Droplet sliding after impingement on an inclined superhydrophobic surface has very broad applications, but the investigations of this variable process are surprisingly lacking in the literature. In this paper, the spreading and sliding characteristics of a water droplet impinging on an inclined hydrophobic surface at low Weber numbers (We≲ 50) are investigated via a numerical approach. The influences of surface inclined angle α, impact velocity, and droplet diameter on droplet spreading diameter and maximum spreading diameter (Ds and Ds_max), sliding lengths of droplet, droplet leading and trailing edges (Ld, Llea and Ltra) are thoroughly examined. Results show that droplet displays markedly distinct behaviors when α≥ 60° as the maximum spreading diameter is noticeably larger and droplet oscillation becomes stronger and more unstable, which are contributed from the accumulated liquid mass at droplet head associated with the drastic growth of the tangential inertial force. However, the instability at α≥ 60° disappears when We≥ 40, resulting from the liquid mass at droplet head dominating the sliding process, which demonstrates that droplet motion at a high inclined angle is primarily determined by droplet leading edge. The nondimensionalized maximum spreading diameter (Ds_max∗) is found to scale with the normal Weber number (WeN) according to a power law (Ds_max∗∝WeNα1), and a universal scaling law of Ld_total∗∝WeT0.6 between the nondimensionalized total sliding length (Ld_total∗) and the tangential Weber number (WeT) is discovered. The relationship between the four distinct post-impingement regimes identified in this work and the Weber and Bond numbers are presented and explained. These results offer fresh insight into the currently insufficient understanding of droplet sliding process on inclined hydrophobic surfaces.