We calculate the electrical resistivity of a two-dimensional electron gas that results from twoparticle collisions and strong Rashba spin-orbit coupling. When combined with impurity scattering, the two-particle correction to the resistivity is proportional to the square of temperature T if only the lower helicity band is filled, but the T 2 term vanishes if the Fermi level is above the Dirac point. If only the electron-electron scattering is present, the resistivity is proportional to T 4 ln |EF /T | below and above the Dirac point, but this term vanishes at the point itself. Our results have implications for other systems with doubly connected Fermi surfaces.