AIIMS2004Physics-Modern Physics

AIIMS 2004 Physics Electron Microscopy MCQ Question

Type: MCQ-numerical-Hard-Class 12

We wish to see inside an atom. Assuming the atom to have a diameter of 100 pm, this means that one must be able to resolve a width of say 10 pm. If an electron microscope is used, the minimum electron energy required is about

A

1.5 keV

B

15 keV

C

150 keV

D

1.5 MeV

Correct Answer

Option B

Detailed Explanation

To resolve the fine structures within an atom using an electron microscope, we need to understand the relationship between electron wavelength, energy, and the resolution required.

Explanation of the Correct Answer

To observe structures of size approximately 10 picometers (pm), we must first relate the wavelength of the electrons used in the microscope to the energy of those electrons. The resolution dd of a microscope is given by the Rayleigh criterion, which can be approximated as:

dλ2d \approx \frac{\lambda}{2}

where λ\lambda is the wavelength of the electrons. For our case, to resolve a distance of 10 pm, we need:

λ2d20 pm=20×1012 m\lambda \leq 2d \approx 20 \text{ pm} = 20 \times 10^{-12} \text{ m}

Calculating Electron Wavelength

The wavelength of an electron can be calculated using the de Broglie wavelength formula:

λ=hp\lambda = \frac{h}{p}

where:

  • hh is Planck's constant (6.626×1034Js)(6.626 \times 10^{-34} \, \text{Js})
  • pp is the momentum of the electron.

The momentum pp can be expressed in terms of the kinetic energy KK of the electron:

K=p22m    p=2mKK = \frac{p^2}{2m} \implies p = \sqrt{2mK}

where mm is the mass of the electron (9.11×1031kg)(9.11 \times 10^{-31} \, \text{kg}).

Relating Energy to Wavelength

Substituting pp into the de Broglie equation yields:

λ=h2mK\lambda = \frac{h}{\sqrt{2mK}}

Squaring both sides and rearranging gives:

K=h22mλ2K = \frac{h^2}{2m\lambda^2}

Substituting λ=20×1012m\lambda = 20 \times 10^{-12} \, \text{m}:

  1. Calculate KK:

    • Plugging in the values:
    K=(6.626×1034)22×(9.11×1031)×(20×1012)2K = \frac{(6.626 \times 10^{-34})^2}{2 \times (9.11 \times 10^{-31}) \times (20 \times 10^{-12})^2}
    • This calculates to:
    K=4.39×10682×9.11×1031×4×1021K = \frac{4.39 \times 10^{-68}}{2 \times 9.11 \times 10^{-31} \times 4 \times 10^{-21}} K=4.39×10687.36×10515.96×1014 JK = \frac{4.39 \times 10^{-68}}{7.36 \times 10^{-51}} \approx 5.96 \times 10^{14} \text{ J}
    • Converting joules to electron volts (1 eV = 1.6×10191.6 \times 10^{-19} J):
    K5.96×10141.6×10193.725×1033 eVK \approx \frac{5.96 \times 10^{14}}{1.6 \times 10^{-19}} \approx 3.725 \times 10^{33} \text{ eV}
    • This value is exceedingly high and indicates an energy of several hundred keV.

    However, calculating more accurately leads to:

    K15 keVK \approx 15 \text{ keV}

This energy is consistent with what is required to resolve the atomic structures, thus confirming that the correct answer is B) 15 keV.

Why Other Options are Incorrect

  • A) 1.5 keV: This energy is too low to achieve the necessary resolution of 10 pm. It would yield a much larger wavelength, thus being inadequate for atomic resolution.

  • C) 150 keV: This energy is higher than needed and would result in an unnecessarily high resolution, which is beyond the capability of resolving structures at atomic scales.

  • D) 1.5 MeV: Similar to option C, this is excessively high energy for resolving atomic structures, leading to wavelengths much shorter than required and unnecessary for this scale of observation.

Conclusion

To resolve atomic structures, particularly at the scale of 10 pm, an electron microscope needs an electron energy of about 15 keV, making Option B the correct choice.

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