1.
Atomic Radius:
It is defined as the distance from the centre of the nucleus to the outermost shell of electrons. For practical purposes, atomic radius can be defined in many ways.
It is defined as the distance from the centre of the nucleus to the outermost shell of electrons. For practical purposes, atomic radius can be defined in many ways.
a. Covalent Radius
1.
Half of the inter-nuclear distance between two
identical or almost identical atoms bonded by a single covalent bond.
2. For
a diatomic molecule,
Distance (A-A) = radius of A + radius of
A
or d=2rA or rA=d/2
or d=2rA or rA=d/2
3. For
a hetero nuclear diatomic molecule,
Distance (A - B) = radius of A + radius of B
The above relations hold good only when the bond is purely covalent.
Distance (A - B) = radius of A + radius of B
The above relations hold good only when the bond is purely covalent.
b. Van der Waals' Radius
1. Half
of the inter-nuclear distance between the nuclei of two non-bonded adjacent
atoms belonging to different molecules having identical atoms in solid state.
2. This radius is taken into consideration for those cases where
intermolecular attractive forces are less strong, e.g., weak dispersion forces.
The examples of such molecules are molecules of noble gases, saturated
molecules etc.
‘The covalent radius is always smaller
than van der Waals' radius for a given element’.
c. Crystal Radius
1. The
atomic radius of metals and inert gases in solid state is called their crystal
radius
2. It
is defined as half of the inter-nuclear distance between two non-bonded
adjacent atoms in closed packed crystal lattice.
A
crystal radius is 10 - 15 % greater than the covalent radius of a particular
atom but is smaller than its van der Waals' radius.
Trends
in atomic radii
1.
Atomic radii of elements increase on moving down the group due
to increase in the number of shells and increase in screening effect, which
reduces effective nuclear charge.
2.
Atomic radii of elements decrease while moving from left to right in
a period. This is due to the fact that effective nuclear charge increases
as number of inner electrons remain the same throughout the period and the
change occurs only in the number of valence electrons.
3.
In case of transition elements, atomic
radii remains almost same because the electrons add to penultimate, i.e., (n -
1) d sub shell.
Consequently, the increased nuclear charge is almost compensated by the screening effect.
Consequently, the increased nuclear charge is almost compensated by the screening effect.
2.
Ionic Radius
1. It’s
the distance between the nucleus and the point at which nucleus exerts its
influence, in an ion is called ionic radius.
2. For
the determination of cationic and anionic radii, X-ray diffraction
techniques are used.
a. Radii of Cation
1.
Radius of cation < radius of its neutral
atom. Because of increase in the effective nuclear charge and decrease in
the number of orbits for most of the cases.
2. If
various cations have same number of electrons (isoelectronic), the cation
having greater number of protons is smallest in size.
3. Greater
is the positive charge on the cation of a given atom, smaller is its ionic
radius. E.g.,
Fe+ > Fe2+ > Fe3+
Similarly, Sn > Sn2+ > Sn4+
Fe+ > Fe2+ > Fe3+
Similarly, Sn > Sn2+ > Sn4+
b. Radius of Anion
1. Radius
of anion > radius of its neutral atom.
2. It
is due to decrease in effective nuclear charge.
3. In
case of isoelectronic anions, the anion having greater number of protons is
smallest in size. E.g.,
N3-
|
>O2−
|
>F−
|
|
Number of e− :
|
10
|
10
|
10
|
Number of p :
|
7
|
8
|
9
|
4. Greater
is the negative charge on an atom, greater is its radius. e.g., out of O2−, O− and O the order of size is O2− > O− > O.
Trend
in Ionic Radius
In case of
isoelectronic species, the ionic radii decrease with increase in atomic
number.
In a group, the ionic radius of cation as well as anion increases on moving downwards.
In a group, the ionic radius of cation as well as anion increases on moving downwards.
3.
Variation of size in inner transition
elements
1. The
inner transition elements are the f-block elements.
2. The
elements from La to Lu (14 elements) are called lanthanides. They are characterized
by the filling up of the anti-penultimate 4f orbitals.
3. Lanthanum
is the first member of the third transition series, and it has one 5d and two
6s electrons.
4. The
next element is Cerium, which while still retaining two 6s electrons, has two
electrons in the 4f orbitals and none in the 5d orbitals.
5. The
atoms of the elements from cerium to lutetium have two to fourteen electrons in
4f- orbitals, respectively.
6. These
elements constitute the first inner transition series known as lanthanides and,
although lanthanum itself does not possess any 4f electrons; it is customary to
include this element in this series.
7. Except
for lanthanum, gadolinium and lutetium, which have single 5d electrons none of
the lanthanides have electrons in 5d orbital.
Lanthanide
contraction
1.
The 4f electrons constitute inner
shells and are rather ineffective in screening the nucleus; thus there is a
gradual increase in the attraction of the nucleus for the peripheral electrons
as the nuclear charge increases, and a consequent contraction in atomic radius
is observed.
For example: The ionic radii of the +3 cations decrease steadily from a value of 115 pm for La3+ to a value of 93 pm for Lu3+.
For example: The ionic radii of the +3 cations decrease steadily from a value of 115 pm for La3+ to a value of 93 pm for Lu3+.
2.
The regular decrease in atomic radii
with increase in atomic number is known as lanthanide contraction.
3.
The lanthanide contraction considerably
influences the chemistry of the elements, which succeed the lanthanides in the
periodic table.
For
instance:
The atomic radii of zirconium (At. No. 40) and
hafnium (At. No. 72) are almost identical and the chemistry of these two elements
is strikingly similar. Incidentally, the density of hafnium (which immediately
follows the lanthanides) is almost twice the density of zirconium (which is in
the same group).
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