Calculate the height of the potential barrier for a head on collision of two deuterons.
Answer
269.4k+ views
Hint: The height of potential barrier here means the electrostatic potential energy between the two deuterons so, use the equation of electrostatic potential energy between two charged particles i.e.
$U = \dfrac{1}{{4\pi { \in _ \circ }}}\dfrac{{{q_1}{q_2}}}{r}$
Where U= potential energy or barrier, ${q_1},{q_2}$ are the two charges and r= distance between the two charges
Complete step by step solution:
Step1: The potential energy for the collision of two charged particles can be given by-
$U = \dfrac{1}{{4\pi { \in _ \circ }}}\dfrac{{{q_1}{q_2}}}{r}$ ………………(1)
Where U= potential barrier, ${q_1},{q_2}$ are the two charges and r= distance between the two charges
Since the deuterons are the charged particles whose magnitude of charge is equal to that of an electron.
Therefore, ${q_1} = {q_2} = 1.6 \times {10^{ - 19}}C$
Also the distance between their centres on collision is given by-
r= radius of 1st deuteron radius of 2nd deuteron
radius of nucleus is given by-
$r = r_0 A^{1/3}$
Where ${r_ 0}$ = fermi constant = 1.6 fm, A= mass number
Since deuteron has a mass number of 2, therefore A=2
Hence radius of deuteron nucleus is given by,
$r$ = $1.6 \times 2^{1/3}$
So the radius of a deuteron nucleus = $2fm$ (Fermi meter)
Therefore \[r = 2 + 2 = 4fm\]
Since, $1fm = {10^{ - 15}}m$
\[ \Rightarrow r = 4 \times {10^{ - 15}}m\]
$\dfrac{1}{{4\pi { \in _ \circ }}} = 9 \times {10^9}N{m^2}{C^{ - 2}}$
Step2: Substituting all the values in equation (1) and simplify
$\Rightarrow$ $U = 9 \times {10^9}\dfrac{{{{\left( {1.6 \times {{10}^{ - 19}}} \right)}^2}}}{{4 \times {{10}^{ - 15}}}}J$.
This potential energy is in J. In order to convert it in eV divides it with charge of electron i.e. $1.6 \times {10^{ - 19}}C$.
Therefore,
$
\Rightarrow U = 9 \times {10^9}\dfrac{{{{\left( {1.6 \times {{10}^{ - 19}}} \right)}^2}}}{{4 \times {{10}^{ - 15}}\left( {1.6 \times {{10}^{ - 19}}} \right)}}eV \\
\Rightarrow U = 360 \times {10^3}eV \\
\Rightarrow U = 360keV \\ $
Hence the height of the potential barrier for a head on collision of two deuterons is 360keV.
Note: Always remember that there is a difference between the electrostatic potential and electrostatic potential energy. Electrostatic potential, at any point in an electric field, is defined as the amount of work done in moving a unit positive charge between infinity and that point, without any acceleration, against the electric force. Every point around a source charge is characterized with electric potential, which is given by-
$V = \dfrac{1}{{4\pi { \in _ \circ }}}\dfrac{q}{r}$
Where V= Electric potential
If instead of bringing a unit positive, we bring a charge 'q' from infinity to that point, work done W in doing so is given by-
\[W = q \times V = \dfrac{1}{{4\pi { \in _ \circ }}}\dfrac{{{q^2}}}{r}\]
This work is termed as 'electrostatic potential energy' of the charge q in the field of charge ‘q'. We can also say that the electric potential, at any point, in an electric field is the potential energy of a unit positive charge placed at that point.
$U = \dfrac{1}{{4\pi { \in _ \circ }}}\dfrac{{{q_1}{q_2}}}{r}$
Where U= potential energy or barrier, ${q_1},{q_2}$ are the two charges and r= distance between the two charges
Complete step by step solution:
Step1: The potential energy for the collision of two charged particles can be given by-
$U = \dfrac{1}{{4\pi { \in _ \circ }}}\dfrac{{{q_1}{q_2}}}{r}$ ………………(1)
Where U= potential barrier, ${q_1},{q_2}$ are the two charges and r= distance between the two charges
Since the deuterons are the charged particles whose magnitude of charge is equal to that of an electron.
Therefore, ${q_1} = {q_2} = 1.6 \times {10^{ - 19}}C$
Also the distance between their centres on collision is given by-
r= radius of 1st deuteron radius of 2nd deuteron
radius of nucleus is given by-
$r = r_0 A^{1/3}$
Where ${r_ 0}$ = fermi constant = 1.6 fm, A= mass number
Since deuteron has a mass number of 2, therefore A=2
Hence radius of deuteron nucleus is given by,
$r$ = $1.6 \times 2^{1/3}$
So the radius of a deuteron nucleus = $2fm$ (Fermi meter)
Therefore \[r = 2 + 2 = 4fm\]
Since, $1fm = {10^{ - 15}}m$
\[ \Rightarrow r = 4 \times {10^{ - 15}}m\]
$\dfrac{1}{{4\pi { \in _ \circ }}} = 9 \times {10^9}N{m^2}{C^{ - 2}}$
Step2: Substituting all the values in equation (1) and simplify
$\Rightarrow$ $U = 9 \times {10^9}\dfrac{{{{\left( {1.6 \times {{10}^{ - 19}}} \right)}^2}}}{{4 \times {{10}^{ - 15}}}}J$.
This potential energy is in J. In order to convert it in eV divides it with charge of electron i.e. $1.6 \times {10^{ - 19}}C$.
Therefore,
$
\Rightarrow U = 9 \times {10^9}\dfrac{{{{\left( {1.6 \times {{10}^{ - 19}}} \right)}^2}}}{{4 \times {{10}^{ - 15}}\left( {1.6 \times {{10}^{ - 19}}} \right)}}eV \\
\Rightarrow U = 360 \times {10^3}eV \\
\Rightarrow U = 360keV \\ $
Hence the height of the potential barrier for a head on collision of two deuterons is 360keV.
Note: Always remember that there is a difference between the electrostatic potential and electrostatic potential energy. Electrostatic potential, at any point in an electric field, is defined as the amount of work done in moving a unit positive charge between infinity and that point, without any acceleration, against the electric force. Every point around a source charge is characterized with electric potential, which is given by-
$V = \dfrac{1}{{4\pi { \in _ \circ }}}\dfrac{q}{r}$
Where V= Electric potential
If instead of bringing a unit positive, we bring a charge 'q' from infinity to that point, work done W in doing so is given by-
\[W = q \times V = \dfrac{1}{{4\pi { \in _ \circ }}}\dfrac{{{q^2}}}{r}\]
This work is termed as 'electrostatic potential energy' of the charge q in the field of charge ‘q'. We can also say that the electric potential, at any point, in an electric field is the potential energy of a unit positive charge placed at that point.
Recently Updated Pages
Circuit Switching vs Packet Switching: Key Differences Explained

JEE General Topics in Chemistry Important Concepts and Tips

JEE Extractive Metallurgy Important Concepts and Tips for Exam Preparation

JEE Atomic Structure and Chemical Bonding important Concepts and Tips

JEE Amino Acids and Peptides Important Concepts and Tips for Exam Preparation

Electricity and Magnetism Explained: Key Concepts & Applications

Trending doubts
JEE Main 2026: Exam Dates, Session 2 Updates, City Slip, Admit Card & Latest News

JEE Main Participating Colleges 2026 - A Complete List of Top Colleges

Kinematics Mock Test for JEE Main 2025-26: Comprehensive Practice

Understanding the Electric Field of a Uniformly Charged Ring

Understanding Atomic Structure for Beginners

Derivation of Equation of Trajectory Explained for Students

Other Pages
CBSE Class 12 Physics Question Paper 2026: Download SET-wise PDF with Answer Key & Analysis

JEE Advanced 2026 Notification Out with Exam Date, Registration (Extended), Syllabus and More

JEE Advanced Percentile vs Marks 2026: JEE Main Cutoff, AIR & IIT Admission Guide

JEE Advanced 2026 Marks vs Rank: Estimate IIT Rank from Your Score

JEE Advanced Weightage Chapter Wise 2026 for Physics, Chemistry, and Mathematics

JEE Main Marking Scheme 2026- Paper-Wise Marks Distribution and Negative Marking Details

