Intriguingly, the clogging behavior of this crosslinked polymer system may have analogies with colloidal jamming. In attractive colloidal systems, the transition between a liquid and jammed or glassy state is controlled by particle volume fraction ϕ, interparticle interaction strength U compared to thermal energy k B T , and the amount of stress applied to the system σ . The phase diagram describing the jamming transition is most often plotted in these three dimensions, on dimensionless axes k B T /U , 1/ϕ and σ/σ 0 , where σ 0 is related to the yield stress of the material. Systems near the origin of this plot are "jammed" and behave as solids while systems far from the origin are liquid. The details of the location and shape of the transitions between jammed, solid-like systems and un-jammed, liquid systems vary based on the materials involved.