  As experimental particle physics becomes more and more precise, it is
becoming increasingly important for Monte Carlo simulations to improve the
precision of their predictions. In terms of the hard matrix element, this means
calculating to a higher order in perturbation theory. To be consistent this
requires both NNLO QCD corrections and NLO EW corrections to be included. There
are also interference effects between these processes that are not simple to
handle consistently. For a broad description of the behaviour of NLO EW
corrections at high energies, the Sudakov logarithmic approach provides a good
approximation, and is much less computationally expensive than the full
calculation. The implementation of EW Sudakov logarithms within the SHERPA
program are outlined here along with some initial results. As well as this, an
overview of the status of full NLO EW computations with SHERPA is presented.
