Cite this asFasano A, Anfuso L (2020) Esophageal temperature evolution during high power short duration ablation: Numerical simulations and clinical suggestions. J Cardiovasc Med Cardiol 7(2): 125-128. DOI: 10.17352/2455-2976.000126
In recent times electrophysiologists started considering the possibility of performing Radiofrequency (RF) ablation for the treatment of atrial fibrillation by delivering shorter pulses of larger power (e.g. 60W, 6s applications). Such a technique is known as High Power Short Duratio (HPSD) Ablation [1-5].
The key point of HPSD ablation is that it allows getting results quite comparable to the traditional approach in shorter time, thus reducing patients’ discomfort and fluoroscopy time. Some electrophysiologists , are even testing very HPSD (90W, 4s applications). It is well known that esophageal thermal lesions are among the most feared complications. In this respect, it has been pointed out that HPSD ablation may force Luminal Esophageal Temperature (LET) to reach dangerous values . Here we want to exploit a mathematical model introduced in a previous paper about traditional RF ablation in order to investigate the thermal effects of a HPSD procedure on the esophagus. More precisely, we address the following questions:
Is HSPD safe and is there a preferable sequence when ablating around the Pulmonary Vein (PV) closest to the esophagus?
How sensitive is LET increase to apparently unimportant differences in the patient’s anatomical configuration? This aspect can be of great importance considering that the tissues compression induced by exerting a contact force on the ablator may reduce the esophagus-ablator distance to some extent.
In several papers [8-12], mathematical models have been used to investigate the thermal field around the ablator, both for RF and cryoablation procedures.
Here we adopt the model by Fasano, et al. . The equations to be integrated are the so-called bioheat equation, describing the evolution of the thermal field with a source term due to RF power absorption, , (T temperature, ρ density, c specific heat, k thermal conductivity, Q heat supply rate p.u. volume, ω blood perfusion rate, index b refers to blood, not indexed symbols refer to tissues), and the equation for the electric potential V, ∆V = 0, (in both equations ∆ is the Laplace operator). The heat source Q due to RF power absorption (metabolic heat is neglected) is given by where σ is the electric conductivity and E=|∇V|is the electric field (the factor 1/2 accounts for the fact that the potential is computed as a static quantity while the RF field is oscillating).
The equations above are solved in a domain representing the patient’s thorax, sketching the heart as a fixed domain (heart beats have little influence on the thermal field), as shown in Figure 1. keeping into account the medium inhomogeneity. For more details on the model and for the values used for the various thermal and electric parameters the reader is referred to quoted paper.
An irrigated ablator is applied at 6 evenly spaced points around the ostium of a PV (Figure 2) facing the esophagus (the worst situation). Interlesion distance is 5.2mm (such a distance is suggested to be less than 6mm [4,13].
Voltage is tuned to achieve a power of 60W. Each application has the duration of 6 sec. Time between successive applications is 50 sec. We compute the LET time variation caused by the cumulated effect of repeated ablations in the presence of a multisensor esophageal thermal probe (ETP), with the central sensor placed at the point closest to the ablator. Specific reference is made to the FIAB 7-sensor Esotherm Multi probe. The choice of the 50 sec time between successive application is tailored to the selected geometry. For our purposes a shorter time would have required a larger distance between the esophagus and the ablator in order to attain a similar result. The study of a correlation between such a time and the anatomical configuration giving comparable LET evolution is beyond the scope of the present paper.
We have considered three geometrical settings:
A. Left Atrium (LA) thickness 2.3mm, epicardial fat layer thickness 1mm, esophagus thickness 2.1mm, distance between esophagus and fat layer 0.5mm. PV cross section area 0.785cm2, blood discharge through the 4 PVs and through each cardiac chamber 5000cm3/min. These conditions correspond to frequent, not particularly critical – but border to critical - physiological data [14, 15].
B. Esophagus thickness 2.5mm, distance between esophagus and fat layer 1.5mm, other data as in (A). The overall sensor-ablator distance is thus increased by 1.2mm compared to case (A).
C. Anatomical configuration similar to (A), but with slightly thinner tissue layers: LA 2mm, esophagus 2mm, no fat layer. Cumulative reduction of sensor-ablator distance with respect to case (A) is 1.4mm.
For (A) and (B) we have considered two sequences of applications:
i. Starting the sequence from Point 1, Figure 2.
ii. Starting the sequence from Point 4, Figure 2.
For (C) we limited ourselves to the sequence (I).
The results shown here refer to the temperature computed on the ETP central sensor. Figure 3 compares the numerical simulations for the geometry (A) in the two sequences (I) (green line) and (II) (red line). Dots represent the temperatures taken every 2 sec. In the sequence (I) LET increases from 37°C to a maximum of 39.1°C, in the sequence (II) it climbs to 39.7°C. It means that if we start ablating from the remotest point, when we come to the closest one the heat already accumulated pushes LET to higher values. The LET increase rate in the first application of Sequence I is (0.13°C/s), a rather large value that would be alarming in the traditional procedures, but is not here because of the short application time. Precisely the same rate is observed in the fourth ramp of Sequence II, which refers once more to Point 1. Note that if the threshold LET value 39.5° is adopted, as it frequently happens, Sequence II would trigger the alarm, while Sequence I would not.
Figure 4 illustrates the same comparison between Sequences I and II with reference to the geometrical Setting (B)
As expected, the slight increase of the sensor-ablator distance yields a moderate lowering of LET, the maximum difference between Sequence I and Sequence II being now reduced to 0.4°C. Comparison between Setting (A) and Setting (B), confined to Sequence I, is shown in Figure 5.
The slight increase of the sensor-ablator distance results in lowering the maximum LET by approximately 0.5°C. A similar difference is detected comparing the respective results for Sequence (II) (not shown here).
In contrast to the moderate changes when passing from (A) to (B), the results obtained for Setting (C), where the sensor-ablator distance is slightly reduced, show an impressive increase of the maximum LET. Since we have learned that Sequence (I) is the most convenient, we limited the computation to that case. Figure 6 illustrates the comparison between (A) and (C).
The maximum LET for Setting (C) is 45.8°C, i.e. 6.7°C larger than in Case (A). This is a striking evidence that very small tissues compression can lead to definitely dangerous LET increase. LET stays above 40°C during almost all the procedure (for the considered PV) and beyond 42°C for about 2.5 min, which is unacceptable. Equally impressive is the increase in the LET rate of change at the first application, passing from 0.13°C/s (Setting A), to 0.3°C/s (Setting C). The maximum LET increase detected by Barbhaiya, et al. . in a clinical procedure was 5.8°C, thus in a comparable range.
The remark about the LET rate of change stresses the importance of the ETP response time. Such a feature is not enough emphasized in the literature concerning atrial ablation, but it is actually quite critical in the presence of rapidly changing temperatures (in such conditions response times exceeding 2 sec are likely to provide false information on LET evolution ).
Our simulations show that HPSD ablation procedures are safe for most anatomical configurations. The Setting (A) represents a borderline configuration in the sense that a reduction of the esophagus-ablator distance as small as 1.4mm leads to a dramatic LET increase (Setting C), while a comparatively small increase has little effect (Setting B). It must be kept in mind that contact force applied to the ablator may produce small tissue compression, thus potentially creating a dangerous situation. Such a possibility had been stressed in the literature . It seems therefore crucial to monitor the esophageal temperature to ascertain whether a HPSD ablation is feasible or not, or in any case to calibrate the procedure to the patient’s needs. LET variations depend also on the ablation sequence. Starting from the point in the PV which is closest to the esophagus leads eventually to a maximum LET that is lower than the one attained when starting from the farthest point (a useful indication for the clinician).
Owing to the possibility that LET increase rate can assume large values, it is very important that the response time of the ETP used is sufficiently small (less than 2s), otherwise the probe is likely to provide the operator with deceptively safe information.
We have computed the thermal field generated by an irrigated ablator during a HPSD ablation procedure. We established that
• With respect to a rather frequent anatomical configuration (Setting A), the procedure is safe.
• It is convenient to start the ablation sequence on a pulmonary vein from the point which is closest to the esophagus, otherwise LET will reach higher values.
• The selected reference configuration (Setting A) is border to critical: while a small increase of the sensor-ablator distance produces modest changes in LET, a comparably small reduction pushes LET to clearly unsafe values, since the esophagus is exposed to a steep thermal gradient.
• We get a clear indication that LET monitoring is of crucial importance and more specifically that it is necessary to use fast responding ETPs, since the LET variation speed can be very large.
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