Question
Question: Calculate the height of the potential barrier for a head on collision of two deuterons....
Calculate the height of the potential barrier for a head on collision of two deuterons.
Solution
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=4π∈∘1rq1q2
Where U= potential energy or barrier, q1,q2 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=4π∈∘1rq1q2 ………………(1)
Where U= potential barrier, q1,q2 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, q1=q2=1.6×10−19C
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=r0A1/3
Where r0 = 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 = 1.6×21/3
So the radius of a deuteron nucleus = 2fm (Fermi meter)
Therefore r=2+2=4fm
Since, 1fm=10−15m
⇒r=4×10−15m
4π∈∘1=9×109Nm2C−2
Step2: Substituting all the values in equation (1) and simplify
⇒ U=9×1094×10−15(1.6×10−19)2J.
This potential energy is in J. In order to convert it in eV divides it with charge of electron i.e. 1.6×10−19C.
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=4π∈∘1rq
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×V=4π∈∘1rq2
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.