Determine crystal lattice structure from powder XRD

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Homework Help Overview

The discussion revolves around analyzing powder XRD data to determine if a substance has a face-centered cubic (fcc) structure. Participants are provided with specific peak angles and relevant equations for calculating interplanar spacing and Miller indices.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • The original poster attempts to calculate sin theta and delta sin theta for various peaks but expresses uncertainty about how to proceed with the information gathered. They also mention the need for guidance on identifying the highest common factor in their calculations.
  • Another participant inquires about the formula for finding lattice parameters using d and 2theta values, as well as how to calculate Miller indices if the structure is known.
  • Subsequent posts outline steps for identifying peaks, calculating sin squared theta, and determining ratios to find Miller indices, suggesting a structured approach to the problem.

Discussion Status

Participants are actively sharing insights and methods for analyzing the XRD data. Some guidance has been offered regarding the identification of peaks and the calculation of ratios, but there is no explicit consensus on the best approach to take next. The discussion remains open with various interpretations being explored.

Contextual Notes

Participants note that the only example previously covered was for a primitive cubic structure, which may limit their understanding of the fcc structure. There is also mention of the need to find integer values for h, k, and l to confirm the lattice structure.

s_gunn
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Homework Statement



Using the powder XRD data below, show that the substance has a face centred cubic structure. (xray lamda = 0.154056 nm)

Peak No.------2(theta)
1 -------------38.06
2 -------------44.24
3 -------------64.34
4 -------------68.77
5 -------------73.07


Homework Equations



2dsin\theta = n\lambda

d = \frac{a}{\sqrt{N}}

\Delta sin\theta = \left(\frac{\lambda}{4a^{2}}\right)N_{2} - N_{1}

N= h^{2}+k^{2}+l^{2}

The Attempt at a Solution



I've worked out sin theta for each sin theta squared and delta sin theta:

Peak------2(theta)------sin theta----sin squared theta---delta sin squared theta
1-----------38.06-------0.32606-------0.10632------------
2-----------44.24-------0.37655-------0.14179------------0.03547
3-----------64.34-------0.53243-------0.28349------------0.1417
4-----------68.77-------0.56475-------0.31894------------0.03545
5-----------73.07-------0.59531-------0.35440------------0.03549

The only example we've covered is with a primitive cubic structure which I almost knew what I was doing(!) and the only advice that the lecturer gave was to "look for the highest common factor of values in the list delta sin squared theta to find \frac{\lambda}{4a^{2}}

I obviously noted that the difference between peak 2 and 3 was the same value as Peak 2 but what I'm meant to do with that information I'm not so sure about!?

I know that a fcc structure only has N values of 3,4,8,11 etc but really could do with some advice as where to go from here!?
 
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Any help at all would be appreciated! I've spent ages searching for answers and the people that I've spolen to at uni have no clue either so i'd love to be able to pass on the knowledge!
 
s_gunn said:

Homework Statement



Using the powder XRD data below, show that the substance has a face centred cubic structure. (xray lamda = 0.154056 nm)

Peak No.------2(theta)
1 -------------38.06
2 -------------44.24
3 -------------64.34
4 -------------68.77
5 -------------73.07


Homework Equations



2dsin\theta = n\lambda

d = \frac{a}{\sqrt{N}}

\Delta sin\theta = \left(\frac{\lambda}{4a^{2}}\right)N_{2} - N_{1}

N= h^{2}+k^{2}+l^{2}

The Attempt at a Solution



I've worked out sin theta for each sin theta squared and delta sin theta:

Peak------2(theta)------sin theta----sin squared theta---delta sin squared theta
1-----------38.06-------0.32606-------0.10632------------
2-----------44.24-------0.37655-------0.14179------------0.03547
3-----------64.34-------0.53243-------0.28349------------0.1417
4-----------68.77-------0.56475-------0.31894------------0.03545
5-----------73.07-------0.59531-------0.35440------------0.03549

The only example we've covered is with a primitive cubic structure which I almost knew what I was doing(!) and the only advice that the lecturer gave was to "look for the highest common factor of values in the list delta sin squared theta to find \frac{\lambda}{4a^{2}}

I obviously noted that the difference between peak 2 and 3 was the same value as Peak 2 but what I'm meant to do with that information I'm not so sure about!?

I know that a fcc structure only has N values of 3,4,8,11 etc but really could do with some advice as where to go from here!?
hai
i want to know what is the formula for finding a,b,c using 'd' and 2theta values. also if the structure is known how to calculate miller indices for the corresponding peaks
 
For Cubic crystal finding hkl (miller indices) is easy note that peak in xrd is a importent factor
(1) Identify the peaks.
(2) Determine sin2\theta
(3) Calculate the ratio sin2\theta/ sin2\thetamin and multiply by the appropriate integers.
(4) Select the result from (3) that yields h2 + k2 + l2 as an integer.
(5) Compare results with the sequences of h2 + k2 + l2 values to identify the Bravais lattice.
(6) Calculate lattice parameters.
 
Identify the peaks and their proper 2 values. Eight peaks for this pattern.
1.jpg

Determine sin2
2.jpg

Calculate the ratio sin2/ sin2min and multiply by the appropriate integers.
3.jpg
 
Select the result from (3) that yields h2 + k2 + l2 as a series of integers.
4.jpg

Compare results with the sequences of h2 + k2 + l2 values to identify the Bravais lattice.
5.jpg
 

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