ADC change on recovery may offer the potential for early, noninvasive detection of stroke and reliable prediction of ischemic brain injury. The ADC decrease has been associated with the depletion of cellular energy stores (19), and cell swelling resulted from the disruption of membrane electrochemical homeostasis (3). Theoretical models of water diffusion in tissues (15, 29, 31) and direct measurements in single cells undergoing physiological perturbation (12) indicate that the predominant biophysical factor underlying the ADC decrease is the reduction of extracellular water volume fraction during cell swelling (rather than changes in the intrinsic diffusion characteristics of intra- and extracellular water). The specificity of the ADC decrease to cell swelling, which is a common pathophysiological response in distressed tissues, has been extended to diffusion-weighted MR imaging studies of other disorders such as cortical spreading depression (5), status epilepticus (36), and acute renal failure (33). MR techniques have long been used in the study of ischemic heart diseases and, in general, have included assessments of 1) myocardial metabolic activities using MR spectroscopy (8, 34), 2) contractile function using rapid imaging (23, 28) and MR tagging (2, 18) methods, and 3) MR image intensity changes induced by endogenous relaxation mechanisms (17, 24) or exogenous contrast agents (8, 26). Each of these approaches has its unique advantages and drawbacks. For example, MR spectroscopy may provide better specificity for pathophysiological responses but is limited in spatial and temporal resolution because of the inherently low concentration of tissue metabolites. Although imaging techniques based on mapping the distribution of water molecules offer improved resolution, regional contractility measurements may not be effective in distinguishing viable but dysfunctional (e.g., stunned or hibernating) tissue from nonviable myocardium. On the other hand, tissue viability and perfusion studies using exogenous contrast agents have been complicated by quantitation difficulties in relating image intensity to contrast agent concentration in tissues. Because of the complexity and heterogeneity of the pathophysiology, proper assessments of ischemic myocardial injury may require not just one but several examinations that are each sensitive to different responses in a comprehensive study. In this regard, tissue diffusion changes may provide new insights regarding the dynamics of myocardial injury and may complement established approaches in the study of ischemic heart diseases. The goal of this study is thus to determine whether tissue ADC changes occur after regional myocardial ischemia in an isolated, perfused rabbit heart model and whether diffusion changes can be used to monitor the nature and evolution of tissue injury. MATERIALS AND METHODS Isolated, perfused heart preparation. Hearts were obtained from New Zealand White male rabbits and were perfused retrogradely via the aorta using an MR-compatible Langendorff apparatus as described previously (1). Tissue and perfusate temperature were maintained at 37°C via a water-filled heat-exchange circuit. The perfusate was continually equilibrated with a 95% O2-5% CO2 gas mixture. To avoid excess hydrostatic pressure accumulation and distension of the left ventricle (LV) resulting from thebesian drainage or aortic valvular insufficiency, a thin (1 mm OD) polyethylene tube was inserted into the LV through the mitral valve to serve as a vent. The beating heart was perfused with a modified Krebs-Henseleit (KH, pH 7.4) bicarbonate buffer containing (in mM) 118.0 NaCl, 25.0 NaHCO3, 5.0 dextrose, 4.6 KCl, 2.5 0363-6135/98 $5.00 Copyright r 1998 the American Physiological Society H697 Downloaded from http://ajpheart.physiology.org/ by 10.220.32.247 on July 31, 2017 Hsu, Edward W., Rong Xue, Alex Holmes, and John R. Forder. Delayed reduction of tissue water diffusion after myocardial ischemia. Am. J. Physiol. 275 (Heart Circ. Physiol. 44): H697–H702, 1998.—The apparent diffusion coefficient (ADC) of water after regional myocardial ischemia was measured in isolated, perfused rabbit hearts by using magnetic resonance imaging (MRI) techniques. After ligation of the left anterior descending coronary artery, the ADC of the nonperfused region showed a gradual but significant decreasing trend over time, whereas that of the normally perfused myocardium remained constant. Morphological analysis revealed that the ADC decrease reflected the expansion of a subregion of reduced ADC within the nonperfused myocardium. The dynamics of the diffusion change and the morphological progression of the affected tissue suggest that the ADC decrease may be linked to the onset of myocardial infarction, which is known to involve myocyte swelling. The ADC reduction provides a potentially valuable MRI tissue-contrast mechanism for noninvasively determining the viability of the ischemic myocardium and assessing the dynamics of acute myocardial infarction. H698 REDUCTION OF WATER DIFFUSION AFTER MYOCARDIAL ISCHEMIA Fig. 1. Effect of anisotropic myocardial fiber orientation on diffusion measurement. Ventricular myocardium contains parallel fibers that are characterized by transmural rotation of fiber angle. Because diffusion is faster along fibers than across fibers, encoding diffusion parallel to fiber planes (a) would produce a transmural variation in the measured apparent diffusion coefficient (ADC). In contrast, the epicardial-endocardial axis (b) is mostly perpendicular to fibers and would thus yield a relatively uniform ADC. extracellular ionic environment in the myocardium. Regional ischemia was induced by permanently ligating (with a 4-O silk suture) the left anterior descending coronary artery (LAD) ,1 cm above the imaging plane. The heart was arrested again, and multiple series of diffusion-weighted images (4 images per series with same parameters as the baseline images) were continuously acquired over a period of 2.5 h. At the conclusion of each experiment, gadoliniumdiethylenetriaminepentaacetic acid (Gd-DTPA), an MR contrast agent, was infused, and standard gradient echo images (TE 30 ms, TR 150 ms) were obtained to independently demarcate the nonperfused region. In all, five hearts were included in this study. Data analysis. ADC maps were generated for each series of diffusion-weighted images via pixel-by-pixel nonlinear leastsquares fitting according to I 5 I0 exp(2bD) (1) where I is the signal intensity, I0 is the diffusion-independent signal intensity (including spin density and relaxation effects), and D is the ADC. The acquisition starting time for each image series was assigned to be the time point (in min) of the corresponding ADC map, with t 5 0 representing the preocclusion time point. It is noted that the calculated exponential decay constant (i.e., the ADC) based on images acquired with constant TR and TE would be independent of the longitudinal (T1 ) and transverse relaxation time (T2 ) contrast present in the individual images. Furthermore, the ADC calculation implicitly assumed a monoexponential signal intensity decay as a function of diffusion weighting. Because each signal intensity decay curve was sampled at only four diffusion-weighting b values, no attempt was made to examine changes in the nature of diffusion (e.g., mono-, bi-, or complex exponential decay). The least-diffusion-weighted image (which contained mostly a mixed T1 and T2 contrast due to the relatively short TR and long TE employed) of each series was used as a guide for defining region-of-interest (ROI) templates. ROI templates were generated for the ischemic and nonischemic LV (both on the free wall) and the perfusate standard. Lacking anatomic landmarks, the same nonischemic ROI template was used for successive time points in each heart. In cases when the heart moved between time points (as could happen between the two epochs of cardioplegia, and subsequently when the ischemic myocardium entered into contracture), the template was redrawn so that approximately the same myocardial volume was covered. In contrast, a separate ischemic ROI template was generated for each time point from the region of reduced intensity in the least-diffusion-weighted image. The assignment of the ischemic region was based on the observation that the region was morphologically consistent with the nonperfused area demarcated by Gd-DTPA enhancement. The ischemic ROI template of the first postocclusion time point (t 5 10 min) was also used for the preocclusion (t 5 0) time point. Mean ADC values were calculated over the ROI templates and normalized to that of the perfusate standard at each time point. The temporal trend of diffusion in each myocardial region was determined, to a first approximation, by normalizing the ADC values to their respective preischemic values and calculating the slope of the ADC as a function of time using linear regression. To avoid unintentional bias associated with subjective determination of the onset of decreased ADC, linear regression was performed on the entire time course. Individual slopes were then averaged among the five hearts and compared with the zero-mean hypothesis using Student’s t-test. A difference with P , 0.05 was considered to be statistically significant. Downloaded from http://ajpheart.physiology.org/ by 10.220.32.247 on July 31, 2017 CaCl2, 1.2 KH2PO4, and 1.0 MgSO4. Because of the sensitivity of diffusion-weighted MR images to bulk motion, the heart was arrested before imaging. Cardiac arrest was induced and maintained by perfusing with a cardioplegic solution [modified St. Thomas’ Hospital solution (35)] that consisted of (in mM) 110.0 NaCl, 16.0 MgCl2, 16.0 KCl, 10.0 NaHCO3, 5.0 dextrose, and 1.2 CaCl2. Bovine serum albumin (BSA, 3% wt/vol) was added to both perfusates to minimize interstitial edema formation. MR imaging. MR imaging experiments were conducted using a General Electric 4.7-T Omega CSI instrument equipped with shielded gradients (Accustar). The perfused heart, together with a small sealed tube of perfusate standard (to provide reference for the ADC), was placed inside a 31-mm-diameter loop-gap radio-frequency transmitter-receiver coil. On cardiac arrest (which occurred several minutes after perfusion was switched to the cardioplegic solution), a series of four baseline diffusion-weighted images [256 3 64 zero-filled to 256 3 256 matrix, 40-mm field of view, 4-mm slice thickness, echo time (TE) 50 ms, repetition time (TR) 1 s, and 2 averages] containing a short-axis view of the heart were acquired using a standard spin-echo sequence, with diffusionweighting levels (or b-values) of 67, 266, 599, and 740 s/mm2. In the first heart, diffusion was encoded in the phaseencoding direction. Because this encoding direction had a component parallel to the myocardial fiber orientations in the targeted ischemic myocardium, anisotropic diffusion and the rotation of fibers caused noticeable, systematic transmural variations in image intensity. This dependence of the ADC on the diffusion-encoding direction and the myocardial fiber orientation is schematically explained in Fig. 1. To reduce the nonuniform anisotropic diffusion effects, we encoded diffusion in the next four hearts in the readout direction, which was mostly perpendicular to the regional myocardial fibers. After the acquisition of baseline images, the perfusate was switched back to normal KH buffer, and the heart was permitted to beat for 10 min to allow restoration of a normal H699 REDUCTION OF WATER DIFFUSION AFTER MYOCARDIAL ISCHEMIA To measure the morphological progression of the ischemic myocardium that showed reduced ADC, we selected a threshold on the ADC maps at 50% of the mean ADC of the perfusate standard (i.e., pixels with higher ADC values were eliminated). The 50% threshold value was selected because the ADC in the core of the ischemic regions decreased below, while the nonischemic regions remained above, the threshold at longer time points. The number of pixels within a contiguous region inside the hypoperfused LV wall was counted. Because small, isolated areas were likely dominated by image noise, contiguous areas of less than three pixels in size were excluded from the tally. The total area was normalized to the size of the corresponding ischemic LV ROI, and the morphological progression was characterized by performing leastsquares curve fitting of the percent area %P as a sigmoid logistic function of time according to the general form vf 2 vi 11 t 1t2 h (2) The fitted parameters vi, vf, h, and t corresponded to (for negative h) the initial and final values of %P, the exponential rate of change, and the linear time-compression factor, respectively. The function was chosen because the morphological progression of tissue injury was found to be a sigmoid logistic function (20); however, a different basis function was used in the present study to better characterize slow changes in the early postocclusion time points. RESULTS Representative images of an isolated, perfused heart are shown in Fig. 2, including least-diffusion-weighted images obtained before (A) and 10 min after LAD occlusion (B), a Gd-DTPA-enhanced image (C), and a corresponding ADC map at t 5 150 min (D). The images contain a short-axis view of the heart in which the LV appears as an annular-shaped region. The nonperfused LV appears in the Gd-DTPA-enhanced image (Fig. 2C) as a relatively bright area because the normally perfused myocardium has a shorter T2 from the presence of high concentration of the contrast agent. The postocclusion image (Fig. 2B) contains an LV region that has reduced signal intensity, and the region is morphologically similar to the hypoperfused zone demarcated in Fig. 2C. On the other hand, the ADC map (Fig. 2D) shows that the ADC within the hypoperfused LV has decreased; however, the area of reduced ADC is smaller than the hypoperfused region. The calculated slopes of the ischemic and nonischemic ADC as functions of time are tabulated in Table 1. The normalized ADC of the ischemic region shows a statistically significant (P , 0.03) decreasing trend over time, with an average slope of 21.38 6 0.20 3 1023 min21 (n 5 5, 6SE). In contrast, no significant trend was found in the ADC of the nonischemic region (0.01 6 0.10 3 1023 min21 average slope, P . 0.8). The linear regression results are summarized graphically in Fig. 3. Individual results of the sigmoid logistic regression describing the morphological progression of the ischemic ADC reduction are tabulated in Table 2. Figure 4 shows the average percent areas of reduced ADC and the response reconstructed from averaged curve-fit Fig. 2. Representative images of an ischemic heart. A–D contain short-axis view of heart showing annular left ventricle (LV). Images are least-diffusion-weighted spin-echo images obtained before (A) and 10 min after ischemic insult (B), gadolinium-diethylenetriaminepentaacetic acid-enhanced gradient echo image that delineates hypoperfused LV as area of higher intensity (C), and calculated ADC map (to be distinguished from a diffusion-weighted image) at 150 min after left anterior descending coronary artery (LAD) occlusion, containing a region of reduced ADC within the hypoperfused LV (D). Circular object at top left of cross-sections is perfusate standard. Images have been numerically scaled to enhance contrast. parameters. The results indicate that the ischemic myocardium showing reduced ADC appears after LAD occlusion and gradually increases in size over time. Extrapolating from the average curve-fit response, the percent area of reduced ADC reaches %P 5 50 at approximately t 5 130 min after LAD occlusion. DISCUSSION Comparison between the least-diffusion-weighted images before and immediately after LAD occlusion (Fig. Table 1. Slopes of regional ADC as a function of time after LAD occlusion Slope, 31023 min21 Heart Ischemic LV Nonischemic LV 1 2 3 4 5 Mean 6 SE 22.045 21.612 21.194 20.933 21.107 21.38 6 0.20 P , 0.03 0.168 20.044 20.341 0.044 0.243 0.01 6 0.10 P . 0.8 Mean apparent diffusion coefficient (ADC) of each region was normalized to respective perfusate standard and preischemic value, and slope was determined by linear regression. P value is determined by testing group average slope to zero-mean hypothesis using Student’s t statistics. LAD, left anterior descending coronary artery. LV, left ventricle. Downloaded from http://ajpheart.physiology.org/ by 10.220.32.247 on July 31, 2017 %P 5 vi 1 H700 REDUCTION OF WATER DIFFUSION AFTER MYOCARDIAL ISCHEMIA 2, A and B, respectively) reveals a region of reduced intensity in the LV of the postocclusion image. The anatomic similarity between the region and the nonperfused area demarcated by Gd-DTPA enhancement (Fig. 2C) indicates that the intensity reduction is linked to the perfusion deficit (i.e., ischemia) in the myocardium. Similar intensity changes after regional myocardial ischemia were reported in a previous study (6). Qualitatively, Fig. 3 indicates that the ADC of the ischemic myocardium appears to remain constant initially, then steadily decreases after 60 min following LAD occlusion. Although the linear regression analysis cannot determine the transition time point in which the ADC reduction begins and is likely to underestimate the slope of the decrease, the decreasing trend of the ADC of the ischemic LV was found to be significant (Table 1). In contrast, the ADC of the nonischemic myocardium remained unchanged over time. The morphological analysis summarized in Table 2 and Fig. 4 Table 2. Least-squares curve-fit parameters describing morphological progression of ischemic myocardium showing decreased ADC Heart vi vf h t, min 1 2 3 4 5 Mean 6 SE 3.0 4.6 3.9 7.9 10.3 5.9 6 1.4 290 70 46 68 46 104 6 47 21.63 21.80 25.87 22.64 26.06 23.60 6 0.98 263 63 103 134 121 137 6 34 The area that showed ADC values lower than 50% of perfusate ADC, as a percentage of the ischemic myocardium area (%P), is fitted to Eq. 2 (see Data analysis). Parameters: vi and vf , initial and final values of %P; h, exponential rate of change; t, linear timecompression factor. Fig. 4. Progression of area within ischemic myocardium showing decreased ADC. No. of pixels that showed ADC values ,50% of perfusate ADC was measured and normalized to area of ischemic myocardium. Data points and error bars represent average (n 5 5) percent areas and 6SEs, respectively, at various time points. Response of each heart was curve-fitted to a sigmoid logistic function (Eq. 2). Solid line represents response reconstructed from averaged curve-fit parameters reported in Table 2. indicates that the ADC decrease in ischemic myocardium reflects an expansion of the area that has reduced ADC within the hypoperfused myocardium rather than a uniform ADC decrease in the entire hypoperfused tissue. These results, combined, suggest that the temporal and morphological progression of the ADC reduction in the ischemic myocardium is a delayed and gradual process. The dynamics of the ADC decrease may reflect the delayed myocyte swelling after myocardial ischemia. Electron microscopic examination of cellular ultrastructure has revealed that little or no cell swelling occurs during the reversible and early stages of irreversible ischemic injury (13). Direct measurement of tissue water and electrolyte content has found that the ischemic canine myocardium is capable of at least partial cell volume regulation through anaerobic glycolysis (14). The ability of myocytes to regulate cell volume is lost after 60 min of ischemia following the onset of irreversible injury (i.e., myocardial infarction). The transition time point between reversible and irreversible cell damage is likely dependent on the severity of ischemia, degree of collateral arterial flow, and the animal species. Studies of dog hearts under total ischemia have found evidence of irreversible damage as early as 20–40 min after ischemic insult (14). However, it has been reported that the jeopardized myocardium can be salvaged by reperfusion as late as 3–6 h after ischemia (25). The delayed and gradual ADC decrease after myocardial ischemia is markedly different from the dramatic change observed in cerebral ischemia. The ADC decrease in the brain has been found to take place within Downloaded from http://ajpheart.physiology.org/ by 10.220.32.247 on July 31, 2017 Fig. 3. ADC of ischemic and nonischemic myocardium as functions of time after LAD occlusion. Each data point represents averaged ADC (n 5 5) normalized to both mean ADC of water standard and the preocclusion (t 5 0) value. Error bars represent 6SEs. Solid lines are reconstructed from averaged parameters of individual linear regression reported in Table 1. REDUCTION OF WATER DIFFUSION AFTER MYOCARDIAL ISCHEMIA producing a considerable through-plane volume-averaging effect in the observed diffusion characteristics. Nevertheless, the present study demonstrates the potential to noninvasively visualize morphological progression of acute myocardial tissue injury through alterations in the tissue ADC. The noninvasive approach is expected to have significant implications for determining infarct size in assessing, for example, the effectiveness of pharmacological protective agents in reducing irreversible tissue injury. Conventional histological methods require the heart to be mechanically sectioned and therefore preclude quantitation of the infarct size in the same heart at different time points. A noninvasive technique is advantageous because repeated measurements can be performed on the same hearts at different time points. Not only does the technique dramatically reduce the number of animals that need to be killed [e.g., 29 animals were used by Miura et al. (20) compared with 5 used in the present study], but also repeated measurements provide improved statistical power by controlling for the heterogeneity in the responses among different animals. In conclusion, the tissue ADC has been shown to decrease after regional myocardial ischemia. The reduction reflects the expansion of a subregion of ischemic myocardium that has decreased ADC. In contrast to acute cerebral ischemia, ischemic ADC reduction in the myocardium is a delayed and gradual process and occurs subsequent to observable T1 and T2 contrast changes. The temporal and morphological progression of the ADC reduction suggests that the diffusion change may be related to the onset of myocardial infarction, which is known to involve myocyte swelling. These findings are promising for using the ADC reduction as an MR imaging tissue-contrast mechanism to noninvasively determine the viability of the ischemic myocardium and to assess the dynamics of acute myocardial infarction. The authors gratefully acknowledge the advice and support of Dr. S. Blackband. This work was supported by an Independent Investigator Grant from the Whitaker Foundation (J. R. Forder). E. W. Hsu was supported by a Howard Hughes Predoctoral Fellowship. Present address for E. W. Hsu: Center for In Vivo Microscopy, Duke Univ. Medical Center, DUMC Box 3302, Durham, NC 22710. Address for reprint requests: J. R. Forder, Div. of NMR Research, Dept. of Radiology and Radiological Sciences, Johns Hopkins Univ. School of Medicine, 217 Traylor Bldg., 720 Rutland Ave., Baltimore, MD 21205-2195. Received 15 July 1997; accepted in final form 16 April 1998. REFERENCES 1. Atalay, M. K., S. B. Reeder, E. A. Zerhouni, and J. R. Forder. Blood oxygenation dependence of T1 and T2 in the isolated, perfused rabbit heart at 4.7 T. Magn. Reson. Med. 34: 623–627, 1995. 2. Axel, L., and L. Dougherty. Heart wall motion: improved method of spatial modulation of magnetization for MR imaging. Radiology 172: 349–350, 1989. 3. Beneviniste, H., L. W. Hedlund, and G. A. Johnson. Mechanism of detection of acute cerebral ischemia in rats by diffusionweighted magnetic resonance microscopy. Stroke 23: 746–754, 1992. Downloaded from http://ajpheart.physiology.org/ by 10.220.32.247 on July 31, 2017 minutes after the onset of ischemia (7) before any detectable relaxation contrast changes (21). 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