This report investigates homoleptic iron(II) complexes of thiazolinyl analogues of chiral PyBox tridentate ligands: 2,6-bis(4-phenyl-4,5-dihydrothiazol-2-yl)pyridine (L 1 Ph), 2,6-bis(4-isopropyl-4,5-dihydrothiazol-2-yl)pyridine (L 1 iPr), and 2,6-bis(4tert-butyl-4,5-dihydrothiazol-2-yl)pyridine (L 1 t-Bu). Crystallographic data imply the larger and more flexible thiazolinyl rings reduce steric clashes between the R substituents in homochiral [Fe((R)-L 1 R) 2 ] 2+ or [Fe((S)-L 1 R) 2 ] 2+ (R = Ph, iPr, or t-Bu), compared to their PyBox (L 2 R) analogues. Conversely, the larger heterocyclic S atoms are in close contact with the R substituents in heterochiraland [Fe(L 1 iPr) 2 ] 2+ exhibit spin-crossover equilibria in CD 3 CN, centered at 344 ± 6 K and 277 ± 1 K respectively, while their heterochiral congeners are essentially low-spin within the liquid range of the solvent. These data imply that the diastereomers of [Fe(L 1 Ph) 2 ] 2+ and [Fe(L 1 iPr) 2 ] 2+ show a greater difference in their spin-state behaviors than was previous found for [Fe(L 2 Ph) 2 ] 2+ . Gas-phase DFT calculations (B86PW91/def2-SVP) of the [Fe(L 1 R) 2 ] 2+ and [Fe(L 2 R) 2 ] 2+ complexes reproduce most of the observed trends, but they overstabilize the high-spin state of SCO-active [Fe(L 1 iPr) 2 ] 2+ by ca. 1.5 kcal mol −1 . This might reflect the influence of intramolecular dispersion interactions on the spin states of these compounds. Attempts to model this with the dispersion-corrected functionals B97-D2 or PBE-D3 were less successful than our original protocol, confirming that the spin states of sterically hindered molecules are a challenging computational problem.