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Question: The ratio of de-Broglie wavelengths of proton and \( \alpha \) -particle having same kinetic energy ...

The ratio of de-Broglie wavelengths of proton and α\alpha -particle having same kinetic energy is
(A) 2:1\sqrt 2 :1
(B) 22:12\sqrt 2 :1
(C) 2:12:1
(D) 4:14:1

Explanation

Solution

It is known that the de-Broglie wavelength of a particle is given by, λ=hp\lambda = \dfrac{h}{p} where is the Planck’s constant and pp is the momentum of the particle. The value of Planck’s constant is given by, h=6.626×1034Jsh = 6.626 \times {10^ - }^{34}Js .

Complete step by step answer:
Here, we have given two particles one is a proton and another is an alpha particle with the same kinetic energy.
Now, we know that the de-Broglie wavelength of a particle is given by, λ=hp\lambda = \dfrac{h}{p} where is the Planck’s constant and pp is the momentum of the particle. The value of Planck’s constant is given by, h=6.626×1034Jsh = 6.626 \times {10^ - }^{34}Js .
So, the de-Broglie wavelength of the alpha particle will be, λα=hp1{\lambda _\alpha } = \dfrac{h}{{{p_1}}} where, p1{p_1} is the momentum of the alpha particle.
The de-Broglie wavelength of the proton will be λp=hp2{\lambda _p} = \dfrac{h}{{{p_2}}} , p2{p_2} is the momentum of the proton.
Now, we have given here the kinetic energy of both the particles are same and kinetic energy of a particle in terms of momentum can be written as, E=p22mE = \dfrac{{{p^2}}}{{2m}}
Or, momentum can be written as p=2mEp = \sqrt {2mE}
So, we can write, the kinetic energy of the alpha particle Eα=p122mα{E_\alpha } = \dfrac{{{p_1}^2}}{{2{m_\alpha }}}
And the kinetic energy of the proton is Ep=p222mp{E_p} = \dfrac{{{p_2}^2}}{{2{m_p}}} .
Now, we have here the kinetic energies are equal. So we can write, Ep=Eα{E_p} = {E_\alpha }
Also we know that mass of an alpha particle is four times the proton so we can write, mα=4mp{m_\alpha } = 4{m_p}
Putting these values in de-Broglie’s wavelength and dividing we have,
λpλα=hp1hp2=p1p2\dfrac{{{\lambda _p}}}{{{\lambda _\alpha }}} = \dfrac{{\dfrac{h}{{{p_1}}}}}{{\dfrac{h}{{{p_2}}}}} = \dfrac{{{p_1}}}{{{p_2}}}
Or, λpλα=2mαE2mpE\dfrac{{{\lambda _p}}}{{{\lambda _\alpha }}} = \dfrac{{\sqrt {2{m_\alpha }E} }}{{\sqrt {2{m_p}E} }}
Putting, mα=4mp{m_\alpha } = 4{m_p} we get,
Or, λpλα=24mpE2mpE\dfrac{{{\lambda _p}}}{{{\lambda _\alpha }}} = \dfrac{{\sqrt {2 \cdot 4{m_p}E} }}{{\sqrt {2{m_p}E} }}
Or, λpλα=22mpE2mpE\dfrac{{{\lambda _p}}}{{{\lambda _\alpha }}} = 2\dfrac{{\sqrt {2{m_p}E} }}{{\sqrt {2{m_p}E} }}
Or, λpλα=2\dfrac{{{\lambda _p}}}{{{\lambda _\alpha }}} = 2
So, the ratio of their de-Broglie wavelength is, 2:12:1
Hence, option (C ) is correct.

Note:
We can observe that if the kinetic energy of the particles are equal then the ratio of their de-Broglie wavelength depends on the square root of their masses. In general we can write the ratio of the de-Broglie’s wavelength of two particles is λ1:λ2=m2:m1{\lambda _1}:{\lambda _2} = \sqrt {{m_2}} :\sqrt {{m_1}} .