We study the integrability of the geodesic equations of the Chazy-Curzon spacetime. It was established that for the equilibrium point p ρ = p z = z = 0 and, ρ 0 ∈ (1, 2), there are only periodic solutions, the Hamiltonian system, describing geodesic motion of Chazy-Curzon space-time has no additional analytic first integral. Our approach is based on the following: if the system has a family of periodic solutions around an equilibrium and if the period function is infinitely branched then the system has no additional analytical first integral.