We study the bcc-hcp phase transition in Ti and Zr with the use of first-pr
inciples calculations. We have determined the complete energy surface from
the bcc to hcp structure. The results are used to find an appropriate Landa
u free energy density for describing this transformation. The proposed Land
au free energy density has two relevant order parameters: shear and shuffle
. Through first-principles calculations, we show that the bcc structure is
unstable with respect to the shuffle of atoms (TA(1) N-point phonon) rather
than the shear. Therefore, we reduce the two order parameter Landau free e
nergy to an effective one order parameter (shuffle) potential, which is a r
easonable approximation. In general, the effective Landau free energy is a
triple-well potential. From the phonon dispersion data and the change in en
tropy at the transition temperature we find the free energy coefficients fo
r Ti and Zr.