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Core Syllabus Module

Atoms and Nuclei

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Chapter Elite-20 Challenge Zone

Target Advanced
JEE Advanced 2010
LEVELJEE Advanced

Comprehension Passage

The key feature of Bohr's theory of spectrum of hydrogen atom is the quantisation of angular momentum when an electron is revolving around a proton. We will extend this to a general rotational motion to find quantised rotational energy of a diatomic molecule assuming it to be rigid. The rule to be applied is Bohr's quantisation condition.
Question 1:

A diatomic molecule has moment of inertia . By Bohr's quantization condition its rotational energy in the level ( is not allowed) is

(A)
(B)
(C)
(D)
Question 2:

It is found that the excitation frequency from ground to the first excited state of rotation for the CO molecule is close to . Then the moment of inertia of CO molecule about its centre of mass is close to (Take )

(A)
(B)
(C)
(D)
Question 3:

In a CO molecule, the distance between C (mass ) and O (mass ), where , is close to

(A)
(B)
(C)
(D)
JEE Advanced 2008
LEVELJEE Advanced

Comprehension Passage

In a mixture of H - He gas (He is singly ionized He atom), H atoms and He ions are excited to their respective first excited states. Subsequently, H atoms transfer their total excitation energy to He ions (by collisions). Assume that the Bohr model of atom is exactly valid.
Question 1:

The quantum number of the state finally populated in He ions is

(A)
2
(B)
3
(C)
4
(D)
5
Question 2:

The wavelength of light emitted in the visible region by He ions after collisions with H atoms is

(A)
(B)
(C)
(D)
Question 3:

The ratio of the kinetic energy of the electron for the H atom to that of He ion is

(A)
1/4
(B)
1/2
(C)
1
(D)
2
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