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Question: If the short wavelength limit of the continuous spectrum coming out of a Coolidge tube is 10Å, then ...

If the short wavelength limit of the continuous spectrum coming out of a Coolidge tube is 10Å, then the de Broglie wavelength of the electrons reaching the target metal in the Coolidge tube is approximately:
A. 0.3Å
B. 3Å
C. 30Å
D. 10Å

Explanation

Solution

Hint: The maximum allowed energy of particles coming out of the Coolidge tube is fixed. The electron energy is converted into X-Rays. As a result, you can apply the energy conservation theorem to find the momentum of the electron. You can use the de Broglie hypothesis to find the wavelength of the electrons.

Formula Used:
The de Broglie wavelength is given by,
λdeBroglie=hp{{\lambda }_{de-Broglie}}=\dfrac{h}{p}......................(1)
The kinetic energy of a particle is given by,
KE=p22mKE=\dfrac{{{p}^{2}}}{2m}.....................(2)
The energy of a photon is given by,
E=hcλE=\dfrac{hc}{\lambda }....................(3)

Where,
λdeBroglie{{\lambda }_{de-Broglie}} is the wavelength of the particle
λ\lambda is the wavelength of the photon
hh is the Planck’s constant
cc is the speed of light
pp is the momentum of the particles
mm is the mass of the particle

Complete step by step answer:

The short wavelength limit of the continuous spectrum is given; hence the energy of the photon is,
hcλmin\dfrac{hc}{{{\lambda }_{\min }}}

It should be equal to the Kinetic energy of the electrons,
KE=p22mKE=\dfrac{{{p}^{2}}}{2m}
Hence, we can write,
hcλmin=p22m\dfrac{hc}{{{\lambda }_{\min }}}=\dfrac{{{p}^{2}}}{2m}
p=2mhcλmin\Rightarrow p=\sqrt{\dfrac{2mhc}{{{\lambda }_{\min }}}}

So, the momentum of the electron is,
p=2mhcλminp=\sqrt{\dfrac{2mhc}{{{\lambda }_{\min }}}}

Now, we can find the de Broglie wavelength using the equation (1),
λdeBroglie=hp{{\lambda }_{de-Broglie}}=\dfrac{h}{p}
λdeBroglie=h×12mhcλmin\Rightarrow {{\lambda }_{de-Broglie}}=h\times \dfrac{1}{\sqrt{\dfrac{2mhc}{{{\lambda }_{\min }}}}}
λdeBroglie=hλmin2mc\Rightarrow {{\lambda }_{de-Broglie}}=\sqrt{\dfrac{h{{\lambda }_{\min }}}{2mc}}

We know the following,
c=3×108c=3\times {{10}^{8}}m/s
h=6.626×1034h=6.626\times {{10}^{-34}} Js
λmin=10{{\lambda }_{\min }}=10 Å
m=9.19×1031m=9.19\times {{10}^{-31}} kg

Hence, the de Broglie wavelength is,
λdeBroglie=(6.626×1034)(10×1010)2(9.19×1031)(3×108)\Rightarrow {{\lambda }_{de-Broglie}}=\sqrt{\dfrac{(6.626\times {{10}^{-34}})(10\times {{10}^{-10}})}{2(9.19\times {{10}^{-31}})(3\times {{10}^{8}})}}
λdeBroglie=0.3\Rightarrow {{\lambda }_{de-Broglie}}=0.3 Å

So, the correct answer is - (A).

Note: The working principle of the Coolidge tube is as follows:
A heated filament emits electrons in the vacuum tube, which we call the Coolidge tube. The electrons are accelerated with the help of an electric field between the filament and the target. These electrons are absorbed in the target and it emits X-Ray. The energy of the electrons are transferred to the X-Ray. That is why we compared the kinetic energy with the energy of the photons.