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Question: The potential difference applied to an X-ray tube is\(V\). The ratio of the de Broglie wavelength of...

The potential difference applied to an X-ray tube isVV. The ratio of the de Broglie wavelength of electron to the minimum wavelength of X-ray is directly proportional to:
A.VV
B.V\sqrt V
C.V32V^{\dfrac{3}{2}}
D.V72 V^{\dfrac{7}{2}}

Explanation

Solution

Hint: The question involves the ratio of the two forms of de Broglie equations, namely the electron or particle and x-ray or the photon. For x-rayλx=hceV\lambda_{x}=\dfrac{hc}{eV} and for electronsλe=h2meV\lambda_{e}=\dfrac{h}{\sqrt{2meV}}. Also that the kinetic energy E=eVE=eV is in both the cases.

Formula used: λx=hceV\lambda_{x}=\dfrac{hc}{eV}
λe=h2meV\lambda_{e}=\dfrac{h}{{\sqrt {2meV}}}

Complete step-by-step solution -
The ratio of the de Broglie wavelength of electron to the minimum wavelength of X-ray is given by the relationship between wavelength λ\lambda and kinetic energy EE is different for particles and photons.
For x-ray:E=hf=hcλxE=hf=\dfrac{hc}{\lambda_{x}} where E=eVE=eV ie the kinetic energy of the electrons ee accelerated through a potential difference (voltage) VV, hh is the Planck’s constant and cc is the speed of light.
Thus can also be written as: eV=hcλxeV= \dfrac{hc}{\lambda_{x}} or λx=hceV\lambda_{x}=\dfrac{hc}{eV}
For electron: E=eV=12×mv2=p22mE=eV=\dfrac{1}{2}\times mv^{2}=\dfrac{p^{2}}{2m} or p=2mEp=\sqrt{2mE} where pp is momentum of the electron and mm is the mass of the electron. And λe=hp=h2mE=h2meV\lambda_{e}=\dfrac{h}{p}=\dfrac{h}{\sqrt{2mE}}= \dfrac{h}{\sqrt{2meV}}
Thus taking the ratio
λeλx=h2meVhceV\dfrac{\lambda_{e}}{\lambda_{x}}=\dfrac{\dfrac{h}{\sqrt{2meV}}}{\dfrac{hc}{eV}}
λeλx=h2meV×eVhc\dfrac{\lambda_{e}}{\lambda_{x}}= \dfrac{h}{\sqrt{2meV}}\times \dfrac{eV}{hc}
λeλxVV\dfrac{\lambda_{e}}{\lambda_{x}}\propto\dfrac{V}{\sqrt V}
λeλxV\dfrac{\lambda_{e}}{\lambda_{x}}\propto \sqrt V
Hence, The ratio of the de Broglie wavelength of electron to the minimum wavelength of X-ray is directly proportional to B.V\sqrt V

Additional Information:
In 1924 a French physicist Louis de Broglie, gave the De Broglie wavelength, is given by the wave-particle duality, where the wavelength of all the objects in quantum mechanics, is given by the probability density of finding the object at a given any point of the space. The de Broglie wavelength of a particle is inversely proportional to its momentum. Matter waves were first experimentally confirmed to occur in George Paget Thomson's cathode ray diffraction experiment and the Davisson-Germer experiment for electrons, and the de Broglie hypothesis has been confirmed for other elementary particles.

Note: The de Broglie wavelength is expressed in two forms, one for photons and another of particles. Also be careful when taking the ratio between two terms. Be cautious while simplifying the ratios. Note that the kinetic energy E=eVE=eV is in both the cases. . For electrons, de Broglie wavelength λe1m\lambda_{e}\propto \dfrac{1}{\sqrt m} andλe1V\lambda_{e}\propto \dfrac{1}{\sqrt V}.
For X-ray, de Broglie wavelength λx1V\lambda_{x}\propto \dfrac{1}{V}