The presence of a close, low‐mass companion is thought to play a substantial and perhaps necessary role in shaping post‐asymptotic giant branch and planetary nebula outflows. During post‐main‐sequence evolution, radial expansion of the primary star, accompanied by intense winds, can significantly alter the binary orbit via tidal dissipation and mass‐loss. To investigate this, we couple stellar evolution models (from the zero‐age main sequence through the end of the post‐MS) to a tidal evolution code. The binary's fate is determined by the initial masses of the primary and the companion, the initial orbit (taken to be circular), and the Reimers mass‐loss parameter. For a range of these parameters, we determine whether the orbit expands due to mass‐loss or decays due to tidal torques. Where a common envelope (CE) phase ensues, we estimate the final orbital separation based on the energy required to unbind the envelope. These calculations predict period gaps for planetary and brown dwarf companions to white dwarfs. The upper end of the gap is the shortest period at which a CE phase is avoided. The lower end is the longest period at which companions survive their CE phase. For binary systems with 1  M⊙ progenitors, we predict no Jupiter‐mass companions with periods ≲270 d. Once engulfed, Jupiter‐mass companions do not survive a CE phase. For binary systems consisting of a 1  M⊙ progenitor with a companion 10 times the mass of Jupiter, we predict a period gap between ∼0.1 and ∼380 d. These results are consistent with both the detection of a ∼50MJ brown dwarf in a ∼0.003 au (∼0.08 d) orbit around the white dwarf WD 0137−349 and the tentative detection of a ∼2MJ planet in a ≳2.7 au (≳4 yr) orbit around the white dwarf GD66.