I show using Landau theory that quenched dislocations can facilitate the supersolid (SS) to normal solid (NS) transition, making it possible for the transition to occur even if it does not in a dislocationfree crystal. I make detailed predictions for the dependence of the SS to NS transition temperature Tc(L), superfluid density and dislocation spacing L, all of which can be tested against experiments. The results should also be applicable to an enormous variety of other systems, including, e.g., ferromagnets.Recent reports[1] of supersolidity -a crystal exhibiting "off-diagonal long-range order" (ODLRO) [2,3]-in solid 4 He raise many questions. First, quantum Monte Carlo simulations [4] find no supersolid phase. Second, the temperature (T ) dependence[1] of the superfluid density ρ S (T ) in the supersolid (SS) differs from that in the superfluid (SF), contradicting theory [5]. Third, no specific heat anomaly is seen at the SS to NS transition.In this paper, I propose a resolution of these puzzles. Since, depending on the material, either local compression or local dilation increase the local transition temperature T c ( r) [5], and since edge dislocations have regions of both types near their cores[6], these defects induce, in all materials, regions of elevated T c , as first noted for superconductors [7]. ODLRO therefore happens at higher temperatures on the tangled network of quenched dislocations in 4 He crystals than in the bulk, as in superconductors [7,8], and can occur even if the clean (dislocationless) lattice remains normal down to T = 0.Specifically, the DGT[5] model with quenched dislocations implies the following scenario: as temperature T decreases below what I'll call the "condensation" temperature T cond , which is always > T clean c , the transition temperature of the clean (i.e., dislocationless) lattice, each dislocation line in a tangled network of them nucleates a cylindrical supersolid "tube" tangent to it. The radius of these tubes grows with decreasing temperature.We can think of places where dislocations cross, making supersolid tubes overlap, as the "sites"of a random lattice. The sections of tube between these "sites" act as ferromagnetic "bonds". The typical length of these bonds is L, the mean dislocation spacing, which grows with annealing; L → ∞ for a clean crystal. This random lattice does not develop macroscopic supersolidity (or undergo any phase transition) at T cond , because the sites lack long-range phase coherence near T cond . However, as temperature is lowered further, such coherence inevitably develops at T = T c (L),