Using the laser photoelectron attachment method with an energy width ≤ 1 meV at low energies (≤ 172 meV) and an electron beam method (energy width about 70 meV) at higher energies (up to 2 eV), we have determined absolute cross sections σ_e (E) for dissociative electron attachment to the dipolar molecules CH₂Br₂ and CCl₃Br by normalization to known electron attachment rate coefficients. At thresholds for vibrational excitation of the CH₂Br₂ molecule, the DA cross section exhibits pronounced structure due to coupling of the attachment process with scattering channels; below the ν₃ = 1 onset for the symmetric CBr₂ stretch vibration, a clear vibrational Feshbach resonance is observed. At low energies the cross sections σ_e (E) show an energy dependence between E^−1/2 and E⁻¹, in essential agreement with predictions of an extended Vogt–Wannier (EVW) capture model which includes the long-range electron–dipole interaction in addition to the polarization force. The determined absolute values are, however, substantially smaller than those predicted by the EVW model. Semiempirical R-matrix calculations have been carried out which show that at low electron energies (E < 0.15 eV) Br⁻ formation from CCl₃Br proceeds by s-wave attachment to the anion ground state while a broad peak, observed around 0.6 eV and evolving predominantly into the Cl⁻ channel, is due to an excited anion state. Comparisons are made with cross sections and rate coefficients obtained in previous photoelectron attachment work (TPSA) and in electron beam as well as swarm experiments. Based on our joint experimental results for σ_e (E), we report the electron temperature dependence of the rate coefficients k_e (T_e) for free electron attachment involving a Maxwellian electron ensemble and a gas at room temperature (T_G = 300 K).