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B. Murienne - Master Project Thesis - Infoscience - EPFL

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Figure 12. Velocity vector field [1].<br />

Conduction velocity vector fields describe the local speed and direction of propagation of cardiac<br />

activity [1]. Traditionally, the direction of propagation is identified manually and the speed is<br />

computed from ∆t between activation at two points along that direction measured with two<br />

electrodes. However, this procedure is valid only if the electrode used is small enough to<br />

distinguish the local activity and if the temporal resolution is good. If the wavefront is not<br />

perpendicular to line connecting electrodes, two different sites appear to activate nearly<br />

simultaneously as shown in Figure 13.<br />

Figure 13. Schematic diagram of a propagating wavefront observed by two electrodes [1].<br />

(a) The wavefront is perpendicular to the line joining the two electrodes.<br />

(b) The wavefront intersects obliquely the line joining the two electrodes.<br />

If the wavefront is perpendicular to the line joining both electrodes (Figure 13.a), the inter-<br />

electrode distance divided by the difference in activation times gives a good estimation of the<br />

propagation velocity. If the wavefront intersects obliquely the line joining both electrodes (Figure<br />

13.b), an artificially high propagation velocity is deduced from the division.<br />

A new method to estimate velocities of multiple wavefronts at different locations and times and<br />

find vector fields of local conduction was developed [1]. The algorithm consists in fitting<br />

polynomials T(x,y) to a set of “active” points in the (x,y,t)-space and estimating velocity vectors<br />

from partial derivatives of these polynomials.<br />

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