EFFECTS OF INTRACAVITARY BLOOD-FLOW AND ELECTRODE-TARGET DISTANCE ON RADIOFREQUENCY POWER REQUIRED FOR TRANSIENT CONDUCTION BLOCK IN A LANGENDORFF-PERFUSED CANINE MODEL
Ta. Simmers et al., EFFECTS OF INTRACAVITARY BLOOD-FLOW AND ELECTRODE-TARGET DISTANCE ON RADIOFREQUENCY POWER REQUIRED FOR TRANSIENT CONDUCTION BLOCK IN A LANGENDORFF-PERFUSED CANINE MODEL, Journal of the American College of Cardiology, 31(1), 1998, pp. 231-235
Objectives, We sought to quantify the effects of electrode-target dist
ance and intracavitary blood how on radiofrequency (RF) pow er require
d to induce transient conduction block, using a Langendorff-perfused c
anine ablation model. Background. Given the thermally mediated nature
of RF catheter ablation, cooling effects of intracavitary blood flow a
nd electrode-target distance will influence lesion extension and geome
try and electrophysiologic effects. Methods. In eight Langendorf-perfu
sed canine hearts, the right ventricular free wall was opened, and the
right bundle branch (RBB) carefully localized by multielectrode activ
ation mapping, The right atrium was paced at cycle length of 500 ms, P
roximal and distal electrodes were attached at the endocardial aspect
of the RBB, and the perfused heart was submerged in heparinized blood
at 37 degrees C, A standard 4-mm tip ablation electrode was positioned
at a constant contact pressure of 5g between the two electrodes at th
e site of maximal RBB potential (0 mm) and 2 and 4 mm distant from thi
s site along a line perpendicular to the RBB, RF pulses (500 kHz) were
delivered for 30s at 0.5-W increments until transient bundle branch b
lock, In four hearts, intracavitary flow was simulated by directing a
30-cm/s jet of blood parallel to the septum at the ablation site, and
the protocol was repeated to assess the effects on power required for
block In one heart, the effect of variable flow was assessed (0, 15 an
d 30 cm/s). Results. An exponential distance related increase was seen
in power required for block, from 1.8 +/- 0.9 W (mean +/- SD) at 0 mm
to 5.4 +/- 1.1 W at 4 mm. In the presence of 30-cm/s flow, an increas
e to 3.9 +/- 0.8 W at 0 mm and 13.1 +/- 2.4 W at 2 mm was seen. At 4 m
m, coagulum formation invariably occurred before block could be induce
d, For 15-cm/s flow, less power was required: 3 and 7 W at 0 and 2 mm,
respectively. Conclusions. Increasing the ablation electrode-target d
istance causes an exponential increase in power required for conductio
n block; this relation is profoundly influenced by intracavitary flow,
Given the geometry of endomyocardial RF lesions, these findings are p
articularly relevant for directly subendocardial ablation targets. (C)
1998 by the American College of Cardiology.