Face-centered cubic lattice.

In summary, an element crystallizes in a face-centered cubic lattice with a basis group of two atoms at [000] and [1/4 1/4 1/4]. The lattice constant is 3.55 x 10^-10 m, and the average volume per atom is 11.8 x 10^-30 m³. The Attempt at a Solution states that the number of atoms per m² is 74%.
  • #1
hhhmortal
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Homework Statement



An element crystallises in a face-centered cubic lattice with a basis group of two atoms at [000] and [1/4 1/4 1/4]. The lattice constant is 3.55 x 10^-10 m

(Q1) How many nearest and second-nearest neighbours does each atom have?

(Q2) Calculate the average volume per atom

Homework Equations





The Attempt at a Solution



Ok, well I tried doing (Q2) I can't make sense of (Q1) though.

For (Q2) I used equation :

(4/3)(pi)(r²) = volume of atom

and r = {√3}/4 x lattice constant


But I don't think this is the case since I want the average volume per atom?

Thanks.
 
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  • #2
^Bump
 
  • #3
Any help at all? After reading some articles, I still can't work out this question.
 
  • #4
Do you know the meaning of "nearest neighbor" and "second nearest neighbor"?

hhhmortal said:
and r = {√3}/4 x lattice constant
Why do you think this is true?

Try to do it the other way around. What is the volume of a cell? How many atoms are there per cell? Answering the second question may be a bit tricky.
 
  • #5
I don't understand what "nearest neighbours and second nearest neighbours" is, especially for this fcc.

And I think that comes from the fact that the length of the diagonal is √3. and a line from one corner to the center corner passes through 4r. so

a = 4r / √3

Are there 4 atoms in this FCC? 3 from the face centered atoms and 1 from the corners.

I calculated the volume of cell to be: a³ = (3.55 x 10^-10)³


But how could I work out average volume of atom?
 
  • #6
hhhmortal said:
I don't understand what "nearest neighbours and second nearest neighbours" is, especially for this fcc.
For a given point, what is the closest possible other point? That other point is a nearest neighbor. There may be more than one nearest neighbor. For example, for a simple cubic, every atom has six nearest neighbors. Can you see why? For the second nearest neighbors, you simply form a sphere, whose radius is the distance to the centers of the nearest neighbors, centered on the atom of consideration, and then you start looking outside that sphere for the centers of atoms that are closest to it. If I'm figuring correctly, each atom of a simple cubic has eight second nearest neighbors.

I suggest to draw a picture, but be careful when considering the consequence of 2-D to 3-D.

Unfortunately, I don't remember if you must count atoms or lattice sites. I will try to find the answer to this and get back to you.



hhhmortal said:
... a line from one corner to the center corner passes through 4r.
It's been a while for me, but isn't that for a BCC?



hhhmortal said:
Are there 4 atoms in this FCC? 3 from the face centered atoms and 1 from the corners.
Maybe you know how to do this better than me. I just weight each corner as 1/8 of a lattic site (b/c corners are shared with 8 cells) and each face-centered site as 1/2 (b/c faces are shared with 2 cells). Then, there are 8 corners and 6 faces. So, I get

1/8 x 8 + 1/2 x 6 = 4

Of course, then you also need to consider how many atoms there are per lattice site.



hhhmortal said:
I calculated the volume of cell to be: a³ = (3.55 x 10^-10)³
I'll take your word for it.



hhhmortal said:
But how could I work out average volume of atom?
If, on average, N atoms occupy a volume of V, then 1 atom, on average, occupies a volume of ...
 
  • #7
Ok well I got it!

From your help I was able to assume that nearest neighbours would be 4 and then second nearest 12 I believe right?

And then you were right in saying that its not 4r, in actual fact its 2√2r

So then I was able to calculate the average volume of an atom to be:

(3.55 x 10^-10)³ / 4 = 11.8 x 10^-30 m³

I'm pretty sure this is the correct value.

I was also able to calculate the packing factor to be 74%.But then I have a last question which is:

What is the number density of atoms (number per m²) on the (1 1 1) planes:

I tried working something out but I am not sure on it, any help for this ?

Thanks!
 

1. What is a face-centered cubic lattice?

A face-centered cubic lattice is a type of crystal lattice structure found in many metallic elements and compounds. It is characterized by a repeating pattern of atoms or ions arranged in a cubic shape, with additional atoms or ions located at the center of each face of the cube.

2. What is the significance of the face-centered cubic lattice?

The face-centered cubic lattice is one of the most common and stable lattice structures found in nature. It has a high packing density, which makes it efficient for storing and transferring energy. It also has important applications in materials science and engineering, as it can affect the properties and behaviors of materials.

3. How is the face-centered cubic lattice different from other lattice structures?

The face-centered cubic lattice differs from other lattice structures, such as the simple cubic lattice and the body-centered cubic lattice, in the arrangement of its atoms. While the simple cubic lattice has atoms only at the corners of the cube and the body-centered cubic lattice has an additional atom at the center of the cube, the face-centered cubic lattice has atoms both at the corners and at the center of each face of the cube.

4. What are some examples of materials with a face-centered cubic lattice?

Some common materials with a face-centered cubic lattice include aluminum, copper, silver, gold, and lead. Many metallic alloys, such as steel, also have a face-centered cubic lattice structure.

5. How does the face-centered cubic lattice affect the properties of materials?

The face-centered cubic lattice can affect various properties of materials, such as their strength, ductility, and electrical conductivity. The arrangement of atoms in this lattice can also influence the behavior of dislocations, which are defects in the crystal structure that can affect the mechanical properties of materials.

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