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Transition Metals: Electronic Structure, Coordination Compounds, and Properties, Exercises of Chemistry

A comprehensive overview of transition metals, covering their electronic structure, coordination compounds, and key properties. It delves into the crystal field theory, explaining how d-orbital energies split in the electrostatic field of ligands. The document also explores the spectrochemical series, which helps predict the color and magnetic properties of complexes. Additionally, it examines the trends in physical and chemical properties of transition metals, including atomic radii and redox potentials. Enriched with examples and diagrams to illustrate concepts and enhance understanding.

Typology: Exercises

2024/2025

Uploaded on 02/24/2025

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Chapter 19: The d-block elements
Trends in Physical Properties
Trends in Chemical Properties
The Electronic Structure
Crystal Field Theory
The Spectrochemical Series
The Colors of Complexes
The Magnetic Properties of Complexes
Ligand Field Theory
Coordination Compounds
Coordination Complexes
The Shapes of Complexes
Isomers
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Chapter 19: The d - block elements

Trends in Physical Properties Trends in Chemical Properties The Electronic Structure Crystal Field Theory The Spectrochemical Series The Colors of Complexes The Magnetic Properties of Complexes Ligand Field Theory Coordination Compounds Coordination Complexes The Shapes of Complexes Isomers

General Properties of Transition Metals:

  • metallic luster
  • wide range of melting points (e.g. W @ 3400 ยฐC, Hg @ - 39 ยฐC) and hardness
  • wide range of reactivity toward O 2 Fe 2 O 3
  • rust Fe 3 O 4
  • magnetite - magnetic recording material Oxides of Cr, Co, and Ni- very hard Coinage metals (Au, Ag, Pt, Pd) do not react readily with O 2

Radial distribution functions Core electrons (1s^2 2s^2 2p^6 )

Na

Remember: ๐ธ๐‘’๐‘™๐‘’๐‘๐‘ก๐‘Ÿ๐‘œ๐‘› โ‰ˆ โˆ’

๐’๐‘’ ๐’“

Radial probability of 3d vs. 4s orbitals Nucleus The energy of an empty atomic 3 d orbital is higher than that of an empty 4s orbital

Electron configurations of the neutral

transition metal elements

4 s

2

4 s

2

3 d

10

4s

2 # Valence electrons/ max. oxidation state 3/ 3 4/^4

5/ 5 6/^6

4 s , 3 d

COMMON OXIDATION STATES

known oxidation states common oxidation states Group 3 4 5 6 7 8 9 10 11 12 Reduction/ Oxidation common = most stable **VO 2

O**^ V

- (3+) - : (^) O : : : : : 4 s , 3 d 5 s , 4 d 6 s , 5 d

Electron configurations of transition metal ions

General Rule: Ionization takes away electrons from the outermost atomic orbitals. Ti (4 s 2 3 d 2 ) โ†’ Ti 2+ ( 3 d 2 ) ( different from Ca (4s 2 ) ) Hundโ€™s Rule: Electron configurations maximizing the spin are preferred by energy. Fe (4 s 2 3 d 6 ) โ†’ Fe 3+ ( 3 d 5 ) The energy of an occupied atomic 3 d orbital is lower than that of an occupied 4s orbital Element 4 s 3 d 4 p Unpaired Electrons Ti โ†‘โ†“^ โ†‘^ โ†‘^2 Element 4 s 3 d 4 p Unpaired Electrons Fe โ†‘โ†“^ โ†‘โ†“^ โ†‘^ โ†‘^ โ†‘^ โ†‘^5

Some important aspects of transition metal ions:

  1. The valence electrons are in d and s orbitals
  2. The d orbitals do not have large radial extension
  3. The d orbitals are therefore mostly nonbonding in complexes of transition metal ions For these reasons, the effects of redox changes are substantially smaller for transition metals than for main group elements

Standard Reduction Potentials

M

n+

+ n e

-

M

The more negative E o , the stronger tendency of M to give electrons in redox reactions (M gets stronger as a reducing agent).

Example:

Fe 2+

  • 2e
  • โ†’ Fe E o = โ€“ 0.44 V Cu 2+
  • 2e

โ†’ Cu E o = 0.34 V

Fe( s ) + Cu

2+

( aq ) โ†’ Fe

2+

( aq ) + Cu( s )

Reaction proceeds spontaneously

The more positive E o, the stronger tendency of Mn+^ to receive electrons in redox reactions (Mn+^ gets stronger as an oxidizing agent)

Reduction Potentials and Transition Metal Reactivity Metals with E **o < 0 are oxidized by H 3 O

upon reacting with acids** Zn ( s ) + 2H 3 O

( aq ) โ†’ Zn 2+ ( aq ) + H 2 ( g ) + 2H 2 O ( l ) Cu 2+

  • 2 e

- โ†’ Cu E o = 0.34 V Cu ( s ) + 2H 3 O

( aq ) โ†’ no reaction Zn 2+

  • 2 e - โ†’ Zn E o = โ€“ 0.76 V

Representation of the 3 d orbitals

d - Orbital lobes affect the properties in two ways: Trends in Physical Properties 1 .) Electrons in the lobes are far apart and weakly repealing each other. 2 .) d - Orbitals are poor at shielding because their electron density is low near the nucleus.

Radial probability of 3d vs. 4s orbitals Nucleus