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J Am Coll Cardiol, 2001; 38:385-393 © 2001 by the American College of Cardiology Foundation |


a St. Marys Hospital and Imperial College School of Medicine, London, United Kingdom
Northwestern Memorial Hospital, Chicago, Illinois, USA
Manuscript received January 15, 2000; revised manuscript received March 1, 2001, accepted April 23, 2001.
Reprint requests and correspondence: Dr. Richard Schilling, Waller Department of Cardiology, St. Marys Hospital, Praed St., London W2 1NY, United Kingdom
r.schilling{at}ic.ac.uk
| Abstract |
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This study was done to characterize human right atrial (RA) flutter (AFL) using noncontact mapping.
BACKGROUND
Atrial flutter has been mapped using sequential techniques, but complex anatomy makes simultaneous global RA mapping difficult.
METHODS
Noncontact mapping was used to map the RA of 13 patients with AFL (5 with previous attempts), 11 with counterclockwise and 2 with clockwise AFL. "Reconstructed" electrograms were validated against contact electrograms using cross-correlation. The Cartesian coordinates of points on a virtual endocardium were used to calculate the length and thus the conduction velocity (CV) of the AFL wave front within the tricuspid annulus-inferior vena cave isthmus (IS) and either side of the crista terminalis (CT).
RESULTS
When clearly seen, the AFL wave front split (n = 3) or turned in the region of the coronary sinus os (n = 6). Activation progressed toward the tricuspid annulus (TA) from the surrounding RA in 10 patients, suggesting that the leading edge of the reentry wave front is not always at the TA. The IS length and CV was 47.73 ± 24.40 mm (mean ± SD) and 0.74 ± 0.36 m/s. The CV was similar for the smooth and trabeculated RA (1.16 ± 0.48 m/s and 1.22 ± 0.65 m/s, respectively [p = 0.67]) and faster than the IS (p = 0.03 and p = 0.05 for smooth and trabeculated, respectively).
CONCLUSIONS
Noncontact mapping of AFL has been validated and has demonstrated that IS CV is significantly slower than either side of the CT.
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The hypothesis for this study was that AFL is the result of a macroreentry circuit that is not dependent on a complete line of block along the CT, nor on slowing of conduction within the IS.
| Methods |
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Mapping procedure. The local ethics committees, whose guidelines were followed, approved the study. Quadripolar catheters were placed in the proximal CS, the high RA and right ventricular apex. A 7F deflectable mapping/ablation 4-mm tip catheter was advanced to the RA via the right femoral vein. Systemic arterial blood pressure was continuously monitored via a 6F femoral arterial sheath. A 9F sheath placed in the left femoral vein was used to introduce the noncontact mapping catheter. Contact catheter data and surface electrocardiograms (ECGs) were recorded simultaneously on a conventional electrophysiology system.
Noncontact mapping system
The noncontact mapping system (EnSite 3000, Endocardial Solutions, St. Paul, Minnesota) has been described in detail elsewhere (7). Briefly, the system consists of a noncontact catheter (9F) with a multielectrode array (MEA) surrounding a 7.5-ml balloon mounted at the end. Raw data detected by the MEA is fed to a silicon graphics workstation via an amplifier.
Before deployment of the MEA, patients were given 10,000 IU heparin with boluses to maintain activated clotting time between 300 and 400 s throughout the study. The MEA catheter was deployed over a 0.035-in. (0.0889 cm) J-tipped guide wire advanced either to the SVC (n = 7) or the pulmonary outflow tract (n = 6), having been positioned using a 7F multipurpose catheter (Fig. 1). This was done to cant the balloon toward an area of interest (the atrioventricular junction), as previous data have demonstrated that the accuracy of electrogram reconstruction is greater with increasing proximity to the endocardium (7).
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Reconstruction of electrograms
The electrical activity detected by the electrodes on the MEA is generated primarily by the potential field on the endocardial surface. Using techniques to resolve these potentials, the system is able to reconstruct >3,000 unipolar electrograms simultaneously and superimpose them onto the virtual endocardium, producing isopotential maps (Fig. 2) with a color range representing voltage. Reconstructed electrograms can also be selected from sites on the virtual endocardium and displayed individually.
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Validation of electrogram reconstruction. Accuracy of electrogram reconstruction was assessed by cross-correlation between reconstructed and contact electrograms from the same endocardial location (7).
Distance and conduction velocity measurements.
The noncontact system displays the Cartesian coordinates relative to the MEA center (in mm) of points on the virtual endocardium (8). It is therefore possible to derive straight-line distances between two points with the formula:
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Definitions. ANATOMICAL TERMINOLOGY. Anatomical nomenclature was used that reflected the true orientation and positioning of the human heart in the thorax. Using this format the SVC and RA appendage are superior and the IVC and the IS are inferior to the TA. The His bundle is positioned in the posterosuperior aspect of the TA, the CS in the posteroinferior aspect of the TA, and the CT is located in the lateral wall of the RA and is oriented from superior to inferior (9).
AFL
Atrial flutter was defined as a rapid atrial rate (>200 beats/min) characterized by a constant cycle length, polarity, morphology and amplitude of the recorded bipolar electrograms and as the presence of a single constant macroreentrant circuit with a constant atrial activation sequence (10). Cycle length was determined from unipolar reconstructed electrogram intervals and confirmed using contact electrograms.
IS
The tricuspid annulus-inferior vena cava isthmus was defined by anatomical landmarks identified using fluoroscopy and electrograms and was considered to extend from the CS posteriorly, the TA superiorly, and the IVC inferiorly. The anterior border of the IS was considered as a line joining the anteroinferior border of the TA with the anterior border of the IVC. It was further defined electrophysiologically by the demonstration of a distinct narrowing and expansion of the AFL wave front on isopotential maps as it entered and exited the IS.
Double potentials
These were defined as bipolar atrial electrograms with two discrete potentials per complete reentry circuit separated by either an isoelectric baseline or a low amplitude interval (11). When fractionated and double potentials were observed, local activation was considered to have occurred at the timing of the electrogram component with the largest negative deflection.
Statistics. Data are presented as means, SD and 95% confidence intervals (CI). Means of continuous, normally distributed data were compared using the Student t test.
| Results |
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AFL. Mean AFL cycle length was 240.92 ± 35.45 ms, with no difference between reconstructed and contact electrogram measurements. All 13 patients had IS-dependent counterclockwise (n = 11) or clockwise (n = 2) AFL. In none of the patients with prior ASD repair was the ASD patch used as a barrier defining the AFL circuit. Apart from the direction, the AFL circuit and CV did not differ significantly between the patients with clockwise and counterclockwise AFL.
Validation of electrogram reconstruction during AFL
Cross-correlation of reconstructed and contact AFL electrograms recorded at 127 different locations was 0.73 ± 0.18 for all distances and 0.8 ± 0.11 for the 62 locations <35 mm from the center of the MEA (p < 0.001), a phenomenon described before (7). Timing difference between contact and reconstructed electrograms was 7.9 ± 12.1 ms for all locations and 3.9 ± 3.7 for those <35 mm from the MEA (p < 0.001).
Characteristics of IS activation
The AFL wave front was seen throughout the entire IS in nine patients with some signal attenuation in three patients with previous ablation procedures. In one patient signal attenuation prevented the IS being clearly defined electrophysiologically. In the remaining patients the IS extent was described using a clock-face projected onto the TA while viewed in the left anterior oblique (LAO) projection. The IS length was seen to extend from 4 h 30 min to 6 h 30 min with expansion/narrowing of the wave front being distant from the CS, which most commonly positioned at 4 oclock (Table 1). In three patients the wave front was seen to split as it passed the CS and the region of the eustachian ridge, one wave front passing inferiorly and one superiorly to the CS before fusing again. In seven patients a single activation wave front slowed and turned superiorly toward the TA in the region of the CS and eustachian ridge, and in two patients the wave front slowed and emerged from the IS inferiorly, suggesting some variation of conduction properties in the posterior IS.
Lateral wall activation patterns during AFL
A line of block was seen on the posterolateral RA wall in 12 patients during AFL. This was confirmed by the presence of double potentials in electrograms reconstructed along this line (Fig. 2A,B). In 10 patients the line of block extended from the IVC to the SVC. In one patient the line of block extended superiorly from the IVC to the mid-lateral RA but did not reach the SVC. In one patient the line of block extended from the SVC to the low RA, but slow activation was seen progressing over a 70-ms interval between the IVC and the CT, which was confirmed by fractionated, reconstructed electrograms of similar duration (Fig. 3A,B).
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| Discussion |
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Validation of noncontact mapping. Electrogram reconstruction using noncontact mapping has been validated in the human ventricle during sinus rhythm (7) and ventricular tachycardia (12) and the RA during atrial fibrillation (13). This is the first validation of AFL, and the results are similar to those during atrial fibrillation.
Location of the re-entry circuit in AFL. The majority of the AFLs are caused by a macrore-entry circuit confined to the RA, which is dependent on anatomical obstacles within the RA (1,14). Previous investigators have concluded that AFL may (4,5) or may not (6) be dependent on slow conduction in the IS. The inferior turning point has been identified as the IS (2,3,15), and the upper turning point is located either anterior or posterior to the SVC (4,16). It has also been suggested that the re-entry wave front producing counterclockwise AFL in the RA rotates around the TA, with the TA constituting the anterior continuous barrier around which the wave front rotates (17), with activation of the rest of the RA radiating from the TA.
The noncontact mapping system has produced high-resolution maps of the entire AFL circuit using data acquired simultaneously. The majority of the AFLs described here are consistent with previous observations that the TA and CT serve as continuous barriers to conduction, but several new observations have been made. First, the leading edge of activation is usually not directly around the TA. In addition, one of the RAs mapped during AFL had a break in the line of block in the CT, demonstrating that it is not always a continuous line of block.
The role of the CT. The presence of double potentials (3,18) during AFL has suggested the presence of barriers to conduction (11,19) in the lateral RA, and it has been inferred that these may be the center of the AFL re-entry circuit (3). Intracardiac echocardiography has confirmed that these electrical barriers are related to the structures of the CT and the eustachian ridge (3), but the nature of the conduction block in these regions has not been clearly defined; it has been postulated that the presence of conduction block differentiates between patients with and without AFL.
Noncontact mapping during AFL has confirmed the presence of a line of conduction block in the lateral RA that is compatible with the location of the CT with both double potentials on reconstructed electrograms in this region and demonstration of conduction block on isopotential maps. Noncontact mapping has demonstrated that this line of conduction block is not complete in all patients during AFL. The AFL wave front has been seen to turn from the posteroseptal RA to the anterolateral RA at the level of the midlateral RA in one patient. In another patient the main wave front was seen to split, with one daughter wave front turning at the level of the IVC with the slow conduction of the wave front through this region preventing premature activation and termination of the re-entry circuit.
Lower-loop re-entry has already been described by Shah et al. (5) and Cheng et al. (20,21) using recordings acquired from catheter electrode recordings taken from the TA and septum. They were unable to distinguish between lower-loop re-entry and a focal atrial tachycardia located at the inferior-anterior aspect of the RA, but they made the point that lower-loop re-entry was noninducible after IS ablation, and it seemed reasonable to assume that this rhythm was isthmus dependent. Cheng et al. also concede that they had insufficient sites, and specifically no data recorded from the posterior RA. Larger numbers of electrograms allowed us to confirm the deductions made by Cheng et al. that the AFL wave front can pass through the inferior CT.
Activation in the region of the CS os. The region of the triangle of Koch and posterior IS has complex anatomy, comprised in part by the eustachian ridge extending into the tendon of Todaro and the CS. Intraoperative mapping in one case of common AFL has revealed slow conduction between the CS and the tricuspid valve colliding with another wave front of activation traveling between the CS and the IVC (22). Slow and irregular activation seen in Kochs triangle may be due to fiber arrangement (23), and it has also been noted that circumferential fibers found around the rest of the TA may be absent in this area (24). Noncontact mapping demonstrated that the wave front slows and turns in the posterior region of the triangle of Koch in the majority of patients, suggesting that it encounters a line of block at the site of the eustachian ridge. Splitting of the wave fronts in this region was also seen, and this may have been a feature of the wave front passing around the CS os. Alternatively, part of the activation wave front may have passed under the eustachian ridge, becoming intramural and thus not visible to the noncontact system. Only two patients with clockwise AFL were included in this series, but a similar activation pattern was seen in the region of the eustachian ridge in these patients, indicating that this is not specific to activation of the wave front direction.
Conduction velocity within the IS. The mean CV of the AFL wave front within the IS was slower than smooth and trabeculated RA adjacent to the CT but only when patients with previous radiofrequency were included in the analysis. This may indicate that IS conduction is not slower than the rest of the RA unless the patient has had previous radiofrequency to the IS; however, the patient numbers studied were small, and this cannot therefore be substantiated by this study, but it is consistent with previous studies. Kinder et al. (6) concluded that there is no functional slowing of conduction within the IS during AFL compared with sinus rhythm, but CV was not measured and comparison with the rest of the atrium was not performed. Tai et al. (4) measured IS CV during pacing (but not AFL) by dividing the bipolar electrogram intervals by interelectrode spacing and found that IS CVs were lower than in our study (0.336 ± 0.045 m/s) and were lower in the mid IS compared with the lateral IS. This may be explained because distance traveled across a complex curved surface is likely to be underestimated by the distance between electrodes on a straight catheter bridging this distance. Also, using bipolar electrograms makes clear definition of local activation difficult.
Study limitations. A proportion of the patients studied had been on amiodarone therapy, which may have affected CV; the results should thus be interpreted with caution. In measuring CV distance, measurements were calculated using a series of short straight-line distances that are an approximation of the true curved surface of the RA and are therefore subject to error. Calculating the shortest distance that a wave front travels is difficult on complex curved surfaces, which is why wave front CV was measured only in portions of the AFL circuit where passage of the leading edge was clearly defined (i.e., within the IS and on either side of the CT). The calculation of CV using contact arrays is also prone to these problems because it is calculated by measuring distances between electrodes on the arrays, which are clearly short straight-line distances. Also, acquisition of clear signals requires that pressure be used to achieve contact between the array and epicardium, which may distort the anatomy and affect the CV.
Conclusions. Using noncontact mapping we have produced the first high-resolution maps of the intact human RA during AFL. We confirm previous observations that the line of block represented by the CT is not necessarily complete in all patients. Maps of activation at the triangle of Koch explain why a line of block between the TA and CS os may terminate some cases of AFL because there is conduction block posteroinferior to the CS os possibly related to the eustachian ridge. The AFL wave front CV within the IS has been measured and confirmed that CV may be, but is not always, slower than the rest of the AFL circuit.
| Footnotes |
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| References |
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