The diffraction phenomena are usually divided into two categories: Fresnel diffraction and Fraunhofer diffraction.In the Fresnel class of diffraction the source of light
and the screen are, in general, at a finite distance from the diffracting aperture.In the Fraunhofer class of diffraction, the source and the screen are at infinite distances from the aperture; this is easily achieved by placing the source on the focal plane of a convex lens and placing the screen on the focal plane of another convex lens.The two lenses effectively moved the source and the screen to infinity because the first lens makes the light beam parallel and the second lens effectively makes the screen receive a parallel beam of light.As lychette said Fraunhoffer diffraction is much easier to analyse than frenel and its just due to this we name the diffraction phenomena differently.