The dynamics and rheology of entangled polymer fluids are dominated at
long times by topological constraints. The topological structure of t
he molecules themselves is known to control the linear stress relaxati
on function in a way that agrees well with the ''tube'' model. Here we
extend the model to calculate the nonlinear elastic response of highl
y branched polymers under large shear strains. The nonlinear strain de
pendence is strongly sensitive to the distribution of free ends in the
molecules, in contrast to the linear stress relaxation. Calculations
for combs, monodisperse trees, and the classical gelation ensemble are
compared to experimental results on the unknown structure of branched
polyethylene, and point strongly to a treelike structure.