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Question

Question: The expression for the Bohr radius of hydrogen-like species is: (A) \[\dfrac{{{n^2}{h^2}}}{{4{\pi ...

The expression for the Bohr radius of hydrogen-like species is:
(A) n2h24π2me2Z\dfrac{{{n^2}{h^2}}}{{4{\pi ^2}m{e^2}Z}}
(B) 1n2[h24π2m(Ze2/4πε0)]\dfrac{1}{{{n^2}}}\left[ {\dfrac{{{h^2}}}{{4{\pi ^2}m(Z{e^2}/4\pi {\varepsilon _0})}}} \right]
(C) n2[4π2mh2(Ze2/4πε0]{n^2}\left[ {\dfrac{{4{\pi ^2}m{h^2}}}{{(Z{e^2}/4\pi {\varepsilon _0}}}} \right]
(D) 1n2[4π2mh2(Ze2/4πε0]\dfrac{1}{{{n^2}}}\left[ {\dfrac{{4{\pi ^2}m{h^2}}}{{(Z{e^2}/4\pi {\varepsilon _0}}}} \right]

Explanation

Solution

Neils Bohr was the first Scientist who explained the H-atom structure and its spectrum. He gave many postulates regarding the position of electrons, radius, and energy structure of Hydrogen atoms. The expression for the radius of H-atom can be deduced by equating the centripetal force and the electrostatic force of attraction. We will use the relation between the angular momentum of electrons from one of Bohr’s postulates.

Complete step by step solution:
Let charge on electron be ‘e’
Let the mass of electron be ‘m’
Let the velocity of the electron be ‘v’
Let the radius of the orbit be ‘r’.
Ze is the positive charge on the nucleus of an atom, where Z == atomic number (For H-atom Z=1Z = 1).
Since electrons revolve in the orbit with a negative charge on them and the nucleus being in the centre. So here, the centripetal force will provide the necessary electrostatic force of attraction. So now,
mv2r=14πε0[k(Ze)(e)r2]\dfrac{{m{v^2}}}{r} = \dfrac{1}{{4\pi {\varepsilon _0}}}\left[ {\dfrac{{k(Ze)(e)}}{{{r^2}}}} \right]
mv2=[k(Ze2)4πε0r].....(i)m{v^2} = \left[ {\dfrac{{k(Z{e^2})}}{{4\pi {\varepsilon _0}r}}} \right].....(i)
By Bohr’s postulate, the angular momentum of electron is given as:
mvr=nh2π.....(ii)mvr = n\dfrac{h}{{2\pi }}.....(ii)
Where n=1,2,3....n = 1,2,3.... now, Squaring (ii) and dividing by (i) we get,
r=n2h2ε0πmZe2r = {n^2}\dfrac{{{h^2}{\varepsilon _0}}}{{\pi mZ{e^2}}}
For H-atom Z=1Z = 1, so it will be,
r=n2h2ε0πme2r = \dfrac{{{n^2}{h^2}{\varepsilon _0}}}{{\pi m{e^2}}}
The required expression is,
r=n2h2ε0πme2r = \dfrac{{{n^2}{h^2}{\varepsilon _0}}}{{\pi m{e^2}}}
Where ‘r’ is the radius of the electron and n=1,2,3....n = 1,2,3.... (Principal quantum number)
ε0=8.85×1012{\varepsilon _0} = 8.85 \times {10^{ - 12}},π=3.14\pi = 3.14, h=h = Planck’s Constant, m=m = mass of electron,
Therefore, Option, ‘(D) 1n2[4π2mh2(Ze2/4πε0]\dfrac{1}{{{n^2}}}\left[ {\dfrac{{4{\pi ^2}m{h^2}}}{{(Z{e^2}/4\pi {\varepsilon _0}}}} \right]’ is the correct answer.

Note: While equating the equations calculations should be done carefully and the correct relation of angular momentum must be used to derive the desired equation in the correct order. If you put all the constant values in the equation for hydrogen first energy level then you will get the value of radius of hydrogen atom will be 0.529A00.529{{ }}{A^0}. Neil Bohr also gave expression for different energy levels of the hydrogen spectra.