We construct the hydrodynamic theory for spin-1/2 Bose gases at arbitrary temperatures. This theory describes the coupling between the magnetization, and the normal and superfluid components of the gas. In particular, our theory contains the geometric forces on the particles that arise from their spin's adiabatic following of the magnetization texture. The phenomenological parameters of the hydrodynamic theory are calculated in the Bogoliubov approximation and using the Boltzmann equation in the relaxation-time approximation. We consider the topological Hall effect due to the presence of a skyrmion, and show that this effect manifests itself in the collective modes of the system. The dissipative coupling between the magnetization and the normal component is shown to give rise to magnetization relaxation that is fourth order in spatial gradients of the magnetization direction. In metallic ferromagnets, magnetization dynamics leads to forces on quasiparticles of geometric origin called spin motive forces, that have gained considerable attention recently [8][9][10][11][12]. Furthermore, spin textures with nonzero chirality, such as the skyrmion lattice observed recently [13,14] induce the so-called topological Hall effect [5,6]. In addition, the coupling between magnetization and quasiparticles has also been shown to give rise to novel forms of magnetization relaxation in this case. A prominent example is inhomogeneous Gilbert damping [15][16][17]. This effect is important in clean solid-state systems. We therefore expect these effects to be particularly important for gases of ultracold atoms, that, in contrast to conventional condensed-matter systems, are free of impurities.The field of ultracold atoms is characterised by exquisite experimental control [18][19][20]. Relevant for our focus is the great amount of recent activity on spinor Bose gases. Firstly, it has been discovered that these gases can be either ferromagnetic or antiferromagnetic depending on the details of the scattering lengths [21,22]. Furthermore, numerous studies at zero temperature, based on the Gross-Pitaevskii equation, have elucidated the longwavelength properties of spinor gases [23,24]. Other areas of current interest in the field include topological excitations, magnetic dipole-dipole interactions and nonequilibrium quantum dynamics [25]. The recent progress in the understanding of ferromagnetic spinor gases and their manipulation by light has also enabled detailed studies of magnetization dynamics [26,27].