Calculating Planar Density for FCC {100}, {110}, {111}

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Discussion Overview

The discussion centers around calculating the planar density for different crystallographic planes ({100}, {110}, {111}, and {200}) in face-centered cubic (FCC) structures. It includes theoretical considerations and specific calculations related to atomic arrangements and densities in these planes.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Homework-related

Main Points Raised

  • One participant outlines the calculation for the {100} plane, stating it has 2 atoms per unit area based on the arrangement of atoms in the square plane.
  • Another participant describes the {110} plane, noting it has 1 atom per unit area, derived from the diagonal cut through the unit cell.
  • The calculation for the {111} plane is presented, with a total of 2 atoms per unit area, based on the triangular arrangement of atoms and the area of the triangle.
  • A participant inquires about the planar density for the (200) plane, prompting a question about visualizing the plane and the number of atoms it intersects.
  • Another participant mentions the (110) plane in the silicon diamond structure, indicating it includes 4 atoms and provides a specific density value.
  • A request is made for information on the number of surface atoms in a cube of FCC gold atoms, given specific atomic radius and cube length parameters.

Areas of Agreement / Disagreement

Participants present various calculations and inquiries, but there is no consensus on the planar density for the (200) plane or the specifics of the gold atom cube, indicating multiple competing views and unresolved questions.

Contextual Notes

Some calculations depend on assumptions about atomic arrangements and definitions of planes, which may not be universally agreed upon. The discussion does not resolve the mathematical steps or the implications of the different atomic arrangements.

Who May Find This Useful

This discussion may be useful for students and researchers interested in crystallography, materials science, and solid-state physics, particularly those studying FCC structures and planar densities.

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HOw od you calculate the planar density for {100}, {110}, {111} for FCC?
 
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Lets start with [100] plane which is a plane parallel to a face of the unit cell and it looks like a square. There is one atom at the center of the square and a total of 4*1/4 atoms on the coners of the plane. Hence there are a net total of 2 atoms inside the square. Now the area is just the area of the square which is a^2 (where a is the lattice constant). So the suface density is 2/a^2 atoms per unit area.

The [110] plane is the plane which cuts the unit cell diagonally in half and it looks like a square. There are just 4*1/4 atoms on the corners of the square - a net total of 1 atom inside the square. The length of one of the sides of the plane is a*sqrt(2). Hence the surface density is 1/(a*sqrt(2)) atoms per unit area.

The [111] plane is a plane that touches the three far corners of the unit cell and it looks like a triangle. There are then a total 1/6*3 atoms that make up the vertices of the triangle and there are a total of 1/2*3 atoms that make up the three edges of the triangle. So you have a net total of 2 atoms inside the triangle. The triangle is an equlilateral triangle with a leg of length a*sqrt(2). The area of an equilateral triangle is s^2*sqrt(3)/4 which then gives us a^2*sqrt(3)/2 as the area of that trinagle. Hence the density is 2/(a^2*sqrt(3)/2) atoms per unit area.
 
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Thank you very much for explaning that very clearly!
 
FCC for (2 0 0)

how do you find the planar density for the (2 0 0) FCC unit cell
 
First of all, can you picture the (200) plane in the FCC unit cell? Secondly, across how many atoms does it cut?
 
Just in case, in Si diamond structure, the plane (110) includes a total of 4 atoms, which increases the density to 9.6*10^(14).
 
I need to know the number at surface atoms in a cube of a FCC lattice of gold atoms knowing that R= 144.2 pm with respect to L( length of the cube) and a ( length of a unit cell )
 

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