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Question: \(CsBr\) crystallizes in a body-centered cubic lattice. The unit cell length is 436.6 pm. Given that...

CsBrCsBr crystallizes in a body-centered cubic lattice. The unit cell length is 436.6 pm. Given that the atomic mass of Cs=133Cs = 133 and that of Br=80Br = 80 amu and Avogadro number being 6.02×1023mol16.02 \times {10^{23}}mo{l^{ - 1}} , the density of CsBrCsBr is:
A.42.5g/cm342.5g/c{m^3}
B.0.425g/cm30.425g/c{m^3}
C.8.5g/cm38.5g/c{m^3}
D.4.25g/cm34.25g/c{m^3}

Explanation

Solution

Lattice structures are topologically ordered, three-dimensional open-celled structures composed of one or more repeating unit cells [2,3]. These cells are defined by the dimensions and connectivity of their constituent strut elements, which are connected at specific nodes.This question can be solved by using the formula ρ=Z×Ma3×NA\rho = \dfrac{{Z \times M}}{{{a^3} \times {N_A}}} where Z,M,a,NA,ρZ,M,a,{N_A},\rho are number of atoms, Mass of consisting atom/molecule, edge length/unit cell length, Avogadro number and density respectively.
Value of ZZ for BCC is 2.

Complete step by step answer:
Let’s deduce the expression ρ=Z×Ma3×NA\rho = \dfrac{{Z \times M}}{{{a^3} \times {N_A}}} from the very beginning.
We know density of unit cell =mass of unit cell/volume of unit cell
Mass of a unit cell = number of atoms in unit cell ×\times mass of single atom = Z×m(1)Z \times m - - - (1) where, Z,mZ,m are number of atoms and mass of single atom/molecule in unit cell. We can find the mass of a single atom/molecular by dividing atomic mass MM by Avogadro’s Number NA{N_A}.
So, m=MNA(2)m = \dfrac{M}{{{N_A}}} - - - (2)
From equation (1) & (2)
Mass of unit cell =Z×MNA(3) = \dfrac{{Z \times M}}{{{N_A}}} - - - (3)
Now we can write density of unit cell ρ=Z×MV×NA(4)\rho = \dfrac{{Z \times M}}{{V \times {N_A}}} - - - (4) where VV is volume of unit cell. As we also know that the volume of a cube is cube of its edge length, consider an edge length aa , so volume V=a3V = {a^3}.
So, equation (4) can be rewritten as ρ=Z×Ma3×NA(5)\rho = \dfrac{{Z \times M}}{{{a^3} \times {N_A}}} - - - (5) .


Now, Let’s calculate the number of atoms in the unit cell that is BCC.
Atoms at the corners are 8 and contribution of each corner atom is 1/8 and atom at centre is one and it is not shared with any other cell.
So, Z=8×18+1=2Z = 8 \times \dfrac{1}{8} + 1 = 2
As per question a=436.6pm=436.6×1010cm,M=133+80=213g/mola = 436.6pm = 436.6 \times {10^{ - 10}}cm,M = 133 + 80 = 213g/mol
Putting all values in equation (5) we get,
ρ=2×213g/mol(436.6×1010cm)3×6.02×1023mol1\rho = \dfrac{{2 \times 213g/mol}}{{{{(436.6 \times {{10}^{ - 10}}cm)}^3} \times 6.02 \times {{10}^{23}}mo{l^{ - 1}}}}
ρ=8.5g/cm3\Rightarrow \rho = 8.5g/c{m^3}

Note:
While deducing the formula ρ=Z×Ma3×NA\rho = \dfrac{{Z \times M}}{{{a^3} \times {N_A}}} we used mm and MM , both are different. mm is mass of single atom MM is atomic mass in amu. So, when we take MM atomic mass in grams, according to concept of moles, we get mass of 1 mole of atoms that are equal in Avogadro’s number =6.02×1023mol1 = 6.02 \times {10^{23}}mo{l^{ - 1}} . So, in order to find the mass of a single atom m=MNAm = \dfrac{M}{{{N_A}}} .