If you think about $G$ as a composition of maps between manifolds
$$ M \mathop{\to}_v TM \mathop{\to}_{dF} \Bbb R,$$
then you can just apply the chain rule to get $D_xG(w) = D_vdF(D_x v(w))$ where the derivatives are taken in higher tangent bundles:
$$ TM \mathop{\to}_{Dv} TTM \mathop{\to}_{DdF} \Bbb R.$$
In coordinates you can expand this using partial derivatives to $DG(w) = w^i v^j F_{,ij} + w^i F_{,j} v^j_{,i}$; so if you have a Riemannian structure you get a coordinate-free formula something like what you were looking for:
$$ DG(w) = \nabla^2 F(v,w) + dF( \nabla_w v ).$$
Here $\nabla$ is the Riemannian connection and $\nabla^2$ the covariant Hessian.