Imagine that I have a particle of charge $q$ at the center of a spherical insulating shell of charge $Q$ and radius $R$.
Both the particle and shell are initially at rest.
Now I apply a force $\mathbf{F}$ to the particle which causes it to have an acceleration $d\mathbf{v}/dt$.
The electric field due to the charge $q$ is given by:
$$\mathbf{E} = - \mathbf{\nabla} \phi - \frac{\partial \mathbf{A}}{\partial t}.$$
Due to the symmetry of the situation the total static electric force on the shell due to the charge is zero.
The $\mathbf{A}$-field due to the charge $q$ at the position of the shell is approximately given by:
$$\mathbf{A} = \frac{q\mathbf{v}}{4 \pi \epsilon_0 c^2R}.$$
Therefore the charge $q$ induces an electric force $\mathbf{f_s}$ on the shell given by:
$$\mathbf{f_s} = -\frac{qQ}{4 \pi \epsilon_0 c^2R}\frac{d\mathbf{v}}{dt}.$$
But the total force on the system as a whole should remain $\mathbf{F}$.
Does this mean that the shell must induce a balancing electric force $\mathbf{f_s}$ back on the accelerating particle?
P.S. As the particle acceleration is constant I believe that there is no radiation reaction force back on the particle (a controversial view I admit, see related link below). Thus there is no change of momentum in the EM field. Therefore the internal forces on the system of charges should balance.