We calculate the electronic structure of AA AA . . . stacked alternating twist 𝑁layer (t𝑁 G) graphene for 𝑁 =3, 4, 5, 6, 8, 10, 20 layers and bulk alternating twist (AT) graphite systems where the lattice relaxations are modeled by means of molecular dynamics simulations. We show that the symmetric AA AA . . . stacking is energetically preferred among all interlayer sliding geometries for progressively added layers up to 𝑁 = 6. Lattice relaxations enhance electron-hole asymmetry, and reduce the magic angles with respect to calculations with fixed tunneling strengths that we quantify from few layers to bulk AT-graphite. Without a perpendicular electric field, the largest magic angle flat-band states locate around the middle layers following the largest eigenvalue eigenstate in a 1D-chain model of layers, while the density redistributes to outer layers for smaller magic twist angles corresponding to higher order effective bilayers in the 1D chain. A perpendicular electric field decouples the electronic structure into 𝑁 Dirac bands with renormalized Fermi velocities with distinct even-odd band splitting behaviors, showing a gap for N=4 while for odd layers a Dirac cone remains between the flat band gaps. The magic angle error tolerance estimated from density of states maxima expand progressively from 0.05 • in t2G to up to 0.2 • in AT-graphite, hence allowing a greater flexibility in multilayers. Decoupling of t𝑁 G into t2G using effective interlayer tunneling proportional to the eigenvalues of a 1D layers chain allows to map t𝑁 G-multilayers bands onto those of periodic bulk AT-graphite's at different 𝑘 𝑧 values. We also obtain the Landau level density of states in the quantum Hall regime for magnetic fields of up to 50 T and confirm the presence of nearly flat bands around which suppressed density of states gap regions can develop by applying an electric field in 𝑁 > 3 systems.