How to reduce friction is a key issue of tribology and plays an important role in solving a number of problems of physics and engineering, e.g., the durability of the nano-friction generator. [2] The well-known and widely used Amontons-Coulomb friction law stipulates that the tangential frictional force is proportional to the normal compressive force. [3] With the main advantage of being simple, this phenomenological macroscopic law fails to be applicable in the field of nano-tribology. [4] Indeed, nano-friction is affected by a number of factors such as the deformations of the components in contact and the degree of atomic mismatches at the contacting interfaces. [5,6] In recent years, a promising fundamental approach to quantitatively understanding micro-or nano-friction consists in determining the redistribution of electrons due to pressure and sliding. [7][8][9] This approach has been successfully used to reveal the relationship between adsorption and static friction and the one between in-plane strain and friction. [10,11] But, to the best of our knowledge, it has not yet been elaborated and applied to establish a direct and quantitative relationship between friction and electrons redistribution driven by the normal load.Some pioneering works have shown that quasi-zero friction or superlubricity is feasible. [12][13][14][15] At present, there are two main strategies for achieving frictionless sliding between both solids in contact: structural superlubricity (SSL) and pressuredriven superlubricity. [12][13][14] SSL occurs only if two contacting surfaces that slide one on the other are incommensurable. [16] It was theoretically predicted and shown to be achievable for microscopic phenomena and even for engineering design. [14,17] Nevertheless, it is very difficult to prepare and keep both ultra-clean surfaces in incommensurate contact. [18] Thus, it is urgent to seek an alternative solution to avoid the harsh incommensurate contact required for SSL. Fortunately, a few works have indicated that the external load may regulate friction to superlubricity even in a commensurate contact. [12,19,20] Initially, pressure-and tension-actuated frictionless sliding was expected to be realized at a gas-solid interface (rare gas layers and metal surfaces), [12,19] but the structural instability of rare gas layer limited further experimental explorations. Recently, the pressure-induced friction collapse rekindles hope for load-driven superlubricity at 2D solid-solid interfaces. [13,20] However, the exploration of load-driven superlubricity has fallen into another dilemma: the critical load of ≈300 GPa required for superlubricity is so demanding that it is experimentally unrealistic. [13] By first-principles calculations, it is shown that the friction at solid-solid interfaces between 2D nanomaterials (TDNMs), such as h-BN and graphene, can be reduced nearly to zero even if the normal load is smaller than 5 GPa. The quantitative analysis of interfacial charge density demonstrates a detailed process in which the pressure-dr...