Chemistry 1000 Lecture 9: Periodic trendspeople.uleth.ca/~roussel/C1000/slides/09trends.pdfRemoving...

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Chemistry 1000 Lecture 9: Periodic trends Marc R. Roussel October 3, 2018 Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 1 / 28

Transcript of Chemistry 1000 Lecture 9: Periodic trendspeople.uleth.ca/~roussel/C1000/slides/09trends.pdfRemoving...

Chemistry 1000 Lecture 9: Periodic trends

Marc R. Roussel

October 3, 2018

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 1 / 28

Some basic ideas

A qualitatively correct result of the Bohr theory

Some results of the Bohr theory are qualitatively correct, even formulti-electron atoms, but need to be reinterpreted.

Recall, from Bohr theory, rn ∝ n2/Z .

We call a set of orbitals with the same n a shell.

Orbitals in a shell are similar in size, proportional to n2/Zeff whereZeff is an effective nuclear charge.

The electron distribution of a closed shell (one in which all the orbitalare filled) is spherical.

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 2 / 28

Some basic ideas

Effective nuclear charge

Theorem: The force on a test charge due to a spherical chargedistribution is

zero if the charge is inside the distribution, andequal to the force due to a single charge equal to thetotal charge of the distribution placed at the centre ofthe sphere if the test charge is outside the sphere.

What this means to us: An electron in a valence orbital feels a forcetoward the nucleus that is reduced by the repulsive force ofthe closed inner shells.On the other hand, the valence orbitals have little effect onthe inner shells.

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 3 / 28

Some basic ideas

Effective nuclear charge

nin

nin

Nucleus of

atomic number

Z

inner shell

containing

electrons

Effective nuclear

Z eff = Z

charge here is

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 4 / 28

Some basic ideas

Effective nuclear chargeExample

The effective nuclear charges experienced by the valence electrons in thesecond row of the periodic table are roughly as follows:

Element Li Be B C N O F Ne

Z 3 4 5 6 7 8 9 10

Zeff 1 2 3 4 5 6 7 8

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 5 / 28

Atomic size

Atomic size

Orbitals don’t have a sharp cut-off.They are “spongy”.So how can we define an atomic size?

Covalent radius: From compounds with single covalent bonds, whethernetwork solids (e.g. diamond) or molecular compounds(e.g. F2)

For elements, the radius is half the distance between thenuclei.For compounds, the distance between the nuclei is the sumof the radii.

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 6 / 28

Atomic size

Atomic size

Metallic radius: Same idea as the covalent radius, but in a metal.What’s the difference, then?In a covalent compounds, some of the valence electrons areshared between two atoms.In a metallic compound, the valence electrons are sharedthroughout the metal.

van der Waals radius: Mostly for noble gases, based on shortest distancebetween atoms in a solid crystal in which the atoms are notbonded to each other.

Important note: These radii are not strictly comparable to each other, sowe should always try to compare measurements of the samekind.

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 7 / 28

Atomic size

Atomic size

Atomic size increases as we move down a group because we areadding shells and r ∝ n2/Zeff .

In a period, for the main-group elements, Zeff increases as we movefrom left to right, so atomic size decreases.

In the transition metals, electrons are being added to an inner shell atthe same rate as Z increases, so Zeff for the outer-shell electrons isroughly constant. Atomic size is therefore roughly constant across thetransition-metal part of a period (with some exceptions).

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 8 / 28

Atomic size

Atomic sizeTrend down a group

140

160

180

200

220

240

260

280

Li Na K Rb Cs

r/pm

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 9 / 28

Atomic size

Atomic sizeTrend across a period

90 100 110 120 130 140 150 160 170 180 190 200

Na Mg Al Si P S Cl

r/pm

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 10 / 28

Atomic size

Atomic sizeTrend in a transition series

120

130

140

150

160

170

Sc Ti V Cr Mn Fe Co Ni Cu Zn

r/pm

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 11 / 28

Atomic size

Ionic radius

Measured analogously to covalent radius, but using crystals of anionic compound.

Bootstrapping problem: You need one radius in order to be able toassign the rest.Convention: r(O2−) = 1.40 A

Generally, similar trends observed as for atomic radii.

Removing electrons (esp. if a shell is emptied) results in cations beingsmaller than the neutral atoms from which they are formed.

The smallest ion in an isoelectronic series has the highest Z .

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 12 / 28

Atomic size

Ionic radius

Example: Put the following ions in order of increasing size: O2−, F−,Na+, Mg2+

Answer: Mg2+ (72 pm), Na+ (102 pm), F− (133 pm), O2− (140 pm)

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 13 / 28

Ionization energy

Ionization energy

Ionization energy = 1st ionization energy = I1

Ionization energy decreases as we go down a group because the outerelectrons are farther from the nucleus and thus more loosely held.

As an overall trend, ionization energy increases as we move from leftto right across a period because the effective nuclear charge increasesand the size of the atom decreases, both of which increase theelectrostatic force between the valence electrons and the nucleus.

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 14 / 28

Ionization energy

We must also consider electronic configuration.

Going from an ns2 to an ns2 np1 configuration, the ionization energydecreases in the first few periods because the p orbital is higher inenergy than the s.Going from an ns2 np3 to an ns2 np4 configuration, the ionizationenergy decreases because pairing electrons in an orbital increaseselectron-electron repulsion, thus making it easier to remove one.

Similar trends are observed in I2, adjusted for the electronicconfigurations of the singly ionized atoms.

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 15 / 28

Ionization energy

Ionization energyTrend down a group

300 400 500 600 700 800 900

1000 1100 1200 1300 1400

H Li Na K Rb Cs

I 1/k

J m

ol-1

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 16 / 28

Ionization energy

Ionization energyTrend across a period for the 1st IE

400

600

800

1000

1200

1400

1600

Na Mg Al Si P S Cl Ar

I 1/k

J m

ol-1

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 17 / 28

Ionization energy

Ionization energyTrend across a period for the 2nd IE

1000

1500

2000

2500

3000

3500

4000

4500

5000

Na Mg Al Si P S Cl Ar

I 2/k

J m

ol-1

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 18 / 28

Electron affinity

Electron affinity

Eea is the negative of the enthalpy change for the processA + e− → A− in the gas phase.

∆H for adding an electron to an atom is usually negative, so Eea ispositive.A larger value of Eea means a stronger attraction for electrons.

Some elements have essentially no ability to accept an additionalelectron.Examples: Be, Mg, N, noble gases. Why?

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 19 / 28

Electron affinity

Electron affinity (continued)

Eea tends to become larger as we go from left to right in a periodbecause of increasing effective nuclear charge and decreasing atomicradius.

Exceptions to the previous observation can generally be rationalized interms of the electron configurations of the atom and anion.

Eea tends to become smaller as we move down a group because ofincreasing atomic radius, but there are many exceptions.

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 20 / 28

Electron affinity

Electron affinityTrend down a group

45

50

55

60

65

70

75

H Li Na K Rb

Eea/kJ mol-1

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 21 / 28

Electron affinity

Electron affinityTrend across a period

0

50

100

150

200

250

300

350

400

Na Mg Al Si P S Cl Ar

Eea/kJ mol-1

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 22 / 28

Electron affinity

Is a full octet especially “stable”?

Many people (including many chemists who should know better) willsay that an octet electron configuration is especially stable.The first problem with this is that it’s not clear what they mean by“stable”.

One might think this means that an octet is especially difficult toionize.

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 23 / 28

Electron affinity

Is a full octet especially “stable”?(continued)

Counterexamples:

If this were so, then the 1st ionization energy of a noble gas should beespecially large. These are relatively large, but fully on-trend, so not“especially” large. The non-metallic p-block elements all tend to havelarge ionization energies.

400

600

800

1000

1200

1400

1600

Na Mg Al Si P S Cl Ar

I 1/k

J m

ol-1

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 24 / 28

Electron affinity

Is a full octet especially “stable”?(continued)

Counterexamples:

Similarly, an electron from a species with a complete outer octetshould be hard to remove. However, the electron affinity of fluorine,for example, which is the same as the ionization energy of the fluorideion, is only 328 kJ mol−1, which isn’t especially large.

So there’s nothing special, per se, about an octet. Removing an electron(e.g.) always requires an electron acceptor. The question then becomeswhether a sufficiently good electron acceptor can be found. Stability is nota matter that can be discussed without a physico-chemical context.

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 25 / 28

Electronegativity

Electronegativity

Usual symbol: χ

An empirical measure of the tendency of an atom to attract electronsThere are in fact several electronegativity scales.

The Mulliken electronegativity scale is linearly related to I + Eea.

The more commonly used Pauling scale is based on bond dissociationenergies, but correlates very well with the Mulliken scale.

Electronegativity decreases as we go down a group.

Electronegativity increases as we go from left to right across a period.

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 26 / 28

Electronegativity

ElectronegativityTrend down a group for χ

0.6

0.8

1

1.2

1.4

1.6

1.8

2

2.2

H Li Na K Rb Cs Fr

χ

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 27 / 28

Electronegativity

ElectronegativityTrend across a period for χ

0.5

1

1.5

2

2.5

3

3.5

Na Mg Al Si P S Cl

χ

Marc R. Roussel Chemistry 1000 Lecture 9: Periodic trends October 3, 2018 28 / 28