On the motion of a test particle around a global monopole in a modified gravity

In this paper we suggest an approach to analyse the motion of a test particle in the spacetime of a global monopole within a $f(R)$-like modified gravity. The field equations are written in a more simplified form in terms of $F(R)=\frac{df(R)}{dR}$. Since we are dealing with a spherically symmetric problem, $F(R)$ is expressed as a radial function $\mathcal{F}(r)\equiv F(R(r))$. So, the choice of a specific form for $f(R)$ will be equivalent to adopt an Ansatz for $\mathcal{F}(r)$. By choosing an explicit functional form for ${\cal F}®$ we obtain the weak field solutions for the metric tensor, compute the time-like geodesics and analyse the motion of a massive test particle. An interesting feature is an emerging attractive force exerted by the monopole on the particle.