The order of angle moments $\mathbf{J}_\mathbf{r}$ in metallic uranium can be appeared due to ordering of pairs of orbital moments $\mathbf{L}_\mathbf{r}$ in ‘orbital glass’ form. Representation of the many-electron operator spinors (MEOS) and their Fourier images (chemical (covalent) bond fluctuations (CBF)) give ‘glass’ parameter ${P_3}(T)=\left\langle{{(L_r^z)}^2}\right\rangle$ as CBF functional and function of temperature $T$. Metallic uranium region ($C_3$) contains $N_3$ elements of Galois groups (GG–G$_3$) in form of pairs of uranium ions sites ($\mathbf{r}$–$\mathbf{R}$) and their moments ($\mathbf{L}_\mathbf{r}\uparrow\downarrow\mathbf{L}_\mathbf{R}$). Orientation of $P_3$ along O$z$ under deformation $u_{33}$ determines the contribution of magnetic susceptibility $\chi_{zz}\sim{P_3}(T)$. Magnetoelectrical resistance $\Delta{R}_{33}\sim{P_3}(T)$. Covalent bond 6$d$–6$d$ increases melting temperature by $\Delta{T_L}\sim10^2$ K for U and Cm (which have one 6$d$ electron). Anomalous Hall effect $R_{13}(P_1, P_3)$ is caused by CBF as well as the residual electrical resistance $R_0$ of transition metals, in particular U.