Atomic force microscopy has been used to image deformed latex films. T
he films were made from core/shell latex particles having a soft shell
and a hard core so that when the films were formed, the continuous ph
ase was composed of the shell polymer in which the hard cores formed l
ong range hexagonal orderings. Upon small amounts of film elongation,
linear necklaces of core particles, perpendicular to the elongation di
rection, were observed at the surface of the films. This observation,
which is mainly due to matrix deformation and has been analyzed theore
tically in the companion paper (preceding paper in this issue), can be
easily understood. When the film is elongated, it becomes thinner in
the direction perpendicular to the elongation; as a result, the core p
articles are pushed together in the direction perpendicular to the elo
ngation, whereas, at the same time, the core particles are pulled apar
t along the direction of elongation. However, as the elongation increa
ses further, AFM images show that, besides the matrix deformation proc
ess, another deformation mechanism, which is a geometrical rearrangeme
nt of the core particles, appears. The response of the film to the str
ain is then characterized by the appearance of breaks in the linear ne
cklace of core particles, which now form zigzags or chevrons. Such a g
eometrical rearrangement of the core particles was anticipated from th
e failure of the theoretical analysis to account for the experimental
strain-stress curves at large film elongations. Therefore, future theo
retical analysis of the mechanical behavior at finite strain of coales
ced core/shell latex films should take into account both deformation m
echanisms.