  Electroweak (EW) corrections can be enhanced at high energies due to the soft
or collinear radiation of virtual and real $W$ and $Z$ bosons that result in
Sudakov-like corrections of the form $\alpha_W^l\log^n(Q^2/M_{W,Z}^2)$, where
$\alpha_W =\alpha/(4\pi\sin^2\theta_W)$ and $n\le 2l-1$. The inclusion of EW
corrections in predictions for hadron colliders is therefore especially
important when searching for signals of possible new physics in distributions
probing the kinematic regime $Q^2 \gg M_V^2$. Next-to-leading order (NLO) EW
corrections should also be taken into account when their size
($\mathcal{O}(\alpha)$) is comparable to that of QCD corrections at
next-to-next-to-leading order (NNLO) ($\mathcal{O}(\alpha_s^2)$). To this end
we have implemented the NLO weak corrections to the Neutral-Current Drell-Yan
process, top-quark pair production and di-jet production in the parton-level
Monte-Carlo program MCFM. This enables a combined study with the corresponding
QCD corrections at NLO and NNLO. We provide both the full NLO weak corrections
and their Sudakov approximation since the latter is often used for a fast
evaluation of weak effects at high energies and can be extended to higher
orders. With both the exact and approximate results at hand, the validity of
the Sudakov approximation can be readily quantified

High Energy Physics - Phenomenology