Rutherford Scattering Formula
The scattering of alpha particles from nuclei can be modeled from the Coulomb force and treated as an orbit. The scattering process can be treated statistically in terms of the cross-section for interaction with a nucleus which is considered to be a point charge Ze. For a detector at a specific angle with respect to the incident beam, the number of particles per unit area striking the detector is given by the Rutherford formula:
The predicted variation of detected alphas with angle is followed closely by the Geiger-Marsden data. The above form includes the cross-section for scattering for a given nucleus and the nature of the scattering film to get the scattered fraction. Another common form for the Rutherford equation is just the differential cross section for scattering from a given nucleus
.
For this equation, some of the constants have been combined to express the cross section in terms of the fine-structure constant, a .
This form of the scattering formula serves as a signature for scattering off a point target in which no structure is evident. The point of departure from Rutherford scattering in the case of the nucleus was the basis for the earliest evaluations of the nuclear radius.
The departure from the point-particle form of scattering has been an indicator of nuclear structure and then at higher energies, the structure of the proton.