Scattering of Alpha Particles: Graph and Conclusions
The scattering of alpha particles by a thin foil (as in Rutherford’s experiment) can be represented by a plot of number of scattered particles versus scattering angle (\( \theta \)).
Graph:
In the graph: - The y-axis represents the number of alpha particles scattered. - The x-axis represents the scattering angle (\( \theta \)). - Most particles are scattered at very small angles, while very few are scattered at large angles.
Two Important Conclusions:
1. Most alpha particles pass through undeflected: This indicates that the atom is mostly empty space, allowing most alpha particles to go straight through the foil without any deflection.
2. Some particles are deflected at large angles: A small number of alpha particles experience large-angle deflections, which implies the presence of a very small, dense, positively charged nucleus at the center of the atom that repels the alpha particles.
Summary:
The plot confirms Rutherford’s nuclear model of the atom: atoms consist of a tiny, dense, positively charged nucleus surrounded by electrons, with most of the atom being empty space. The scattering distribution is key evidence for the nuclear structure of the atom.
A beam of light of wavelength \(\lambda\) falls on a metal having work function \(\phi\) placed in a magnetic field \(B\). The most energetic electrons, perpendicular to the field, are bent in circular arcs of radius \(R\). If the experiment is performed for different values of \(\lambda\), then the \(B^2 \, \text{vs} \, \frac{1}{\lambda}\) graph will look like (keeping all other quantities constant).