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Question

A peak in the X-ray diffraction pattern is observed at $2\theta = 78^\circ$, corresponding to {311} planes of an fcc metal, when the incident beam has a wavelength of 0.154 nm. The lattice parameter of the metal is approximately

The correct answer is
0.4 nm

Calculating FCC Lattice Parameter using XRD Data

This problem requires calculating the lattice parameter ('a') of a face-centered cubic (fcc) metal using information from an X-ray diffraction (XRD) experiment. We can use Bragg's Law and the formula for interplanar spacing in cubic crystals.

Applying Bragg's Law and Interplanar Spacing Formula

  1. Identify Given Parameters:
    • Diffraction angle: $2\theta = 78^\circ$
    • Plane indices: {311}
    • Wavelength: $\lambda = 0.154$ nm
    • Crystal structure: fcc
  2. Calculate the angle $\theta$:

    $\theta = \frac{2\theta}{2} = \frac{78^\circ}{2} = 39^\circ$

  3. Determine the sum of squares for the plane indices:

    For {311} planes in an fcc lattice, the indices are $h=3, k=1, l=1$. The sum of squares is:

    $h^2 + k^2 + l^2 = 3^2 + 1^2 + 1^2 = 9 + 1 + 1 = 11$

  4. Use Bragg's Law to find interplanar spacing ($d$):

    Bragg's Law is $n\lambda = 2d \sin\theta$. Assuming the first-order peak ($n=1$):

    $\lambda = 2d \sin\theta$

    Rearranging for $d$:

    $d = \frac{\lambda}{2 \sin\theta}$

    Substitute the values:

    $d = \frac{0.154 \text{ nm}}{2 \times \sin(39^\circ)}$

    Using $\sin(39^\circ) \approx 0.6293$:

    $d \approx \frac{0.154 \text{ nm}}{2 \times 0.6293} \approx \frac{0.154}{1.2586} \approx 0.12236$ nm

  5. Relate interplanar spacing to lattice parameter for fcc:

    The formula for interplanar spacing ($d_{hkl}$) in a cubic system is:

    $d_{hkl} = \frac{a}{\sqrt{h^2 + k^2 + l^2}}$

    Rearranging to solve for the lattice parameter 'a':

    $a = d_{hkl} \times \sqrt{h^2 + k^2 + l^2}$

  6. Calculate the lattice parameter ('a'):

    Substitute the calculated $d$ and the sum of squares:

    $a \approx 0.12236 \text{ nm} \times \sqrt{11}$

    Using $\sqrt{11} \approx 3.3166$:

    $a \approx 0.12236 \text{ nm} \times 3.3166 \approx 0.4058$ nm

  7. Conclusion:

    The calculated lattice parameter is approximately 0.4058 nm, which is closest to the option 0.4 nm.

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Important Questions from Crystal Structure Density Atomic Packing Factor

  1. Match the crystal systems in Column I with the corresponding axial lengths (a, b, c) and interaxial angles ($\alpha$, $\beta$, $\gamma$) provided in Column II
    Column IColumn II
    (P) Tetragonal(1) $a \neq b \neq c$, $\alpha = \beta = \gamma = 90^\circ$
    (Q) Rhombohedral(2) $a = b \neq c$, $\alpha = \beta = \gamma = 90^\circ$
    (R) Orthorhombic(3) $a \neq b \neq c$, $\alpha = \gamma = 90^\circ \neq \beta$
    (S) Monoclinic(4) $a = b = c$, $\alpha = \beta = \gamma \neq 90^\circ$
  2. The coordination number for an octahedral site in pure copper is __________.
  3. The lattice parameter of face-centered cubic iron ($\gamma$-Fe) is 0.3571 nm. The radius (in nm) of the octahedral void in $\gamma$-Fe is _______________

  4. For a bcc metal the ratio of the surface energy per unit area of the (100) plane to that of the (110) plane is ________
  5. Pure iron transforms from body centered cubic (BCC) to face centered cubic (FCC) crystal structure at $912 \text{ °C}$. If the lattice parameter of the BCC phase is $0.293 \text{ nm}$ and that of the FCC phase is $0.363 \text{ nm}$, the associated volume change is ________ (in % to one decimal place)
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