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Question: An \(\alpha \) particle having energy \(10MeV\) collides with a nucleus of atomic number 50. Then di...

An α\alpha particle having energy 10MeV10MeV collides with a nucleus of atomic number 50. Then distance of closest approach will be
A. 14.4×10−16m B. 1.7×10−7m C. 1.4×10−12m D. 14.4×10−15m \begin{aligned} & \text{A}\text{. }14.4\times {{10}^{-16}}m \\\ & \text{B}\text{. }1.7\times {{10}^{-7}}m \\\ & \text{C}\text{. }1.4\times {{10}^{-12}}m \\\ & \text{D}\text{. }14.4\times {{10}^{-15}}m \\\ \end{aligned}

Explanation

Solution

- Hint: The scattering of an alpha particle through a large angle with respect to its original direction of motion is caused by an atom whose most of the mass and all of the positive electric charge is being concentrated at the center or the nucleus of the atom. In this collision between the alpha particle and the atom, we define a term known as distance of closest approach, which is the distance between the centres of the alpha particle and the atom. At the distance of closest approach, the kinetic energy of the alpha particle is converted into its potential energy.

Complete step-by-step solution
The distance of the closest approach of two particles is defined as the distance between their centers when the particles are externally tangent to each other. The objects can be exact geometric shapes or physical particles with well-defined boundaries. The distance of closest approach is also called the contact distance.
For the simplest objects, such as spheres, the distance of closest approach is the sum of their radii. For non-spherical objects, the distance of closest approach is a function of the orientation of the objects in the space.


At the distance of closest approach, the whole kinetic energy of the particle gets converted into potential energy.
Therefore,
KE=14πεo2Ze2rKE=\dfrac{1}{4\pi {{\varepsilon }_{o}}}\dfrac{2Z{{e}^{2}}}{r}
Where,
ZZ is the atomic number
ee is the charge on an electron
rr is the distance of closest approach
Putting values,
KE=10×1.6×10−13 14πεo=9×109 Z=50 e=1.6×10−19 \begin{aligned} & KE=10\times 1.6\times {{10}^{-13}} \\\ & \dfrac{1}{4\pi {{\varepsilon }_{o}}}=9\times {{10}^{9}} \\\ & Z=50 \\\ & e=1.6\times {{10}^{-19}} \\\ \end{aligned}
We get,
10×1.6×10−13=9×109×2×50×(1.6×10−19)2r r=9×109×2×50×(1.6×10−19)210×1.6×10−13 r=14.4×10−15m \begin{aligned} & 10\times 1.6\times {{10}^{-13}}=9\times {{10}^{9}}\times \dfrac{2\times 50\times {{\left( 1.6\times {{10}^{-19}} \right)}^{2}}}{r} \\\ & r=\dfrac{9\times {{10}^{9}}\times 2\times 50\times {{\left( 1.6\times {{10}^{-19}} \right)}^{2}}}{10\times 1.6\times {{10}^{-13}}} \\\ & r=14.4\times {{10}^{-15}}m \\\ \end{aligned}
The distance of closest approach is 14.4×10−15m14.4\times {{10}^{-15}}m
Hence, the correct option is D.

Note: Students should note the key difference between the distance of closest approach and the impact meter. Distance of closest approach is the distance between the centre of nucleus and the point from which the alpha particle, which is approaching directly to the nucleus, returns, while Impact parameter is expressed as the perpendicular distance of the velocity vector of the alpha particle from the central line of the nucleus; when the particle is far away from the atom.
Distance of closest approach is expressed as rr Impact parameter is expressed as bb.