It is usually believed that wall slip contributes small effects to macroscopic flow characteristics. Here we demonstrate that this is not the case for the thermocapillary migration of a long bubble in a slippery tube. We show that a fraction of the wall slip, with the slip length λ much smaller than the tube radius R, can make the bubble migrate much faster than without wall slip. This speedup effect occurs in the strongslip regime where the film thickness b is smaller than λ when the Marangoni number S = τ T R/σ 0 ( 1) is below the critical value S * ∼ (λ/R) 1/2 , where τ T is the driving thermal stress and σ 0 is the surface tension. The resulting bubble migration speed is found to be U b ∼ (σ 0 /µ)S 3 (λ/R), which can be more than a hundred times faster than the no-slip result U b ∼ (σ 0 /µ)S 5 (Wilson,