We study oil in water emulsions when the interaction between the dropl
ets becomes strongly adhesive, causing them to stick together. However
, the droplets still retain their integrity and do not coalesce. By us
ing emulsions with droplets that are monodisperse in size, we are able
to clearly observe their structure when the emulsions become adhesive
. We show that the structure of strongly adhesive emulsions reflects a
complex interplay among the strength of the adhesion, the droplet vol
ume fraction, phi, and the time evolution of the adhesion. Initially,
strong adhesion of the droplets leads to the formation of an emulsion
gel. Moreover, the gel possesses a well-defined characteristic length
scale, d(c), as evidenced by an intense ring of small angle light scat
tering. The characteristic length scale decreases as the droplet volum
e fraction increases. At low phi, the structure of the emulsion gel is
fractal on length scales shorter than d(c), and the measured fractal
dimension suggests that the gelation mechanism is controlled by diffus
ion-limited cluster aggregation. However, at higher phi, the short ran
ge structure is more compact, rather than fractal, and a different mec
hanism must be responsible for the gelation. If the strength of the ad
hesion is increased still further, the droplets become more deformed,
resulting in massive restructuring of the emulsion gel. The structure
fractures into independent, more compact flocs, eliminating the overal
l rigidity of the emulsion gel. These results help rationalize some of
the diverse structures that are observed upon flocculation of the mor
e usually studied polydisperse emulsions.