Following the conjecture on the correspondence between the dual resonance amplitude and the very high order Feynman diagram, we calculate the dual resonance amplitude cor responding to the globular Feynman diagram. We find that it develops essential singularities in the Lorentz-invariant variables. It has been suggested by several authors 1 l' 2 l that amplitudes in the dual res onance model can be obtained by taking the continuum limit of the F eynman amplitudes corresponding to the very high order planar diagrams. It seems rather peculiar that only the planar Feynman diagram can lead to the dual reso nance amplitude. In general any Feynman diagram can be drawn in a three dimensional topological space. However, we need higher dimensional topolo gical spaces in order to discuss the continuum limits of the very high order Feynman diagrams. For example, the Klein-bottle-like Feynman diagram can be drawn in the three-dimensional space before taking the continuum limit. But, once we take the continuum limit, we need the four-dimensional space to draw