 Null Kaluza-Klein reduction of a stationary force

For an Eisenhart-Duval lift, reduction along the null isometry fixes a nonzero conserved $p_u=t\prime$ and projects geodesics to $(t,\mathbf{x})$. One never divides by $g_{uu}=0$. When $\mathbf{E}=-\nabla U$ and $\nabla \times \mathbf{A}=\mathbf{B}$, the reduced equation is $\ddot{\mathbf{x}}=\mathbf{E}+2\mathbf{B}\times \dot{\mathbf{x}}$. Every trajectory admits a null lift by choosing $\dot{u}=U+2\mathbf{A}\cdot \dot{\mathbf{x}}-\frac{1}{2}|\dot{\mathbf{x}}{|}^2$.