The Bohr model can explain by chance only some very simple examples for energy spectra (harmonic oscillator, simple hydrogen atom, rigid rotator). It fails in all other cases. It was very important historically to find "modern QT". The key issue to be solved were indeed the atomic spectra, including the anomalous Zeeman effect. The latter lead finally to spin.
Bohr also confused the issue with the Stern-Gerlach result: Stern started the whole endeavor of this technically very challenging experiment to disprove the space-quantization hypothesis made within the Bohr-Sommerfeld model. In short: With this model one would have expected three lines and one Bohr magneton for the magnetic moment of the Ag atom (Debye, Sommerfeld 1916). Remarkably, in his very gibberish way Bohr discussed the third line away somehow, given the facts from the anomalous Zeeman effect, where one gets a split in two lines in the alkali atoms instead of 3 as expected from the Bohr-Sommerfeld model.
See, e.g.,
N. Bohr, The Theory of Spectra and Atomic Constitution, Cambridge University Press (1922)
This "normal Zeeman" effect one gets for strong magnetic fields when the spin-orbit coupling is negligible compared to the interaction with the strong magnetic field, one can neglect the spin in the transitions altogether and one gets the split from the orbital angular momentum (for ##l=1## in a triplet) (Paschen-Back effect). For details, see the nice Wikipedia article:
https://en.wikipedia.org/wiki/Zeeman_effect
To Stern's surprise, he and Gerlach finally of course found the direction quantization and a split in only two not three lines.
The final resolution was of course the introduction of half-integer spin (spin 1/2 for the electron) and the gyrofactor 2, which resulted in the split into two lines rather than 3 but still with one Bohr-magneton for the interaction strength. So Bohr was just lucky once more with an ad-hoc hypothesis, and Stern congratulated him with a postcard showing the famous photograph of the two-line split in comparison to the single line when no magnetic field was applied. Somewhat later Stern and Gerlach also quantitatively verified the strength to be 1 Bohr magneton (with an error ##\lesssim 10\%##).