We
study the mechanism of spiral wave unpinning in the Belousov–Zhabotinsky
(BZ) reaction with a DC electric field. The unpinning is characterized
by the phase of the spiral tip around the obstacle boundary at the
time of unpinning. We systematically measure the unpinning phase as
a function of the chirality of spiral rotation, the initial phase
of the spiral, the size of the pinning obstacle, the direction, and
the strength of the applied electric field. In both BZ experiments
and simulations using the Oregonator model, we observe that the spiral
wave always unpins at a fixed position with respect to the applied
field. The wave unpins when the electric field component in the direction
of the tip velocity of the spiral waves becomes equal to a threshold
field strength. From these observations, we deduce a relation between
the phase of unpinning, the size of the pinning obstacle, the strength,
and the direction of the electric field, and it agrees with our observations.
We conclude from our observations that a retarding ‘electric
force’ on the chemical wave is responsible for the unpinning
in the BZ medium. Our results indicate that the ‘electric force’
is more effective in unpinning when the wave moves away from the anode
than when it is moving toward it.