Chemical Science Short Notes - General Trend of f-Block Elements!!! (Download PDF)

By Renuka Miglani|Updated : February 21st, 2023

Are you looking for some short and reliable notes during your CSIR-NET preparations? Then, you have come to a perfect place!

Candidates preparing for their CSIR NET exam might need to get some short study notes and strategies to apply while preparing for the key exam of their life. At this point, We at Byjus Exam Prep come up with short notes on the General Trend of f-Block Elementswhich comes under the Inorganic Chemistry section of the Chemical Science syllabus

Our experienced Exam experts have meticulously designed this set of short notes on the General Trend of f-Block Elements to give you the most standard set of study materials to be focused upon. In this cut-throat competitive world, students need to prepare themselves with the best study materials to help them learn for their future. So, here we are offering the best study notes that are reliable and can be used by students during their preparations for the upcoming CSIR-NET 2023 exam.

Are you looking for some short and reliable notes during your CSIR-NET preparations? Then, you have come to a perfect place!

Candidates preparing for their CSIR NET exam might need to get some short study notes and strategies to apply while preparing for the key exam of their life. At this point, We at Byjus Exam Prep come up with short notes on the General Trend of f-Block Elements, which comes under the Inorganic Chemistry section of the Chemical Science syllabus

Study Notes on General Trend of f-Block Elements 

Lanthanoid Chemistry:

All lanthanoids are electropositive metals having remarkable chemical properties. Between two lanthanoids, there exists a significant difference only in their atomic or ionic radius. For example, the electronic and magnetic properties of the material generally depend on the exact separation of the atoms and the extent of overlap of various atomic orbitals.

General trends:

Generally, all elements from La to Lu are highly electropositive having standard potentials of the Ln3+/Ln couple like that of Mg2+/Mg. They can easily form an oxidation state Ln (III). Some properties change significantly. Like, the radii of Ln3+ ions contract steadily from 116 pm for La3+ to 98 pm for Lu3+. The decrease in atomic radius takes place due to an increase in effective atomic number, Zeff, as electrons are added to the poorly shielding 4f subshell.

The given below graph shows that the decrease in ionic radius corresponds to two gentle curves intersecting at Gd3+ (f7). The effect can be compared with d block and later can be traced to the splitting of the f-orbital energies by the crystal field generated by the ligand environment, but this splitting is less as compared to d block. On the left of the series, the lower energy f orbitals (which point away from the ligands) are occupied as the number of f electrons increases (f1 to f*). For later configurations, such as f6 and f7, the higher energy f orbitals are occupied, and as these point towards the ligands, the increased electron-ligand repulsion results in a smaller than expected decrease in ionic radius.

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Due to the 18 per cent decrease in ionic radius from La3+ to Lu3+, an increase in the hydration enthalpy across the series takes place. The reason behind the occurrence of the lanthanoids as Ln (III) is that once the s and d electrons are removed, the f electrons will be held tightly by the nucleus. A further consequence of the burying of the f electrons is that an Ln3+ ion has no frontier orbitals with directional preference, so ligand-field stabilization plays only a small part in the properties of lanthanoid complexes. For a few complexes weak stabilization energies (of a few kilojoules per mole) are observed for configurations such as f4, f10, and f11 when compared with f0, f7, and f14.

Superimposed on the common occurrence of Ln3+, there are some atypical oxidation states that are most prevalent when the ion can attain the relatively more stable empty (f0), half-filled (f7), or filled (f14) subshell So, due to this, Ce3+ (f1) can be oxidized to Ce4+ (f4+) and the latter is a strong and useful oxidizing agent. The next most common of the atypical oxidation states is Eu2+ (f7), and there are several stable Eu2+ compounds, including Eul2, EuSO4, and EuCO3, and solutions of this ion are generally stable. The ions Sm2+ and Yb2+ also have extensive chemistry but get reduced from water to hydrogen in aqueous solutions. Recently, Dy (II), Nd (II), and Tm (II) have been produced in molecular complexes in solution; an example is NdI2(THF)5. Other reasonably stable oxidation states include Pr (IV) and Tb (IV), and the oxides of these elements formed in air, Pr6O11, and Tb4O7, contain mixtures of Ln (III) and Ln (IV). Under very strongly oxidizing conditions, Dy (IV) and Nd (IV) can be obtained. An Ln3+ ion is a hard Lewis acid as it binds with F and oxygen-containing ligands and its occurrence with PO43- minerals. 

Element names, symbols, and selected properties of the lanthanoids

Z

Name

Symbol

Configuration

Standard potential

Radius

Nox

57

Lanthanum

La

[Xe]

-2.38

116

2(n), 3,4

58

Cerium

Ce

[Xe]f1

-2.34

114

2(n), 3, 4

59

Praseodymium

Pr

[Xe]f2

-2.35

113

2(n), 3, 4

60

Neodymium

Nd

[Xe]f3

-2.32

111

2(n), 3

61

Promethium

Pm

[Xe]f4

-2.29

109

3

62

Samarium

Sm

[Xe]f5

-2.30

108

2(n), 3

63

Europium

Eu

[Xe]f6

-1.99

107

2,3

64

Gadolinium

Gd

[Xe]f7

-2.28

105

3

65

Terbium

Tb

[Xe]f8

-2.31

104

3,4

66

Dysprosium

Dy

[Xe]f9

-2.29

103

2(n),3

67

Holmium

Ho

[Xe]f10

-2.33

102

3

68

Erbium

Er

[Xe]f11

-2.32

100

3

69

Thulium

Tm

[Xe]f12

-2.32

99

2(n),3

70

Ytterbium

Yb

[Xe]f13

-2.22

99

2, 3

71

Lutetium

Lu

[Xe]f14

-2.30

98

3

 

Dy

Dysprosium

Eu

Europium

Nd

Neodymium

Pr

Praseodymium

Sm

Samarium

Tb

Terbium

Tm

Thulium

Yb

Ytterbium

 

 

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