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Question: In the H-atom if x is the radius of the first Bohr orbit, the De Broglie wavelength of an electron i...

In the H-atom if x is the radius of the first Bohr orbit, the De Broglie wavelength of an electron in 3rd3rd orbit is:
A. 3πx3\pi x
B. 6πx6\pi x
C. 9x2\dfrac{{9x}}{2}
D. x2\dfrac{x}{2}

Explanation

Solution

In the question, we have to calculate the De-Broglie wavelength. Using the Bohr postulates, the relation was determined for the radius of Bohr orbit.
We have, mvr=nh2πmvr = \dfrac{{nh}}{{2\pi }} ; v represents the velocity of an electron, r represents the radius, h represents Planck’s constant, n represents the principal quantum number of orbit.
Here, the mentioned expression is being used for angular momentum given by De-Broglie.
Further the general formula was determined for radius that can be written as r=n2h24π2mZKe2r = \dfrac{{{n^2}{h^2}}}{{4{\pi ^2}mZK{e^2}}}

Complete step by step answer:
As we already mentioned the general formula the radius of nth{n^{th}} Bohr orbit i.e.
r=n2h24π2mZKe2r = \dfrac{{{n^2}{h^2}}}{{4{\pi ^2}mZK{e^2}}}
n represents the principal quantum number of orbits like n is 0, 1, 2, …
h represents the Planck’s constant
m represents the mass of an electron
K represents the Coulomb’s constant
e represents the charge of an electron
In this expression Z represents the atomic number.
Now, we know that the atomic number of hydrogen is 1.
Therefore, the expression of radius for hydrogen atom will be as follows:
r=n2h24π2mKe2r = \dfrac{{{n^2}{h^2}}}{{4{\pi ^2}mK{e^2}}}
So, we can say that according to the Bohr rαn2r\alpha {n^2}
We are given that x is the radius of Bohr’s first orbit (r1{r_1}), thus using the above expression we can write it as follows:
r1r3=n12n32\dfrac{{{r_1}}}{{{r_3}}} = \dfrac{{{n_1}^2}}{{{n_3}^2}} Here r3{r_3} represents the radius of 3rd3rd orbit.
r1r3=1232\Rightarrow \dfrac{{{r_1}}}{{{r_3}}} = \dfrac{{{1^2}}}{{{3^2}}}
r3=9r1\Rightarrow {r_3} = 9{r_1} (Solving it in terms of r1{r_1})
Here we know r1{r_1} is x.
So, r3=9x{r_3} = 9x
Now, if we see the expression given by De-Broglie for angular momentum i.e.
mvr=nh2πmvr = \dfrac{{nh}}{{2\pi }}
If the electron is in 3rd3rd orbit then mvr3=3h2πmv{r_3} = \dfrac{{3h}}{{2\pi }}
hmv=2πr33\Rightarrow \dfrac{h}{{mv}} = \dfrac{{2\pi {r_3}}}{3}
We know that De-Broglie have given the expression for wavelength which can be written as:
λ=hmv\lambda = \dfrac{h}{{mv}} ; λ\lambda is the De-Broglie wavelength
Thus, λ=2πr33\lambda = \dfrac{{2\pi {r_3}}}{3}
After substituting the value of r3{r_3} in the above expression, we get
λ=2π9x3\lambda = \dfrac{{2\pi 9x}}{3}
λ=6πx\Rightarrow \lambda = 6\pi x
In the last, we can conclude that the wavelength for electron in 3rd3rd orbit is 6πx6\pi x

So, the correct answer is Option B.

Note: We have come across the term ‘angular momentum of electron’. The concept of angular momentum is given by De-Broglie. The electron revolving around the nucleus shows both wave and particle character. The circumference of the orbit is considered to be an integral multiple of the wavelength of the electron whose wave is existing in the phase.