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1/10

Q: If you could deliver 30 W of RF energy for 30 sec using any of the ablation (abl) electrodes shown in the figure, which RF ablation catheter creates larger ablation lesion size?

A: Let’s talk about how the RF abl lesion is formed.
2/10
The size of the lesion created by RF is determined by the amount of tissue heated to >>50°C.

Heat is generated when charged ions in tissue oscillate rapidly (following the alternating RF current) converting RF energy to kinetic/thermal energy (Ohmic/Resistive Heating)
3/10
According to Ohm’s law, the amount of power per unit volume (resistive heating) equals the square of current density times the impedance (resistance) of the tissue, which in turn, is a function of the square of RF current density.
4/10
RF current density (and power dissipation per unit volume) decreases rapidly (with the 4th power of distance) as it distributes radially from abl electrode. Thus, only a thin (<2 mm) rim of tissue in contact with the electrode is directly heated by RF (Resistive Heating)
5/10
Heat is then conducted into deeper layers of myocardium (Conductive Heating), which extends the abl lesion size.

Heat is also conducted back to the circulating blood pool and to the metal ablation electrode. This heat loss opposes myocardial heating and lesion formation.
6/10
When power output is fixed, a larger abl electrode creates smaller lesion size by 2 mechanisms:
(1) It exposes more of the electrode surface area to the cooling effect of blood.
(2) It reduces RF current density (due to larger surface area), which reduces tissue heating.
7/10
Active cooling of the abl electrode and tissue surface by irrigation increases the amount of heat loss from the tissue (acting as a heat sink) and can reduce lesion size in the setting of a fixed RF power delivery.
8/10
In our question, power delivered to tissue is fixed. However, the proportion of heat stolen from tissue by abl electrode & blood is least (& current density is higher) with small non-irrigated electrode. Thus, heat remaining in tissue is maximized & lesion size is larger.
9/10
So, why do we use large or irrigated abl electrodes?

The temperature of small non-irrigated abl electrodes rises quickly, which limits RF energy delivery (in temp-controlled mode) and can precipitate coagulum formation, which increases impedance and limits power delivery.
10/10
When RF power output is unlimited, cooling of the abl electrode passively (by using a larger electrode size) or actively (by using saline irrigation) helps to avoid electrode-tissue interface overheating, allowing for greater power delivery and creation of larger lesions.

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More from @ZiadIssaMD

20 Aug
#IssaTweetorials
1/
What are the types of CTI-dependent atrial macroreentry?

CTI-dependent macroreentrant atrial tachycardias (MRATs) are confined to the RA & incorporate the CTI as a critical part of the circuit. All these MRATs can be eliminated by CTI ablation.
#EPeeps
2/
CTI-dependent MRATs include:
(1) peritricuspid reentry (clockwise and counterclockwise typical atrial flutter [AFL])
(2) peritricuspid double-wave reentry
(3) lower loop reentry
(4) intra-isthmus reentry.
3/
PERITRICUSPID REENTRY
In typical AFL the wavefront rotates around the tricuspid annulus. A line of conduction block in the RA free wall is usually required to as a critical lateral boundary that prevents short-circuiting of the flutter wavefront around the IVC.
Read 7 tweets
13 Aug
#IssaTweetorials
#EPEEPS
Do you know the mechanism of typical atrial flutter (AFL)?
1/
Typical AFL is a macroreentrant circuit with the activation wavefront rotating clockwise or counterclockwise around the tricuspid annulus and using the CTI as an essential part of the circuit.
2/
Conduction across the CTI is relatively slower than the rest of the atrium (likely due to the anisotropic fiber orientation), which provides the protected zone of relatively slow conduction necessary for the flutter reentry circuit.
3/
Key to the development of typical AFL is formation of a line of transverse conduction block in the RA free wall, which acts as a critical lateral boundary that prevents short-circuiting of the flutter wavefront around the IVC and, hence, extinguishes (see video).
Read 9 tweets

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