The various four-fermion production channels in e + e − annihilation are discussed and the CC11 process e+e−→fˉ1uf1df2dfˉ2d=e , is studied in section d2σ/ds1ds2 , with s1,s2 being the invariant masses squared of the two fermion pairs, may be expressed by six generic functions. All but one may be found in the literature. The cross section, including initial-state radiation and the Coulomb correction, is discussed and compared with other calculations from low energies up to √ s = 2 TeV