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Question: The de-Broglie wavelength of a free electron with kinetic energy \['E'\] is \[\lambda \]. If the kin...

The de-Broglie wavelength of a free electron with kinetic energy E'E' is λ\lambda . If the kinetic energy of the electron is doubled, the de-Broglie wavelength is
A.λ2A.\dfrac{\lambda }{{\sqrt 2 }}
B.2λB.\sqrt 2 \lambda
C.λ2C.\dfrac{\lambda }{2}
D.2λD.2\lambda

Explanation

Solution

We will use the equation to find de-Broglie wavelength to find the kinetic energy of the electron with wavelength λ\lambda . De-Broglie wavelength of a particle is inversely proportional to the momentum of that particular body. We should know that kinetic energy and momentum of a particle is related as K.E=P22mK.E = \dfrac{{{P^2}}}{{2m}} where PP is momentum of body and mm is the mass of the body.

Formula used:
λ=h2mK.E\lambda = \dfrac{h}{{\sqrt {2mK.E} }}

Complete step by step answer:
The formula for finding de-Broglie wavelength is given as,
λ=hP=hmv\lambda = \dfrac{h}{P} = \dfrac{h}{{mv}}
Where, hh is the planck's constant.
Where, mm is the mass of that particle.
Now, K.E=P22mK.E = \dfrac{{{P^2}}}{{2m}}
P=2m(K.E)\Rightarrow P = \sqrt {2m\left( {K.E} \right)}
Now, substituting this equation for P in the de-Broglie equation, we will get,
λ=hP=h2m(K.E)\lambda = \dfrac{h}{P} = \dfrac{h}{{\sqrt {2m\left( {K.E} \right)} }}
Where, λ\lambda is the wavelength of the electron.
hh is the planck's constant having the value 6.626×10346.626 \times {10^{ - 34}}.
mm is the mass of the electron) 9.1×1031kg9.1 \times {10^{ - 31}}kg.
And K.E is the kinetic energy of the electron.
So,the de-Broglie wavelength of a free electron with kinetic energy K.EK.E is given as λ\lambda .Now we find the de-Broglie wavelength if the kinetic energy gets doubled
λ1=λ{\lambda _1} = \lambda
K.E1=K.EK.{E_1} = K.E
K.E2=2K.EK.{E_2} = 2K.E
λ2=?{\lambda _2} = ?
From the above derived formulae we can write
λ1=h2m(K.E1){\lambda _1} = \dfrac{h}{{\sqrt {2m\left( {K.{E_1}} \right)} }} …….(1)
λ2=h2m(K.E2){\lambda _2} = \dfrac{h}{{\sqrt {2m\left( {K.{E_2}} \right)} }}……..(2)
Now we take ratio of (1) by (2) we get
λ1λ2=h2m(K.E1)h2m(K.E2)\dfrac{{{\lambda _1}}}{{{\lambda _2}}} = \dfrac{{\dfrac{h}{{\sqrt {2m\left( {K.{E_1}} \right)} }}}}{{\dfrac{h}{{\sqrt {2m\left( {K.{E_2}} \right)} }}}}
λ1λ2=2m(K.E2)2m(K.E1)=(K.E2)(K.E1)=(K.E2)(K.E1)\Rightarrow \dfrac{{{\lambda _1}}}{{{\lambda _2}}} = \dfrac{{\sqrt {2m\left( {K.{E_2}} \right)} }}{{\sqrt {2m\left( {K.{E_1}} \right)} }} = \dfrac{{\sqrt {\left( {K.{E_2}} \right)} }}{{\sqrt {\left( {K.{E_1}} \right)} }} = \sqrt {\dfrac{{\left( {K.{E_2}} \right)}}{{\left( {K.{E_1}} \right)}}}
We were given the kinetic energy get doubled so taking K.E2=2K.E1K.{E_2} = 2K.{E_1} we get
λ1λ2=(2K.E1)(K.E1)=2\dfrac{{{\lambda _1}}}{{{\lambda _2}}} = \sqrt {\dfrac{{\left( {2K.{E_1}} \right)}}{{\left( {K.{E_1}} \right)}}} = \sqrt 2
λ2=λ12\Rightarrow {\lambda _2} = \dfrac{{{\lambda _1}}}{{\sqrt 2 }}
Therefore, the de-Broglie wavelength becomes λ2\dfrac{\lambda }{{\sqrt 2 }} if the kinetic energy gets doubled.

Note:
In questions like this, remembering the relation between wavelength and kinetic energy of a particle directly will help to solve the problem quickly. The matter shows wave- particle duality relation that means at one moment the matter shows the wave behaviour and at another moment it acts like a particle. De-Broglie used the wave behaviour of the matter and gave the relations between the momentum and the wavelength of the particle.