The topic of superconductivity in strongly disordered materials has attracted a significant attention. In particular vivid debates are related to the subject of intrinsic spatial inhomogeneity responsible for non-BCS relation between the superconducting gap and the pairing potential. Here we report experimental study of electron transport properties of narrow NbN nanowires with effective cross sections of the order of the debated inhomogeneity scales. We find that conventional models based on phase slip concept provide reasonable fits for the shape of the R(T) transition curve. Temperature dependence of the critical current follows the text-book Ginzburg-Landau prediction for quasione-dimensional superconducting channel I c~( 1-T/T c ) 3/2 . Hence, one may conclude that the intrinsic electronic inhomogeneity either does not exist in our structures, or, if exist, does not affect their resistive state properties.Keywords: strongly disordered superconductivity, quantum phase slip PACS: 74.81.Fa, Coexistence of strong disorder and superconductivity, being a macroscopically coherent state, is the very intriguing topic. Of particular interest is the superconductor-insulator transition (SIT) observed in highly disordered two-dimensional (2D) thin films 1 as well as in ultra-thin superconducting nanowires 2,3 . Though the phenomenon has been discovered more than twenty years ago, the debates about its origin are still vivid, both in relation to thin wires 4 , 5 as we all thin films 6,7,8,9,10 . Recent experiments 11,12,13 on three representative materials InO x , NbTi and NbN indicate the existence of 'intrinsic electronic inhomogeneity', claimed to be not determined by chemical or/and structural imperfection of the films. While the scanning tunnel microscopy (STM) technique can indeed reveal the spatial variation of the superconducting order parameter, the corresponding electron transport measurements in 2D films cannot shed light on the internal inhomogeneity, if it is present, for the following reason: As soon as a single channel of supercurrent is formed across a 2D superconductor, it shunts all non-superconducting inclusions. Hence, in 2D geometry inhomogeneity-dependent deviations from fluctuation-governed behavior can be resolved by electron transport experiments only at the top of R(T) transition at T>T c . In the opposite limit T