A recent experimental study showed that, distorting a CoPc molecule adsorbed on a Au(111) surface, a Kondo effect is induced with a temperature higher than 200 K. We examine a model in which an atom with strong Coulomb repulsion (Co) is surrounded by four atoms on a square (molecule lobes), and two atoms above and below it representing the apex of the STM tip and an atom on the gold surface (all with a single, half-filled, atomic orbital). The Hamiltonian is solved exactly for the isolated cluster, and, after connecting the leads (STM tip and gold), the conductance is calculated by standard techniques. Quantum interference prevents the existence of the Kondo effect when the orbitals on the square do not interact (undistorted molecule); the Kondo resonance shows up after switching on that interaction. The weight of the Kondo resonance is controlled by the interplay of couplings to the STM tip and the gold surface, and between the molecule lobes. Coupling of localized spins to conduction electrons may lead to a transport anomaly known as the Kondo effect [1,2]. This effect, that usually shows up at low temperatures, consists of a sharp peak at the Fermi level, whose half-width is known as the Kondo temperature (T K ), and a conductance close to one conductance quantum G 0 = 2e 2 /h. The Kondo temperature in the case of magnetic impurities in non-magnetic metals is around 50 K [1], whereas in artificial atoms (quantum dots) is just a few hundred mK [3,4]. In a recent experiment [5,6] it has been shown that it is possible to control the characteristics, and even the existence, of the Kondo resonance by modifying the chemical surroundings of a magnetic atom. The experiments were carried out on a cobalt phthalocyanine molecule (CoPc) adsorbed on a Au(111) surface. Dehydrogenation of this molecule (d-CoPc) by means of voltage pulses from a Scanning Tunneling Microscope (STM) triggered a Kondo effect with a rather high Kondo temperature (T K ≈ 200 K). This temperature is even higher than that observed for bare Co adsorbed on a similar surface [6,7]. Besides such a high T K , one of the most remarkable results of [5] is the fact that the undistorted molecule does not show a Kondo effect, while it is readily promoted by distorting the molecule upon dehydrogenation. Topographic images taken by means of the STM [5] indicated that the CoPc molecule has four almost non-overlapping lobes symmetrically placed around the Co atom. Dehydrogenation distorts the molecule and forces those lobes to overlap. In addition it strongly decreases the distance from the molecule lobes to the gold surface and increases the Co/gold surface distance in approximately 30% [5].We hereby propose a simple model that accounts for some of the salient features of the experiment described above. We take a model Hamiltonian on a small atomic arrangement which is solved exactly, and subsequently connected to semi-infinite chains used to describe the STM tip and the gold surface. Fig. 1 depicts this atomic arrangement. A central site with a single atomic or...