Let , , and let
Use the method of reflections for Stokes flow. At the fixed sphere, the first sphere produces the incident Stokeslet velocity to leading order. In Faxén translation law, set the second sphere's translational velocity to zero. The applied holding force is therefore
The first sphere's finite-radius potential dipole adds to the incident velocity, as does the Laplacian term in Faxén translation law at the fixed sphere. Multiplying by gives the stated next correction. There is no intermediate term. This is the holding force and torque for a sphere in a distant Stokeslet.
The vorticity of a Stokeslet at displacement is . At the fixed sphere, , so
Set its angular velocity to zero in Faxén rotation law. The applied holding couple is
The displayed sign is the external couple needed to oppose the ambient rotation, rather than the hydrodynamic couple on the sphere.
The leading reflected flow at the first sphere is . Apply Faxén translation law there with its prescribed force . Since , the mobility correction from a fixed distant sphere is
The next correction comes from finite-radius terms in the incident/reflected flow and in Faxén translation law, together with the fixed sphere's induced stresslet and holding-couple rotlet. Each gives at the first sphere. The symbol is its isolated-sphere velocity scale, not its actual velocity in the two-sphere problem.
The first sphere has no applied couple. Its angular velocity follows from Faxén rotation law and the reflected Stokeslet:
The component of parallel to contributes no vorticity. The next reflected rotlet and stresslet give the stated error order.

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