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For side-by-side spheres, reflection in the vertical mid-plane exchanges the spheres while preserving their common velocity, so their axial drags are equal. For vertically aligned spheres, reflection in the horizontal mid-plane exchanges them and reverses velocity; applying linearity to reverse all velocities back restores the original problem and again gives equal axial drag. These are symmetries of the exact two-sphere Stokes problem.

At a distant side-by-side centre, the leading flow produced by one sphere is $3aU/(4b)$ in the direction of translation. On its axis it is $3aU/(2b)$. This ambient entrainment lowers the relative velocity of the other sphere. Using Stokes drag law with that relative velocity gives the mutual drag reduction of two distant translating spheres:The feedback of the corrected force into the other sphere's flow enters at the next order. If the coefficient $6\pi$ is needed directly from the preceding solution, its pressure anomaly is $p=3\mu Ua\cos \theta /(2R^2)$. At the surface the traction components are $t_R=-3\mu U\cos \theta /(2a)$ and $t_{\theta }=3\mu U\sin \theta /(2a)$; their axial projection is the constant $-3\mu U/(2a)$. Integrating over $4\pi a^2$ gives the single-sphere force $-6\pi \mu aU{\mathbf{e}}_z$, as used above.