Geiger-Marsden Experiment: Analysis and Derivation
Step 1 (Graph and Conclusions): [1 Mark]
The graph of the number of scattered particles ($N$) versus the scattering angle ($\theta$) shows an exponential decrease as the angle increases.
- Conclusion 1: Most $\alpha$-particles pass through the gold foil with very little or no deflection, indicating that the atom is mostly empty space.
- Conclusion 2: A very small fraction of $\alpha$-particles undergo large-angle scattering, indicating the presence of a small, dense, positively charged nucleus at the center.
Step 2 (Governing Law for Distance of Closest Approach): [1 Mark]
At the distance of closest approach ($r_0$), the entire initial kinetic energy ($K$) of the $\alpha$-particle is converted into electrostatic potential energy ($U$) as the particle momentarily comes to rest before reversing its direction.
By the Law of Conservation of Energy:
$$K = U$$ $$\frac{1}{2}mv^2 = \frac{1}{4\pi\epsilon_0} \cdot \frac{(Ze)(2e)}{r_0}$$Step 3 (Mathematical Derivation and Final Expression): [1 Mark]
Rearranging the equation to solve for $r_0$:
$$r_0 = \frac{1}{4\pi\epsilon_0} \cdot \frac{2Ze^2}{\frac{1}{2}mv^2}$$ $$r_0 = \frac{4Ze^2}{4\pi\epsilon_0 mv^2}$$Where:
- $Z$ = Atomic number of the target nucleus.
- $e$ = Elementary charge.
- $m$ = Mass of the $\alpha$-particle.
- $v$ = Initial velocity of the $\alpha$-particle.
💡 EL10 Concept Insight: Imagine throwing a ball at a wall; the closer it gets before bouncing back, the stronger the "push" from the wall. In this experiment, the $\alpha$-particle is the ball, and the nucleus is the wall; the distance of closest approach is simply the point where the particle's speed drops to zero because the nucleus's positive charge is pushing it away too hard to go any further.