LEVELJEE Main
Visualized Solution
The Sigma Insight: Nucleus and Nuclear Reaction
The Cosmic Engine
Have you ever looked up at the night sky and wondered what powers those brilliant points of light? The answer lies in the very heart of atoms, in a process called nuclear fusion.
This is the exact same process we are going to explore in this problem. We are looking at the fusion of two deuteron nuclei to form a single helium nucleus.
Analyzing the Setup Let us break down the players in our cosmic drama
We start with two deuterons. A deuteron is the nucleus of deuterium, a heavy isotope of hydrogen, consisting of one proton and one neutron.
When these two deuterons collide with enough energy, they overcome their electrostatic repulsion and fuse together. The result is a helium-4 nucleus, also known as an alpha particle, which contains two protons and two neutrons.
But here is the magical part: the mass of the resulting helium nucleus is slightly less than the combined mass of the two original deuterons. Where did this missing mass go?
According to Einstein's famous equation, it is converted into pure energy!
The Master Equation To calculate this released energy, we do not need to measure the masses directly
We can use the concept of binding energy.
Binding energy is the energy required to completely disassemble a nucleus into its constituent protons and neutrons. Conversely, it is the energy released when those nucleons bind together to form the nucleus.
The problem gives us the binding energy per nucleon. This is a measure of how tightly bound the nucleus is. A higher binding energy per nucleon means a more stable nucleus.
The total energy released in a fusion reaction is simply the difference between the total binding energy of the products and the total binding energy of the reactants.
Calculating the Reactant Energy Let us calculate the total binding energy of our reactants
We have two deuterons.
Each deuteron has nucleons. The problem states that the binding energy per nucleon for a deuteron is .
So, the binding energy of one deuteron is .
Since we have two deuterons fusing, the total binding energy of the reactants is:
Calculating the Product Energy
Now, let us look at our product, the helium nucleus.
A helium-4 nucleus has nucleons. Its binding energy per nucleon is given as . This high value indicates that helium-4 is an exceptionally stable nucleus.
The total binding energy of the helium nucleus is:
Final Calculation We are now ready for the final step
We subtract the total binding energy of the reactants from the total binding energy of the product.
This is the energy released in just one single fusion event!
While might seem like a tiny amount of energy on a macroscopic scale, remember that a single gram of deuterium contains roughly atoms. If all of them fused, the energy released would be astronomical.
This is the very principle that scientists and engineers are trying to harness in fusion reactors on Earth, hoping to provide a clean, virtually limitless source of energy for the future.
Similar Questions
LEVELJEE Main
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
(A)
(B)
(C)
(D)
LEVELJEE Main
Consider the reaction : . Mass of the deuterium atom = 2.0141 u. Mass of helium atom = 4.0024 u. This is a nuclear ........ reaction in which the energy released is ...... MeV.
LEVELJEE Main
If the binding energy per nucleon in and nuclei are and respectively, then in the reaction energy of proton must be
(A)
(B)
(C)
(D)
JEE Main 2019
LEVELJEE Main
Consider the nuclear fission Given that the binding energy/nucleon of , and are respectively, , and , identify the correct statement.
(A)
Energy of will be released.
(B)
Energy of will be supplied.
(C)
energy will be released.
(D)
Energy of has to be supplied.
LEVELJEE Main
If a star can convert all the He nuclei completely into oxygen nuclei. The energy released per oxygen nuclei is : (Mass of the helium nucleus is and mass of oxygen nucleus is )
(A)
(B)
(C)
(D)
LEVELJEE Advanced
It is proposed to use the nuclear fusion reaction; in a nuclear reactor of rating. If the energy from the above reaction is used with a per cent efficiency in the reactor, how many grams of deuterium fuel will be needed per day? (The masses of and are atomic mass units and atomic mass units respectively.)
LEVELJEE Advanced
Assume that a neutron breaks into a proton and an electron. The energy released during this process is (mass of neutron kg, mass of proton kg, mass of electron kg)
(A)
MeV
(B)
MeV
(C)
MeV
(D)
MeV
JEE Main 2020
LEVELJEE Advanced
You are given that mass of , mass of and mass of . When of is converted into by proton capture, the energy liberated (in ), is [Mass of nucleon ]
(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
LEVELJEE Advanced
A star initially has deuterons. It produces energy via the processes and . If the average power radiated by the star is W, the deuteron supply of the star is exhausted in a time of the order of The mass of the nuclei are as follows: ; ; ; .
(A)
s
(B)
s
(C)
s
(D)
s
