Geiger-Marsden Experiment (Rutherford Scattering)
- The experiment measured the number of alpha particles (\( N \)) scattered at different angles (\( \theta \)).
- The observed scattering pattern led to significant conclusions about atomic structure.
Graph: Variation of \( N \) with \( \theta \)

Conclusions from the Graph
1. Most alpha particles pass undeflected, meaning the atom is mostly empty space.
2. Few particles are scattered at large angles, implying a small, dense, positively charged nucleus. Expression for Distance of Closest Approach The distance of closest approach (\( r_0 \)) is the minimum separation between the alpha particle and the nucleus before it stops and reverses.
- At the point of closest approach, the initial kinetic energy of the alpha particle is converted into electrostatic potential energy: \[ \frac{1}{2} m v^2 = \frac{1}{4\pi\epsilon_0} \frac{Z e \cdot 2e}{r_0} \]
Solving for \( r_0 \): \[ r_0 = \frac{1}{4\pi\epsilon_0} \frac{2 Z e^2}{\frac{1}{2} m v^2} \] \[ r_0 = \frac{4 \pi \epsilon_0 \cdot 2 Z e^2}{m v^2} \] Thus, the distance of closest approach is: \[ r_0 = \frac{2 Z e^2}{4 \pi \epsilon_0 \cdot \frac{1}{2} m v^2} \]
This represents the minimum distance between the alpha particle and the nucleus before repulsion stops its motion.
A racing track is built around an elliptical ground whose equation is given by \[ 9x^2 + 16y^2 = 144 \] The width of the track is \(3\) m as shown. Based on the given information answer the following: 
(i) Express \(y\) as a function of \(x\) from the given equation of ellipse.
(ii) Integrate the function obtained in (i) with respect to \(x\).
(iii)(a) Find the area of the region enclosed within the elliptical ground excluding the track using integration.
OR
(iii)(b) Write the coordinates of the points \(P\) and \(Q\) where the outer edge of the track cuts \(x\)-axis and \(y\)-axis in first quadrant and find the area of triangle formed by points \(P,O,Q\).