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Solid State Test - 25

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Solid State Test - 25
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  • Question 1
    1 / -0
    If a is the lattice parameter, the volume of an fcc crystal having $$N$$ atoms is :
  • Question 2
    1 / -0
    The physical dimension of unit cells in a crystal lattice:
    Solution
    Lattice parameter which refers to the physical dimension of unit cells in a crystal lattice. Lattices in three dimensions generally have three lattice constants, referred to as a, b, and c.
  • Question 3
    1 / -0
    If A is the molecular mass of an element, a is the edge length and $$N$$ is the Avogadro's number, then the density for simple cubic lattice is :
    Solution
    $$\text{Density}$$ $$=$$ $$\dfrac{\text{Number of molecules present in lattice (Z)} \times \text{Mass of each molecule (m)}}{\text{Volume of lattice (V)}}$$

    In simple lattice, each lattice has one molecule and mass of each molecule is $$\dfrac{\text{Molar mass (A)}}{\text{Avogadro's number (N)}}$$

    For simple cubic lattice, $$Z = 1$$

    Hence, $$\text{density} = \dfrac{Z\times A}{N\times a^{3}}=\dfrac{A}{N\times a^3}$$, where $$a$$ is the edge length.
  • Question 4
    1 / -0
    The lattices of Na and Al are bcc and fcc respectively. Presuming them to be closed packed, their packing fractions are, respectively :
    Solution
    Packing fraction is known as the fraction of volume occupied by the constituent particles in crystal structure.
    GIVEN
    Lattices of $$Na$$ is Body centred cubic $$BCC$$
    Lattices of $$Al$$ is Face centred cubic $$FCC$$

    SOLUTION 

    $$Packing\hspace{0.1cm}fraction$$ =$$\dfrac{N_{atom}\hspace{0.1cm}V_{atom}}{V_{unit\hspace{0.05cm}cell}}$$

    Packing fraction of BCC ($$Na$$)

    Number of atoms ($$N_{atom}$$) = $$2$$
    Volume of atoms ($$V_{atom}$$) = $$\dfrac{4}{3}$$$$\pi$$$$r^{2}$$
    Volume of unit cell ($$V_{unit\hspace{0.05cm}cell}$$) = $$($$$$\dfrac{4r}{\sqrt3}$$$$)^{3}$$

    Particle fraction $$_{BCC}$$ =$$\dfrac{N_{atom}\hspace{0.1cm}V_{atom}}{V_{unit\hspace{0.05cm}cell}}$$

                                      = $$\dfrac{2\times\dfrac{4}{3}\pi r^{2}}{(\dfrac{4r}{\sqrt3})^{3}}$$
                                     
                                       = $$\dfrac{\pi \sqrt{3}}{8}$$

    $$\mathbf Particle fraction $$$$_{BCC}$$$$\cong$$ $$\mathbf 0.6802$$

    Packing fraction of FCC ($$Al$$)

    Number of atoms ($$N_{atom}$$) = $$4$$
    Volume of atoms ($$V_{atom}$$) = $$\dfrac{4}{3}$$$$\pi$$$$r^{30}$$
    Volume of unit cell ($$V_{unit\hspace{0.05cm}cell}$$) = $$($$$$\dfrac{4r}{\sqrt2}$$$$)^{3}$$

    Particle fraction $$_{FCC}$$ = $$\dfrac{4\times\dfrac{4}{3}\pi r^{3}}{(\dfrac{4r}{\sqrt2})^{3}}$$

                                        =$$\dfrac{\pi \sqrt{2}}{12}$$

    Particle fraction $$_{FCC}$$ = $$0.74$$        

    The particle fractions for $$Na$$ and $$Al$$ are $$0.68$$ and $$0.74$$.

    The correct option : B



  • Question 5
    1 / -0
    The density of solid argon (atomic mass $$=40$$ amu) is $$1.68$$ g/ml at $$40$$ K. If the argon atom is assumed to be a sphere of radius $${1.50 \times 10^{-8}}$$ cm, then the percentage of solid Ar which is space will be: 
    [use $$N_A=6\times 10^{23}$$]
    Solution
    As we know, density $$=1.68 = \dfrac{nM}{VN_A}=\dfrac{n\times 40}{V\times6\times 10^{23}}$$
    $$\implies V = 39.53 \times 10^{-24}\ n$$
    The radius of argon is $$1.5 \times 10^{-8}$$ cm and so, the empty space is $$\left (1-\dfrac{4}{3} \right ) \times n\times \pi r^3 \times \dfrac{100}{V} = 64.3\%$$
  • Question 6
    1 / -0
    An atomic solid crystallizes in a body centre cubic lattice and the inner surface of the atoms at the adjacent corner are separated by $$60.3$$ pm. If the atomic weight of A is $$48$$, then the density of the solid is nearly:
    Solution
    According to the given diagram,

    The separation between the inner surface of the atoms at adjacent corners is given by-
    $$a - 2r =60.3$$

    For BCC,

    $$\sqrt3 a = 4r$$

    So, density $$= \dfrac{nM}{VN_A}$$$$ = \dfrac{2 \times 48 \times 10^{30}}{(463.8)^3 \times 6.023 \times 10^{23}} = 1.7$$ $$g/cc$$

  • Question 7
    1 / -0
    The packing efficiency of a simple cubic crystal with an interstitial atom exactly fitting at the body center is:
    Solution
    For a simple cubic, $$ a=2r $$
    Therefore, the radius of the interstitial atom exactly fitting at the centre of the cube is $$R=  \dfrac{1}{2} \times (a\sqrt 3 -2r) $$ 

    $$R= \dfrac{1}{2} \times (a\sqrt 3 -a) $$

    $$R= 0.366a $$

    Packing fraction $$ =  \dfrac{\text{volume occupied by spheres}}{a^3} $$

    Packing fraction $$ =  \dfrac{ (\dfrac{1}{8} \times 8 \times \dfrac{4 \pi r^3}{3}) + ( 1 \times \dfrac{4 \pi R^3}{3} ) }{a^3} $$ 

    Packing fraction$$ =  \dfrac{4\pi ({(\dfrac{a}{2})}^3 + (0.366a)^3)}{3a^3} $$

    Packing fraction $$= 0.7285$$.
  • Question 8
    1 / -0
    Sodium (atomic mass $$=23$$ amu) crystallizes in a bcc arrangement with the interfacial separation between the atoms at the edge $$53.6$$ pm. The density (in g cm$$^{-3}$$) of sodium crystal is:
    Solution
    According to given condition,
    $$ {a-2R} = 53.6$$ pm
    $$ a(1 - {2(\sqrt 3 )\over 4}) = 53.6  $$ pm

    $$\implies a=400$$ pm
    So, density $$= \dfrac{nM}{VN_A}$$$$ = \dfrac{2 \times 23 }{(400)^3 \times 6.023 \times 10^{23}\times 10^{-24}} = 1.19$$ g/cc
  • Question 9
    1 / -0
    If A is the molecular mass of an element, a is the edge length and $$N$$ is the Avogadro's number, then the density for face-centered cubic lattice is :
    Solution
    $$\text{Density}$$ $$=$$ $$\dfrac{\text{Number of molecules present in lattice (Z)} \times \text{Mass of each molecule (m)}}{\text{Volume of lattice (V)}}$$

    In face-centered cubic lattice, each lattice has four molecules and mass of each molecule is $$\dfrac{\text{Molar mass (A)}}{\text{Avogadro's number (N)}}$$

    Hence, $$\text{Density} = \dfrac{Z\times A}{N\times a^{3}}=\dfrac{4\times A}{N\times a^3}$$, where $$a$$ is the edge length.
  • Question 10
    1 / -0

    Directions For Questions

    Packing fraction of a unit cell is defined as the fraction of the total volume of the unit cell occupied by the atom(s).$$\displaystyle \text{Packing fraction (P.F)} = \dfrac{\text{Volume of the atom (s) present in a unit cell}}{\text{Volume of unit cell}}$$                                          $$=\dfrac {Z \times \dfrac{4}{3} \pi r^{3}}{a^{3}}$$ Percentage of empty space $$=100-\text{P.F}\times 100$$ where $$Z$$  is the effective number of atoms in a cube, $$r$$ is the radius of an atom and $$a$$ is the edge length of the cube.

    ...view full instructions

    Packing fraction in face-centered cubic unit cell is :
    Solution
    Packing efficiency (P.E.) $$=\dfrac {n\times\dfrac 43 \pi r^3}{V} \times 100$$
    For a FCC lattice, $$n=4$$
    Therefore, P.E. $$=\dfrac{4\times \dfrac 43 \times {(\dfrac {a}{2\sqrt 2}}^3)}{a^3} =\dfrac {\pi}{3\sqrt2} \times 100=74\%$$
    Hence. in FCC, $$74\%$$ of the total volume is occupied by atoms.
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