Sodium metal crystallizes in bcc lattice with cell edge . The radius of sodium atom will be-
(B). For bcc,
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Sodium metal crystallizes in bcc lattice with cell edge . The radius of sodium atom will be-
(B). For bcc,
A metallic element exists as cubic lattice. Each edge of the unit cell is 2.88 . The density of the metal is 7.20 g . How many unit cell will be present in 100 g of the metal -
(B). The volume of the unit cell
The volume of 100 g of the metal =
Number of unit cells in this volume
An alloy of copper, silver and gold is found to have copper constituting the ccp lattice. If silver atoms occupy the edge centres and gold is present at body centre, the alloy has a formula-
(C). ccp lattice = fcc lattice
(Each edge centered atom is contributed by 4 unit cell)
Frenkel defect is not found in the halides of alkali metals because alkali metals have
Frenkel defect is not found in pure alkali metal halides. This is because of the larger size of the cations of the alkali metals, due to the large size the cations cannot fit into the interstitial sites.
Iodine crystal are-
(C). Molecular solids are the substances having molecules as constituent units having interparticle forces such as Vander Waal’s forces or hydrogen bonds.
8 : 8 co-ordination of CsCl is found to change into 6 : 6
co-ordination on:
High temperature changes 8 : 8 co-ordination to 6 : 6 whereas high pressure changes 6 : 6
co-ordination to 8 : 8.
At room temperature, sodium crystallises in a body centred cubic cell with a 4.24 . The theoretical density of sodium is- (Atomic mass of sodium=23.0 g )
(C). The value of Z for a bcc unit cell is 2.
Volume V=
Which is amorphous solids-
(D). Amorphous solids neither have ordered arrangement (i.e. no definite shape) nor have sharp melting point like cyrstals, but when heated, they become soft until they assume the properties usually related to liquid. It is therefore they are regarded as super cooled liquids.
The unit cell dimensions of a cubic lattice (edges a, b, c and the angles between them, ) are
(A). It is based on the definition of the cubic lattice.
The most efficient packing of similar spheres is obtained in
(C). The hexagonal close packing and the face-centred cubic system have the closest packing as their packing efficiency is 74 %.
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