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Lecture 21: Ionic to Covalent • Reading: Zumdahl 13.4-13.6 • Outline – Binary Ionic Compounds – Partial Ionic Compounds – Covalent Compounds

Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

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Page 1: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Lecture 21: Ionic to Covalent

• Reading: Zumdahl 13.4-13.6

• Outline– Binary Ionic Compounds– Partial Ionic Compounds– Covalent Compounds

Page 2: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Electronegativity

• Electronegativity: The ability of an atom in a molecule to attract shared electrons to itself.

Page 3: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Electronegativity• Electronegativity can be defined in many ways.

Pauling model is the most widely used.

• Idea: compare the bond energy of an “HX” molecule to that of the average of an HH bond and an XX bond:

Expected energy = [(H-H energy)(X-X energy)]1/2

= (H-X)experimental - (H-X)expected

= 0: covalent > 0: ionic character

Page 4: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Electronegativity (cont.)• Pauling used this approach to develop a scale, where

F = 4.0 (flourine has largest electronegativity).

F = 4

Cl = 3.2

O = 3.4

C = 2.6

H = 2.2

Na = 0.9

Page 5: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Electronegativity (cont.)• The key idea is this: the greater the electronegativity

difference between two atoms, the more ionic the bond.

• Example: Which of the following compounds is expected to demonstrate intermediate bonding behavior (i.e., polar covalent).

Cl-Cl O-H Na-Cl

elect 0 1.2 2.3

Page 6: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Dipole Moments• The above discussion involved bonds in

which electrons were shared, but shared unequally in polar, covalent bonds

• In the HF example, when placed in an electric field the HF atoms will align.

• This observation demonstrates that the centers of negative and positive charge do not coincide.

Page 7: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Dipole Moments (cont.)• When the centers of negative and positive charge are

separated, we say that the molecule has a dipole moment.

Page 8: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Dipole Moments (cont.)• The dipole moment () is defined as:

= QR

Charge magnitude Separation distance

+ center

R

Page 9: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Dipole Moments (cont.)• The units of dipole moment are generally the Debye (D):

D = 3.336 x 10-30 C.m

• Example, the dipole moment of HF is 1.83 D. What would it be if HF formed an ionic bond (bond length = 92 pm)?

M = (1.6 x 10-19 C)(9.2 x 10-11 m)

= 1.5 x 10-29 C.m x (1D/3.336 x 10-30 C.m)

= 4.4 D

Page 10: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Dipole Moments (cont.)• Molecular geometry is a critical factor in determining if a

molecule has a dipole moment:

Page 11: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Dipole Moments (cont.)• Molecular geometry is a critical factor in determining if a

molecule has a dipole moment:

No net dipole moment. Dipoles add vectorially!

Page 12: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Properties of Ions• When will a stable bond be formed?

• When one exams a series of stable compounds, it becomes evident that in the majority of compounds, bonding is achieved such that atoms can achieve a nobel-gas configuration

• Example: NaCl versus Na+Cl-

Na: [Ne]3s1 Cl: [Ne]3s23p5

Na+: [Ne] Cl-: [Ne]3s23p6 = [Ar]

Page 13: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Properties of Ions (cont.)

• In this example involving NaCl, we have a metal (Na) bonding to a non-metal (Cl).

• Metal/non-metal binding generally results in ionic bonding.

Page 14: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Properties of Ions (cont.)

• One can use this tendency to satisfy the “octet rule” to predict the stoichiometry of ionic compounds.

• Example: Ca and O

Ca: [Ar]4s2 O: [He]2s22p4

2 e-

Ca2+: [Ar] O2-: [He]2s22p6 = [Ne]

Formula: CaO

Page 15: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Properties of Ions (cont.)

• Ions on figure correspond to nobel-gas electron configurations.

• To form ionic binary compounds, one simply combines in proportions such that total charge is zero.

• This approach is not to be applied to transition metals.

Page 16: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Properties of Ions (cont.)

• Note that size decreases for isoelectronic species.

• Mainly a consequence of increased charge of nucleus.

Page 17: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Partial Ionic Compounds

• From last lecture, if two atoms forming a bond have differing electronegativities, they will form a bond having ionic character.

• But where is the dividing line between “ionic” bonding and “polar covalent” bonding?

• In the end, total ionic bonding is probably never achieved, and all “ionic” bonds can be considered polar covalent, with varying degrees of ionic character.

Page 18: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Dipole Moments• The dipole moment () is defined as:

= QR

Charge magnitude Separation distance

+ center

R

Page 19: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Dipole Moments (cont.)

• Example, the dipole moment of HF is 1.83 D. What would it be if HF formed an ionic bond (bond length = 92 pm)?

M = (1.6 x 10-19 C)(9.2 x 10-11 m)

= 1.5 x 10-29 C.m x (1D/3.336 x 10-30 C.m)

= 4.4 D

Page 20: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Partial Ionic Compounds (cont.)• We can define the ionic character of bonds as follows:

% Ionic Character = x 100%(dipole moment X-Y)experimental

(dipole moment X+Y-)calculated

Page 21: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Partial Ionic Compounds (cont.)

Covalent

Polar Covalent

Ionic

Increased Ionic Character

Page 22: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Covalent Compounds

• In covalent bonding, electrons are “shared” between bonding partners.

• In ionic bonding, Coulombic interactions resulted in the bonding elements being more stable than the separated atoms.

• What about covalent bonds…what is the “driving force”?

Page 23: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Covalent Compounds (cont.)

• Back to H2.

Page 24: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Covalent Compounds (cont.)

• The same concept can be envisioned for other covalent compounds:

Think of the covalent bond as theelectron density existingbetween the C and H atoms.

Page 25: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Covalent Compounds (cont.)• We can quantify the degree of stabilization by seeing how

much energy it takes to separate a covalent compound into its atomic constituents.

q

CH4(g)

C(g) + 4H(g)

Page 26: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Covalent Compounds (cont.)• Since we broke 4 C-H bonds with 1652 kJ in, the bond

energy for a C-H bond is:

1652kJ mol4

413kJ mol

• We can continue this process for a variety of compounds to

develop a table of bond strengths.

Page 27: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Covalent Compounds (cont.)• Example: It takes 1578 kJ/mol to decompose CH3Cl into

its atomic constituents. What is the energy of the C-Cl bond?

CH3Cl: 3 C-H bonds and 1 C-C bond.

3 (C-H bond energy) + C-Cl bond energy = 1578 kJ/mol

413 kJ/mol

1239 kJ/mol + C-Cl bond energy = 1578 kJ/mol

C-Cl bond energy = 339 kJ/mol

Page 28: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Covalent Compounds (cont.)

• We can use these bond energies to determine Hrxn:

H = sum of energy required to break bonds (positive….heat into system) plus the sum of energy released when the new bonds are formed (negative….heat out from system).

Hrxn Dbonds broken Dbonds formed

Page 29: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Covalent Compounds (cont.)• Example: Calculate H for the following reaction using

the bond enthalpy method.

CH4(g) + 2O2 (g) CO2 (g) + 2H2O (g)

Go to Table 13.6:

C-H 413O=O 495

O-H 467C=O 745

4 x2 x

4 x2 x

Page 30: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Covalent Compounds (cont.)CH4(g) + 2O2 (g) CO2 (g) + 2H2O (g)

Hrxn Dbonds broken Dbonds formed = 4D(C-H) + 2D(O=O) - 4D(O-H) - 2D(C=O)

= 4(413) + 2(495) - 4(467) - 2(745)

= -716 kJ/mol

• Exothermic, as expected.

Page 31: Lecture 21: Ionic to Covalent Reading: Zumdahl 13.4-13.6 Outline –Binary Ionic Compounds –Partial Ionic Compounds –Covalent Compounds

Covalent Compounds (cont.)CH4(g) + 2O2 (g) CO2 (g) + 2H2O (g)

• As a check:

Hrxno H f

o (prod.) H fo (react .)

= H°f(CO2(g)) + 2H°f(H2O(g)) - H°f(CH4(g)) - 2 H°f(O2(g))

0

= -393.5 kJ/mol + 2(-242 kJ/mol) - - (-75 kJ/mol)

= -802.5 kJ/mol