We present wall-resolved large-eddy simulations (LES) of the incompressible Navier-Stokes equations together with empirical modeling for turbulent Taylor-Couette (TC) flow where the inner cylinder is rotating with angular velocity Ω i and the outer cylinder is stationary. With R i , R o the inner and outer radii respectively, the radius ratio is η = 0.909. The subgrid-scale (SGS) stresses are represented using the stretched-vortex subgrid-scale model while the flow is resolved close to the wall. LES is implemented in the range Re i = 10 5 − 3 × 10 6 where Re i = Ω i R i d/ν and d = R o − R i is the cylinder gap. It is shown that the LES can capture the salient features of the TC flow, including the quantitative behavior of span-wise Taylor rolls, the log-variation in the mean velocity profile and the angular momentum redistribution due to the presence of Taylor rolls. A simple empirical model of the turbulent, TC flow is developed consisting of near-wall, loglike turbulent wall layers separated by an annulus of constant angular momentum. The model is closed by a proposed scaling relation concerning the thickness of the wall layer on the inner cylinder. Model results include the Nusselt number N u (torque required to maintain the flow) and various measures of the wall-layer thickness as a function of both the Taylor number T a and η. These agree reasonably with experimental measurements, direct numerical simulation (DNS) and the present LES over a range of both T a and η.In particular, the model shows that, at fixed η < 1, N u grows like T a 1/2 divided by the square of the Lambert, (or Product-Log) function of a variable proportional to T a 1/4 . This cannot be represented by a power law dependence on T a. At the same time the wall-layer thicknesses reduce slowly in relation to the cylinder gap. This suggests an asymptotic, very large T a state consisting of constant angular momentum in the cylinder gap with u θ = 0.5 Ω i R 2 i /r, where r is the radius, with vanishingly thin turbulent wall layers at the cylinder surfaces. An extension of the model to rough-wall turbulent wall flow at the inner cylinder surface is described. This shows an asymptotic, fully rough-wall state where the torque is independent of Re i /T a, and where N u ∼ T a 1/2 . arXiv:1908.06577v1 [physics.flu-dyn]