Determination of Precise Lattice Parameter of FCC and BCC phases using X-ray diffraction

Errors in measurement of interplanar spacing d and lattice parameter(s) a using modern diffractometers can occur due to :

  • Misalignment of the instrument
  • Absorption of X-Rays by the specimen
  • Displacement of the specimen from the diffractometer axis must be minimized (observational error)
  • Vertical divergence of the incident beam
  • Use of a flat specimen instead of a curved one to correspond to the diffractometer circle


Figure 1: X-Ray Diffractogram for an FCC material

Observational error :

  • For a cubic material :

Where the d-spacing is measured from Bragg’s law :

Here, n = 1 which is the first order of diffraction and λ = 1.5406 Å for Cu-Kα radiation.

  • Precision in measurement of a or d depends on precision in derivation of sinθ.

Figure 2: Error in the measurement of sin θ decreases as the value of θ increases

  • Take partial derivative of the Bragg equation :



  • For a cubic system :



  • The term ∆a⁄a (or ∆d⁄d) is the fractional error in a (or d) caused by a given error in θ. The fractional error approaches zero as θ approaches 90°.

  • Values of a will approach the true value as we approach 2θ = 180° (i.e., θ = 90°). We can’t measure a value at 2θ = 180°. We must plot measured values and extrapolate to 2θ = 180° versus some function of θ.

Absorption Error :

  • For a cubic crystal with a lattice parameter a, a Nelson-Riley extrapolation function is used :


Steps:

  1. From the diffractogram, we will obtain the values of all the parameters, viz., 2θ, θ, θ in radians, sin θ, sin2θ, cos2 θ
  2. Calculate the (h k l) planes for each peak using equation (1)
  3. Calculate the corresponding values of a in each case

Procedure of the experiment:
• For F(θ) vs a and perform a linear fitting of the data obtained.
• The line of best fit which will be obtained will be further extrapolated to F(θ) = 0 and the y-intercept will give us the precise lattice parameter for the particular material.

FCC: The above procedure yields a precise lattice parameter for FCC to be 3.631±0.003 Å.