60
Chapter 13 Slide 1 of 60 Chapter 13 Bonding: General Concepts

Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

  • Upload
    others

  • View
    1

  • Download
    0

Embed Size (px)

Citation preview

Page 1: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 1 of 60

Chapter 13

Bonding: General Concepts

Page 2: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 2 of 60

Chemical Bonds: A Preview

• Forces called chemical bonds hold atoms together in molecules and keep ions in place in solid ionic compounds.

• Chemical bonds are electrical forces; they reflect a balance in the forces of attraction and repulsion between electrically charged particles.

• Through appropriate measurements, scientists can determine the internuclear distances that correspond to the lowest energy states of molecules.

• Quantum mechanical calculations can then be used to develop a theoretical model that fits the experimental measurements.

Page 3: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 3 of 60

Electrostatic Attractions and Repulsions

Page 4: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 4 of 60

Energy of Interaction

A B

B

B

B

A

A

A

Page 5: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 5 of 60

Electronegativity

• Electronegativity (EN, expressed as χ), is a measure of the ability of an atom to attract bonding electrons to itself when the atom is in a molecule.

• Mulliken’s EN

Absolute EN, χ = (IE + EA)/2• Pauling’s EN

define χH = 2.2∆ χ = χA - χB = [∆ΑΒ(kJ)/96.49]1/2 = [∆ΑΒ(kcal)/23.06]1/2

∆ΑΒ = D(A-B) - 1/2 [D(A-A) + D(B-B)]

Bond dissociation energy of A-B

Page 6: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 6 of 60

Pauling’s Electronegativities

2.2

Page 7: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Electronegativity Differenceand Bond Type

• Two identical atoms have the same electronegativity and share a bonding electron pair equally. This is called a non-polar covalent bond. (For χA ~ χB, or lχA - χBl < 0.3)

• In covalent bonds between atoms with somewhat larger electronegativity differences (0.3 < lχA - χBl < 1.8) , electron pairs are shared unequally. The electrons are drawn closer to the atom of higher electronegativity, and the bond is called a polar covalent bond.

• With still larger differences in electronegativity (lχA - χBl > 1.8) , electrons may be completely transferred from metal to nonmetal atoms to form ionic bonds.

Page 8: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 8 of 60

Electronegativity and Bond Type

Page 9: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 9 of 60

Ionic Bonds and Ionic Crystals

• When atoms lose or gain electrons, they acquire a noble gas configuration, but do not become noble gases.

• Because the two ions formed in a reaction between a metal and a non-metal have opposite charges, they are strongly attracted to one another and form an ion pair.

• The net attractive electrostatic forces that hold the cations and anions together are ionic bonds.

• The highly ordered solid collection of ions is called an ionic crystal.

Page 10: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Interionic Forces of Attraction- Coulombic Force

E = (Z+Z-)/4πεr

Page 11: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 11 of 60

Formation of a Crystalof Sodium Chloride

Page 12: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Unit Cell of Sodium Chloride

Page 13: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 13 of 60

Energy Changes inIonic Compound Formation

• The enthalpy of formation of the ionic compound is more important than first ionization energy and electron affinity.

• The overall enthalpy change can be calculated using a step-wise procedure called the Born-Haber cycle.

• The sum of the enthalpy change values for the individual steps is in accordance with Hess’s Law.

• The large negative value of the lattice energy is the major factor that makes ionic compound formation an energetically favorable process.

Page 14: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 14 of 60

A Born-Haber Cycle Example

- EA(Cl)IE(Na)

1/2D(Cl-Cl)

∆Ηsublimation (Na) ∆H5 = - UU : lattice energy

Page 15: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 15 of 60

A Born-Haber Cycle ExampleU

1/2D(Cl-Cl)

∆Ηsublimation (Na)

IE(Na) -EA(Cl)

lattice energy U = - ∆Ηf0(NaCl) + ∆Ηsublimation (Na) + 1/2D(Cl-Cl) + IE(Na) - EA(Cl)

= (+411 +107 +122 + 496 –349) kJ/mol

= +787 kJ/mol

∆Ηf0(NaCl)

NaCl(s) Na+(g) + Cl-(g)

Na(g) + Cl(g)Na(s) + 1/2Cl2(g)

Page 16: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 16 of 60

The Lewis Theory ofChemical Bonding

• Electrons, particularly valence electrons, play a fundamental role in chemical bonding.

• When metals and non-metals combine, valence electrons usually are transferred from the metal to the non-metal atoms giving rise to ionic bonds.

• In combinations involving only non-metals, one or more pairs of valence electrons are shared between the bonded atoms producing covalent bonds.

• In losing, gaining, or sharing electrons to form chemical bonds, atoms tend to acquire the electron configurations of noble gases.

Page 17: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 17 of 60

Lewis Symbols

• In a Lewis symbol, the chemical symbol for the element represents the nucleus and core electrons of the atom, and dots around the symbol represent the valence electrons.

Page 18: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 18 of 60

Using Lewis Symbolsto Represent Ionic Bonding

• Instead of using complete electron configurations to represent the loss and gain of electrons, Lewis symbols can be used for ionic bond.

·· ··Na· + ·Cl: → Na1+ :Cl: 1-

·· ··

Page 19: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 19 of 60

Lewis Structures OfSimple Molecules

• A Lewis structure is a combination of Lewis symbols that represents the formation of covalent bonds between atoms.

• In most cases, a Lewis structure shows the bonded atoms with the electron configuration of a noble gas; that is, the atoms obey the octet rule. (H obeys the duet rule.)

Page 20: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 20 of 60

Lewis Structures (continued)

• The shared pairs of electrons in a molecule are called bonding pairs.

• In common practice, the bonding pair is represented by a dash (-).

or• The other electron pairs, which are not shared, are

called non-bonding pairs, or lone pairs.

Page 21: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 21 of 60

2nd period elements follow octet rule

The non-metals of the second period (except boron?) tend to form a number of covalent bonds equal to eight minus the group number.

Page 22: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 22 of 60

Coordinate Covalent Bonds

For example:• hydronium ions

H3O+

• F3B-NH3

In some cases, one atom provides both electrons of the shared pair to form a bond called a coordinate covalent bond (or dative bond).

Page 23: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 23 of 60

Multiple Covalent Bonds

• The covalent bond in which one pair of electrons is shared is called a single bond.

• Multiple bonds can also form:– Double bonds have two shared pairs of

electrons.– Triple bonds have three shared pairs of

electrons.• A double bond is represented by two dashes (=).• A triple bond is represented by three dashes (≡).

Page 24: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 24 of 60

Polar and Non-polarCovalent Bonds

Page 25: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 25 of 60

Formal Charge

Formal charge = # of valence electrons - [# of lone pair electrons + ½ (bonding

electrons)]• Usually, the most plausible Lewis structure is one with

no formal charges.• When formal charges are required, they should be as

small as possible.• Negative formal charges should appear on the most

electronegative atoms.• Adjacent atoms in a structure should not carry formal

charges of the same sign.

Page 26: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 26 of 60

Formal Charge Illustrated

Page 27: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 27 of 60

Lewis Structures & Formal Charge

CO FC(C) = 4 - 2 - 3 = -1

FC(O) = 6 - 2 - 3 = +1

CO2 FC(C) = 4 - 0 - 4 = 0

FC(O) = 6 - 4 - 2 = 0

N2O ↔ ↔

(-1) (+1)

(0) (0) (0)

(-1) (0)(+1) (0) (+1) (-1) (-2) (+1) (+1)

(+2) (-1)(-1)

resonance structures

Page 28: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 28 of 60

Resonance: Delocalized Bonding

• Resonance theory states that whenever a molecule or ion can be represented by two or more plausible Lewis structures that differ only in the distribution of electrons, the true structure is a composite, or hybrid, of them.

• The different plausible structures are called resonance structures.

• The actual molecule or ion that is a hybrid of the resonance structures is called a resonance hybrid.

• Electrons that are part of the resonance hybrid are spread out over several atoms and are referred to as being delocalized.

Page 29: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 29 of 60

Resonance

ClO42-

(+3) (+2) (+1)

(0) (-1)

(-1)

(-1)(-1)

(-1)

(-1) (-1)

(-1)

(0)

↔↔ ↔

Oxoacids: HNO3, H2SO4, HClO4

Page 30: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 30 of 60

Molecules that Don’t Followthe Octet Rule

• Molecules with an odd number of valence electrons have at least one of them unpaired and are called free radicals.

• Some molecules have incomplete octets. These are usually compounds of Be, B, and Al, generally have some unusual bonding characteristics, and are often quite reactive.

Page 31: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 31 of 60

Molecules that Don’t Followthe Octet Rule (continued)

• Some compounds have expanded valence shells, which means that the central atom has more than eight electrons around it.e.g. SF6, PCl5

Page 32: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 32 of 60

Bond Lengths

• The term bond order indicates whether a covalent bond is single (b.o. = 1), double (b.o. = 2), or triple (b.o. = 3).

• Bond length is the distance between the nuclei of two atoms joined by a covalent bond.

• Bond length depends on the particular atoms in the bond and on the bond order.

• The length of the covalent bond joining unlike atoms is the sum of the covalent radii of the two atoms.

• Bond lengths are usually measured in picometers(10-12 meter).

Page 33: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 33 of 60

A Visualization of Bond Dissociation Energy

Page 34: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 34 of 60

Bond Energies

• Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent bonds between atoms in a molecule in the gas phase.

• An average bond energy is the average of the bond-dissociation energies for a number of different molecules containing the particular bond.

average bond energy of O-H= (499 + 428)/2 = 464 J/mol

bond-dissociation energy of H-H= 436 kJ/mol

Page 35: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 35 of 60

Bond Energies

Page 36: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 36 of 60

Representative Bond Lengths & Average Bond Energies

??

?

Page 37: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 37 of 60

Bond Dissociation Energies & Hreaction

•The sum of the enthalpy changes for breaking the old bonds and forming the new bonds is the enthalpy change for the reaction.

C2H6 + Cl2 → C2H5Cl + HCl

∆Hreaction = ∆Hbond broken + ∆Hbond formed

= Σ D(bonds broken) - Σ D(bonds formed)

∆H = [D(C-H) + D(Cl-Cl)] - [D(C-Cl) + D(H-Cl)]

= [414 +243] – [339 + 431] = -113 kJ/mol

> 0 < 0

∆ H

Page 38: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 38 of 60

Molecular Geometry

• The molecular geometry, or the shape of a molecule is described by the geometric figure formed when the atomic nuclei are imagined to be joined by the appropriate straight lines.

• Determination of molecular geometry1. Valence-Shell Electron-Pair Repulsion (VSEPR)- Pairs of valence electrons in bonded atoms repel one another.- The mutual repulsions push electron pairs as far from one another

as possible.

2. Ligand Field Stabilization Energy- Mainly for compounds with the central atoms as transition metals

Page 39: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 39 of 60

Molecular Geometry of Water

Page 40: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 40 of 60

Electron-Group Geometries

• An electron group is any collection of valence electrons, localized in a region around a central atom, that repels other groups of valence electrons.

• The mutual repulsions among electron groups lead to an orientation of the groups that are called electron-group geometry.

Page 41: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 41 of 60

Electron-Group Geometries

#. ofElectron Pair

Electron-groupGeometry

2 linear

3 trigonal planar

4 tetrahedral

5 Trigonalbipyramidal

6 octahedral

Page 42: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 42 of 60

A Balloon Analogy

Page 43: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 43 of 60

Geometries of Methane#. of electron group on C = 1/2 (4 + 4) = 4

Electron group geometry: tetrahedral

VSEPR notation AX4

Molecular geometry: tetrahedral

109.50

Page 44: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 44 of 60

Molecular Geometry of Water

#. of electron group on O = 1/2 (6 + 2) = 4

Electron group geometry: tetrahedral

VSEPR notation AX2E2

Molecular geometry: bent

104.50 103.20

A: the central atom in a structureX: terminal atomsE: the lone pairs of electrons

Page 45: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 45 of 60

Electron Repulsion

• Lone-pair – Lone-pair > Lone-pair – Bonding-pair> Bonding-pair – Bonding-pair

• Triple bond > Double bond > Single bond

Electron Repulsion

Page 46: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 46 of 60

Molecular Geometry forIodine Pentafluoride (IF5)

#. of electron group on I = 1/2 (7 + 5) = 6

Electron group geometry: octahedral

VSEPR notation AX5E

Molecular geometry: Square pyramidal

Page 47: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 47 of 60

Molecular Geometry forSulfur Tetrafluoride (SF4)

#. of electron group on S = 1/2 (6 + 4) = 5

Electron group geometry: trigonal bipyramidal

VSEPR notation AX4E

Molecular geometry: trigonal pyramidal or Seesaw

9001200

900

Page 48: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 48 of 60

Molecular Geometry forIodine Trifluoride (IF3)

#. of electron group on I = 1/2 (7 + 3) = 5

Electron group geometry: trigonal bipyramidal

VSEPR notation AX3E2

Molecular geometry: triangular or T-shaped

9001200

1200

Page 49: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 49 of 60

Molecular Geometry forIodine Tetrafluoride Ion (IF4

-)

#. of electron group on I = 1/2 (7 + 4 +1) = 6

Electron group geometry: octahedral

VSEPR notation AX4E2

Molecular geometry: Square planar

Page 50: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 50 of 60

A VSEPR Summary

Page 51: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 51 of 60

A VSEPR Summary (continued)

Page 52: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 52 of 60

A VSEPR Summary (continued)

Page 53: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 53 of 60

A VSEPR Summary (continued)

Page 54: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 54 of 60

Polar Moleculesand Dipole Moments

• A molecule with separate centers of positive and negative charge is called a polar molecule.

• The dipole moment (µ) of a molecule is the product of the magnitude of the charge (δ) and the distance (d) that separates the centers of positive and negative charge.

µ = δ d

Page 55: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 55 of 60

Polar Moleculesand Dipole Moments

• Dipole moments are generally expressed in a quantity

called a debye.

• 1 debye (D) = 3.34 x 10-30 C m = 10-18 esu

• charge of electron = 1.602 x 10-19 C = 4.80 x 10-10 esu

Page 56: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 56 of 60

Polar Moleculesand Dipole Moments

Calculation of percentage ionic character of HCl

Η−Cl, µ = 1.08 D, r H-Cl = 127pm

δ = µ /d = 1.08 x 3.34 x 10-30 /(127 x 10-12 )

= 2.84 x10-20 C

percentage ionic character = [2.84 x10-20 / (1.602 x 10-19)]

x 100% = 17.7%

Page 57: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 57 of 60

Dipole-Dipole Interactions

Dipole momentµ = δ ·d

E = - 2(µ1 ·µ2)/4πεr3

d

r

µ2

µ1

Page 58: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 58 of 60

How Polar Molecules Behave in an Electric Field

Page 59: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 59 of 60

Bond Dipoles andMolecular Dipoles

• All polar covalent bonds have a bond dipole; a separation of positive and negative charge centers in an individual bond.

• Bond dipoles have both a magnitude and a direction.

• molecular dipole = vector sum of bond dipolesCO2, linear with no dipole moment (µ = 0 D) water is bent (bond angle = 104.5o) and µ = 1.84 D.

Page 60: Chapter 13case.ntu.edu.tw/CASTUDIO/Files/speech/Ref/CS0099S1B02_13.pdf · Bond Energies • Bond-dissociation energy (D) is the quantity of energy required to break one mole of covalent

Chapter 13 Slide 60 of 60

Molecular Shapesand Dipole Moments

• Molecules can be predicted to be polar or non-polar based on the following three-step approach:– Use electronegativity values to predict bond

dipoles.– Use the VSEPR method to predict the molecular

shape.– From the molecular shape, molecular dipole =

vector sum of bond dipoles• Lone-pair electrons can also make a contribution to

dipole moments. e.g. NH3 µ = 5.0 x 10-30 C.mNF3 µ = 0.7 x 10-30 C.m