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LEVELJEE Main

Animated Solution for Physics - Atoms and Nuclei: The binding energy per nucleon of deuteron () and helium nucleus () is and respectively. If two deuteron nuclei react to form a single helium nucleus, then the energy released is

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The Sigma Insight: Nucleus and Nuclear Reaction

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The Power of Fusion

Calculating Energy Release in Nuclear Reactions
Have you ever wondered what powers the Sun and the stars? The answer lies in the incredible process of nuclear fusion, where light atomic nuclei combine to form heavier, more stable ones. In this problem, we are going to explore a miniature version of this cosmic event: the fusion of two deuteron nuclei to form a single helium nucleus.
Our goal is to calculate the exact amount of energy released during this reaction. To do this, we need to understand the concept of binding energy.

Understanding Binding Energy

Binding energy is the energy required to completely disassemble a nucleus into its constituent protons and neutrons. Conversely, it is also the energy released when those nucleons bind together to form the nucleus.
A crucial metric is the binding energy per nucleon. This tells us how tightly bound each individual proton or neutron is within the nucleus. The higher the binding energy per nucleon, the more stable the nucleus.
When a nuclear reaction occurs, the energy released (often called the Q-value) is simply the difference between the total binding energy of the final products and the total binding energy of the initial reactants:
Let's break down our specific reaction step-by-step.

Analyzing the Reactants

Deuterium
Our reactants are two deuteron nuclei (). A deuteron is an isotope of hydrogen containing one proton and one neutron, giving it a total of nucleons.
The problem states that the binding energy per nucleon for a deuteron is .
To find the total binding energy of a single deuteron, we multiply the binding energy per nucleon by its total number of nucleons:
Since our reaction involves two deuterons fusing together, we must account for both of them. Therefore, the total binding energy of our reactants is:

Analyzing the Product

Helium
When the two deuterons fuse, they form a single helium nucleus (), also known as an alpha particle. This nucleus contains two protons and two neutrons, making a total of nucleons.
Helium is a remarkably stable nucleus. The problem gives its binding energy per nucleon as .
Just like we did for the deuterons, we calculate the total binding energy of the helium nucleus by multiplying its binding energy per nucleon by its total number of nucleons:

The Final Calculation

Energy Released
Now we have all the pieces of the puzzle. We know the total binding energy of what we started with (the reactants) and what we ended up with (the product).
To find the energy released (), we subtract the reactants' binding energy from the product's binding energy:
And there we have it! The fusion of two deuterons into a helium nucleus releases a massive of energy.
This result perfectly illustrates a fundamental principle of nuclear physics: whenever light nuclei fuse to form a nucleus with a higher binding energy per nucleon, the system transitions to a lower, more stable energy state, and the "excess" energy is radiated away into the universe.

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The binding energies per nucleon for deuteron () and helium () are and respectively. The energy released when two deuterons fuse to form a helium nucleus () is ......... .

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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