Respuesta :
Answer : The crystal structure of Rhodium is, FCC (Z=4)
Explanation :
Nearest neighbor distance, r = 0.1345nm=1.345\times 10^{-8}cm (1nm=10^{-7}cm)
Atomic mass of rhodium (M) = 102.9 g/mole
Avogadro's number [tex](N_{A})=6.022\times 10^{23} mol^{-1}[/tex]
First we have to calculate the cubing of edge length of unit cell for BCC and FCC crystal lattice.
For BCC lattice : [tex]a^3=(\frac{4r}{\sqrt{3}})^3=(\frac{4\times 1.345\times 10^{-8}cm}{\sqrt{3}})^3=3.04\times 10^{-23}cm^3[/tex]
For FCC lattice : [tex]a^3=(\sqrt{8}r)^3=(\sqrt{8}\times 1.345\times 10^{-8}cm)^3=5.50\times 10^{-23}cm^3[/tex]
Now we have to calculate the density of unit cell for BCC and FCC crystal lattice.
Formula used :
[tex]\rho=\frac{Z\times M}{N_{A}\times a^{3}}[/tex] .............(1)
where,
[tex]\rho[/tex] = density
Z = number of atom in unit cell (for BCC = 2, for FCC = 4)
M = atomic mass
[tex](N_{A})[/tex] = Avogadro's number
a = edge length of unit cell
Now put all the values in above formula (1), we get
[tex]\rho=\frac{2\times (102.9g/mol)}{(6.022\times 10^{23}mol^{-1}) \times (3.04\times 10^{-23}Cm^3)}=11.24g/Cm^{3}[/tex]
[tex]\rho=\frac{4\times (102.9g/mol)}{(6.022\times 10^{23}mol^{-1}) \times (5.50\times 10^{-23}Cm^3)}=12.42g/Cm^{3}[/tex]
From this information we conclude that, the given density is approximately equal to the density of FCC unit lattice.
So, the crystal structure of Rhodium is, FCC (Z=4)
The Rhodium atom has FCC crystal structure since the density calculation matches the given density value.
The given parameters;
- radius of the Rhodium atom, r = 0.1345 nm = 0.1345 x 10⁻⁹ m.
- density of the atom, ρ = 12.41 g/cm³
The edge length of unit cell for BCC and FCC crystal lattice is calculated as follows;
[tex]BCC: \ \ \ a^3 = (\frac{4r}{\sqrt{3} } )^3 \ \ = \ \ (\frac{4\times 0.1345 \times 10^{-7} }{\sqrt{3} } )^3 \ =2.996 \times 10^{-23} \ cm^3 \\\\FCC : \ \ \ a^3 \ = (\sqrt{8} \ r)^3 \ \ = (\sqrt{8} \times 0.1345\times 10^{-7} )^3= 5.5 \times 10^{-23} \ cm^3[/tex]
The density of unit cell for each crystal lattice is calculated as follows;
[tex]\rho = \frac{Z \times M}{a^3 \times N_A}[/tex]
where;
- ρ is the density
- Z is number of atom in unit cell
- M is the atomic mass = 102.9 g/mol
- [tex]N_A[/tex] is the Avogadro's number
- a is the edge length
The density of unit cell for BCC crystal lattice (Z = 2);
[tex]\rho = \frac{Z \times M}{a^3 \times N_A}\\\\\rho = \frac{2 \times 102.9}{2.996 \times 10^{-23} \times 6.02 \times 10^{23}}\\\\\rho = 11.41 \ g/cm^3[/tex]
The density of unit cell for FCC crystal lattice (Z = 4);
[tex]\rho = \frac{Z \times M}{a^3 \times N_A}\\\\\rho = \frac{4 \times 102.9}{5.5 \times 10^{-23} \times 6.02 \times 10^{23}}\\\\\rho = 12.43 \ g/cm^3[/tex]
Thus, we can conclude that the Rhodium atom has FCC crystal structure since the density calculation matches the given density value.
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