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The Sigma Insight: Nucleus and Nuclear Reaction
The Geometry of the Nucleus
Calculating Nuclear Radii
When we dive into the microscopic world of atoms, the nucleus sits at the very center, holding almost all the mass. But how big is it? Unlike everyday objects, we can't just take a ruler and measure a nucleus. Instead, physicists have discovered a beautiful, simple relationship between the number of nucleons (protons and neutrons) in a nucleus and its physical size.
The Empirical Formula for Nuclear Radius
Through scattering experiments, it was found that the volume of a nucleus is directly proportional to its mass number, . Since volume scales with the cube of the radius (), it naturally follows that the radius scales with the cube root of the mass number. This gives us the famous empirical formula:
Here, is a constant, roughly equal to (femtometers, where ). This formula implies that nuclear matter has a constant density, regardless of whether it's a light element like Carbon or a heavy one like Uranium.
The Power of Ratios
In our problem, we are given the radius of an Aluminum nucleus () as and asked to find the radius of a Tellurium nucleus ().
Instead of calculating from the Aluminum data and then plugging it into the Tellurium equation, we can use a much more elegant mathematical tool: ratios. By dividing the equation for Tellurium by the equation for Aluminum, the constant completely cancels out!
Final Calculation
Now, we simply substitute the known values into our ratio equation. The mass number of Tellurium is , and for Aluminum, it is .
Notice how perfectly these numbers are chosen? Both and are perfect cubes! The cube root of is , and the cube root of is .
Cross-multiplying gives us our final answer:
The radius of the Tellurium nucleus is exactly . This method of using ratios is a powerful technique in physics, saving time and reducing the chance of calculation errors.
Similar Questions
JEE Main 2020
LEVELJEE Main
The radius of a nucleus of mass number can be estimated by the formula m. It follows that the mass density of a nucleus is of the order of ( kg)
(A)
(B)
(C)
(D)
LEVELJEE Advanced
Let be the mass of proton, the mass of neutron. the mass of nucleus and the mass of nucleus. Then
* Multiple Correct Options
(A)
(B)
(C)
(D)
JEE Main 2021
LEVELJEE Main
From the given data, the amount of energy required to break the nucleus of aluminium is . Mass of neutron Mass of proton Mass of aluminium nucleus (Assume corresponds to joule of energy) (Round off to the nearest integer)
JEE Advanced 2016
LEVELJEE Advanced
The electrostatic energy of protons uniformly distributed throughout a spherical nucleus of radius is given by The measured masses of the neutron, , and are , , and , respectively. Given that the radii of both the and nuclei are same, ( is the speed of light) and . Assuming that the difference between the binding energies of and is purely due to the electrostatic energy, the radius of either of the nuclei is ()
(A)
2.85 fm
(B)
3.03 fm
(C)
3.42 fm
(D)
3.80 fm
LEVELJEE Main
A nucleus disintegrates into two nuclear parts which have their velocities in the ratio . The ratio of their nuclear sizes will be
(A)
(B)
(C)
(D)
JEE Main 2019
LEVELBoard
The ratio of mass densities of nuclei of and is close to
(A)
5
(B)
2
(C)
0.1
(D)
1
LEVELJEE Main
An -particle of energy is scattered through by a fixed uranium nucleus. The distance of the closest approach is of the order of
(A)
(B)
(C)
(D)
LEVELJEE Main
Order of magnitude of density of uranium nucleus is ()
(A)
(B)
(C)
(D)
JEE Advanced 2007
LEVELJEE Main
In the options given below, let denote the rest mass energy of a nucleus and a neutron. The correct option is
(A)
(B)
(C)
(D)
JEE Advanced 2013
LEVELJEE Advanced
Comprehension Passage
The mass of a nucleus is less than the sum of the masses of number of neutrons and number of protons in the nucleus. The energy equivalent to the corresponding mass difference is known as the binding energy of the nucleus. A heavy nucleus of mass can break into two light nuclei of masses and only if . Also two light nuclei of masses and can undergo complete fusion and form a heavy nucleus of mass only if . The masses of some neutral atoms are given in the table below:
$\begin{array}{llll}
_{1}^{1}\text{H} & 1.007825\text{u} & _{1}^{2}\text{H} & 2.014102\text{u} \\
_{3}^{6}\text{Li} & 6.01513\text{u} & _{3}^{7}\text{Li} & 7.016004\text{u} \\
_{64}^{152}\text{Gd} & 151.919803\text{u} & _{82}^{206}\text{Pb} & 205.974455\text{u} \\
_{1}^{3}\text{H} & 3.016050\text{u} & _{2}^{4}\text{He} & 4.002603\text{u} \\
_{30}^{70}\text{Zn} & 69.925325\text{u} & _{34}^{82}\text{Se} & 81.916709\text{u} \\
_{84}^{210}\text{Po} & 209.982876\text{u} & &
\end{array}$
Question 1:
The correct statement is
(A)
The nucleus can emit an alpha particle.
(B)
The nucleus can emit a proton.
(C)
Deuteron and alpha particle can undergo complete fusion.
(D)
The nuclei and can undergo complete fusion.
Question 2:
The kinetic energy (in keV) of the alpha particle, when the nucleus at rest undergoes alpha decay, is
(A)
5316
(B)
5422
(C)
5707
(D)
5818
