We allow an external 〈q\ifmmode\bar\else\textasciimacron\fi{}q〉 condensate to enter standard SU(2)\ifmmode\times\else\texttimes\fi{}U(1) electroweak theory via the vacuum expectation value 〈0\ensuremath{\Vert}:q\ifmmode\bar\else\textasciimacron\fi{}(x)q(y):\ensuremath{\Vert}0〉, as in QCD sum-rule applications. For a given flavor, we then find that any gauge-parameter dependence of quark self-energies on the ``mass shell'' is eliminated provided that the mass shell is made to coincide with both the expansion-parameter mass occurring in the operator-product expansion of 〈0\ensuremath{\Vert}:q\ifmmode\bar\else\textasciimacron\fi{}(x)q(y):\ensuremath{\Vert}0〉 and the standard electroweak mass acquired via the Yukawa coupling to the usual scalar vacuum expectation value of spontaneous symmetry breaking. This result indicates that if the QCD-generated order parameter 〈q\ifmmode\bar\else\textasciimacron\fi{}q〉 and associated dynamical mass(es) ${m}_{q}^{\mathrm{dyn}}$ are utilized as external input parameters in electroweak calculations involving hadrons, then new corrections must be introduced into the q\ifmmode\bar\else\textasciimacron\fi{}qW and q\ifmmode\bar\else\textasciimacron\fi{}qZ vertices in order to preserve SU(2)\ifmmode\times\else\texttimes\fi{}U(1) Ward identities.