copyright©2000 by houghton mifflin company. all rights reserved. 1 ch 7 atomic structure

98
Copyright©2000 by Houghto n Mifflin Company. All ri ghts reserved. 1 Ch 7 Atomic Structure

Upload: oliver-booth

Post on 20-Jan-2016

215 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

1

Ch 7 Atomic Structure

Page 2: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

2

Rutherford Model

QuickTime™ and a decompressor

are needed to see this picture.

Page 3: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

3

Page 4: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

4

Figure 7.2Classification of Electromagnetic

Radiation

Page 5: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

5

Electromagnetic Radiation

Radiant energy that exhibits wavelength-like behavior and travels through space at the speed of light in a vacuum.

Page 6: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

6

Light is a wave

Wavelength Distance between 2

similar points (meters)

Frequency Number of waves in a second (frequency (s1) or hertz (Hz))

Speed v (m/s)

Light: energy that travels like a wave through spaceWave properties:

Page 7: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

7

Wavelength and Frequency

Page 8: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

8

Light is a wave

All light travels the same speed:

high , has short low , has long

high = high energy

Page 9: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

9

Light is a wave

Created by movement of electric charge

An electric field and magnetic field perpendicular to each

Self-propagating

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 10: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

10

Wavelength and frequency can be interconverted.

= c/(C =

= frequency (s1) or hertz (Hz)

= wavelength (m)

c = speed of light (m s1)

(2.9979 x 108 m/s)

Page 11: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

11

Figure 7.2Classification of Electromagnetic

Radiation

Page 12: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

12

Matter is not what it appears to be.

Before 1900:

Matter particle

Light a wave

Max Planck:

not all energies were emitted from objects heated incandescence

Page 13: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

13

Planck’s Constant

E = change in energy, in Jh = Planck’s constant, 6.626 1034 J s = frequency, in s1

= wavelength, in m

Energy gained or lost only in Energy gained or lost only in whole number whole number multiples. Transfer of energy is quantized: multiples. Transfer of energy is quantized: occur in discrete units, called quanta.occur in discrete units, called quanta.

E = nhnhcn = 1, 2,3,..

Page 14: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

14

Light is a particle

Einstein: theorizes that light made of photons.

Gets Nobel Prize QuickTime™ and aTIFF (Uncompressed) decompressorare needed to see this picture.

Page 15: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

15

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 16: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

16

Photoelectric Effect

ExperimentExperiment: light of different frequency shone on metal

Results:Results: e- ejected only at minimum

No e- ejected if too low, EVEN IF light intensity is increased.

WHY?WHY? Why some frequency and not others?

Page 17: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

17

- High photon = high E photon

- One photon hits one electron - If photon E not = to e- E nothing happens (even if bright)

-Giant example

Light made of photons

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 18: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

18

Photoelectric Effect

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 19: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

19

Light made of photons

Einstein: electromagnetic radiation is

quantized:

Ephoton = h = hc

Page 20: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

20

Energy and Mass

Einstein’s special theory of relativity: (1905) Energy has mass:

E = mc2

Or

m=E/c2

E = energym = massc = speed of light

Page 21: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

21

Energy and Mass

(Hence the (Hence the dualdual nature of light.) nature of light.)

Does a photon have mass?

for a photon with wavelength m = E = hc/ mh

c2 c2 c Ephoton= hc/

Page 22: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

22

Figure 7.4Dual Nature of light

Page 23: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

23

If light can be a particle can a particle (e-) be a wave?

m = h /m = h /vh / m h / m v

= wavelength, in m

h = Planck’s constant, 6.626 1034 J s = kg m2 s1

m = mass, in kg

v = velocity in m/s

Louis de Broglie’s Louis de Broglie’s Equation 1920Equation 1920

Page 24: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

24

Wave interference

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 25: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

25

Water wave interference

Page 26: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

26

Interference in water waves

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 27: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

27

Water interference

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 28: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

28

Interference patterns

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 29: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

29

Light interference

Page 30: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

30

Interference Pattern

Page 31: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

31

Electron interference

Diffraction patterns caused by interferenceX-rays passing through NaCl crystal are diffracted.Electrons passing through NaCl crystal are diffracted x-rays

Page 32: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

32

Diffraction using NaClcrystal

Page 33: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

33

So, Debroglie was right: all matter show both wave like and

particle like behavior

Page 34: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

34

How does all this stuff relate to the e- and the atom?

QuickTime™ and a decompressor

are needed to see this picture.

Bohr model: electrons are at set distances from the nucleus (energy levels)

Page 35: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

35

How do we know this?:we can use Einstein’s ideas to

explain bright-line spectra Observe the light coming from the hydrogen emission tube.

“Excited” atoms only emit certain frequencies (colors) of light Why not all frequencies of light? Look at hydrogen emission. Each line is one frequency of light.

Page 36: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

36

Figure 7.6A Continuous Spectrum (a) and A Hydrogen Line Spectrum (b)

Page 37: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Absorption, emission, and energy

Ground State: electrons in lowest energy state.

Excited State: when one electron absorbsabsorbs one photon and jumps to higher energy level.

When electron falls back to G.S. it

emits emits one photon.

electron can only absorb photons or emit photons of just the right energy because levels are fixed.

Absorption

photon

Emission

photon

Page 38: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

38

The emitted photons are seen as light of specific frequency (i.e. colors).

What color emitted if electron could go anyway?

A: the contiuous spectrum

Page 39: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

39

What is the energy difference between levels?

Must be equal to the energy of the photon emitted. Energy levels are quantized:

∆E = h= hc

Page 40: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

40

Figure 7.7A Change between Two Discrete

Energy Levels

Page 41: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

41

Figure 7.8Electronic Transitions in the Bohr Model for the Hydrogen Atom

Page 42: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

42

The Bohr Model

E = energy of the levels in the H-atom

z = nuclear charge (for H, z = 1)

n = an integer

E = 2.178 10 J (18 2− × − z n/ )2

The electron in a hydrogen atom moves around the The electron in a hydrogen atom moves around the nucleus only in certain allowed circular orbits. The nucleus only in certain allowed circular orbits. The energy of each level is given by this equation:energy of each level is given by this equation:

Page 43: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

43

The Bohr Model

Ground State: The lowest possible energy state for an atom (n = 1).

Page 44: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

44

Energy Changes in the Hydrogen Atom

E = Efinal state Einitial state

= hcEΔ

Page 45: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

45

Standing waves in spring: - exist only at specific and ( .5, 1, 1.5, 2.0, 2.5, ect.) - are quantized.

Electron waves: - exist only at certain

and (and energy) - only form certain

distances from nucleus. - are quantized

Page 46: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

46

Figure 7.10The Hydrogen Electron Visualized as a Standing Wave Around the Nucleus

Page 47: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

47

Quantum Mechanics

Schrodinger’s equations: Based on the wave properties of the atom

= wave function

= mathematical operator

E = total energy of the atom

A specific wave function is often called an orbital.

$H E =

$H

Page 48: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

48

What is the orbital for H when n=1?

1s orbital

Orbitals are not the Bohr orbits.

Where is the electron in the orbital?

Page 49: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

49

Heisenberg

There is a limit to how precisely we can both the position and momentum of a an electron at a given timeQuickTime™ and a

decompressorare needed to see this picture.

Page 50: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

50

Heisenberg Uncertainty Principle

x mvh

⋅ ( ) ≥ 4π

• x = position• mv = momentum• h = Planck’s constant• The more accurately we know a

particle’s position, the less accurately we can know its momentum.

Page 51: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

51

What is an orbital?

If we don’t know the motion of an electron, what is an orbital?

square of the wave function gives the probability of finding an electron at a given position.

--> (a) probability distrib.

for H 1s orbital

Page 52: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

52

Figure 7.12Radial Probability Distribution

(the probability distribution in each spherical shell.)

Page 53: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

53

Bohr radius

Turns out that for H 1s orbital, the max radial probability is 5.29x10-2 nm,

= Bohr’s innermost “orbit”.

Page 54: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

54

How big is the 1s?

Probab. Decreases with radius, but never goes to zero.

Size definition: Size of the orbital is the radius of the sphere that encloses 90% of the electron’s probability.

Page 55: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

55

Quantum Numbers (QN)Schrodinger equation has many wave function solutions.

Each are described by quantum numbers1. Principal QN (n = 1, 2, 3, . . .) - related to size and energy of the orbital.

(this gives the”rings” or “shells)

2. Angular Momentum QN (l = 0 to n 1) - relates to the shape of the orbital. (ex. s p d f also called subshells)

1. Magnetic QN (ml = l to l ) - relates to orientation of the orbital in space relative to other orbitals. Gives you the number of each type of orbital.

(ex.: px py pz)

4. Electron Spin QN (ms = +1/2, 1/2) - relates to the spin states of the electrons.

(see pg 310, table 7.2)

Page 56: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

56

Orbitals when n=1 (principal quantum #):

(l = 0 to n-1)

(ml = l to - l ): l =0 ml=0 1s orbital only.

Only 1 or 2 electrons are described by an orbital.

Total electrons at n=1? : .

Page 57: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

57

When n= 2,(l = 0 to n-1) ml = l to - l ):

l = 0 and l = 1

When l = 0, ml = 0 2s orbitalWhen l = 1 ml = -1, 0, 1 giving three 2p orbitals:

2px 2py 2pz

Total orbitals:Total electrons:

Page 58: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

58

The P orbitals (energy level 2 and up)

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Page 59: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

59

When n=3 (l = 0 to n-1) ml = l to - l ):

l = 0 , 1 , 2

When l = 0, ml = 0 giving one 3s orbital

When l = 1 ml = -1, 0, 1 giving three 3p orbitals:

3px 3py 3pz

When l = 2 ml = -2,-1, 0, 1,2 giving 5 d orbitals

Total orbitals level 3:Total electrons level 3:

Page 60: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

60

When n=4

l = 0 , 1 , 2, 3 when l = 0 , 1 , 2 : 4s 4px 4py 4pz 4 d’s (5 of them)

when l =3 4f orbitals (7 of them)Total orbitals: Total electrons:

Page 61: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

61

electron spin quantum number:ms = +1/2 or - 1/2

Page 62: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

62

Pauli Exclusion Principle

In a given atom, no two electrons can have the same set of four quantum numbers (n, l, ml, ms).

Therefore, an orbital can hold only two electrons, and they must have opposite spins.

Page 63: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

63

Quantum Model

static.howstuffworks.com/ gif/atom-quantum.jpg

Page 64: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

64

Hydrogen orbitals are degenerate

All H orbitals with the same n have the same energy.

Page 65: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

65

Polyelectronic Atoms

• How does it work after Hydrogen?

• Shielding (e- repel, feel less attraction to +)

• Hydrogen orbitals: degenerate

• Hydrogenlike orbitals: NOT degenerate!

• Ens < Enp < End < Enf …etc.

• Why?

Page 66: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

66

Figure 7.20A Comparison of the Radial Probability Distributions of the 2s and 2p Orbitals

2p appears closer to nucleus? Less energy? No, look at small 2s hump. “2s penetrates to the nucleus” penetration effect

Page 67: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

67

Figure 7.21The Radial Probability Distribution for the 3s, 3p, and 3d Orbitalsso,

E3s<E3p<E3d

Page 68: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

68

History of the Periodic Table7.10

Dobereiner: triads

Newlands: octaves

Meyer / Mendeleev: arrangements by atomic masses.

Theory → prediction

Page 69: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

69

Figure 7.23Mendeleev’s Early Periodic Table,

Published in 1872

Prediction: Ga, Ge (see table 7.3, pg318 to see how

cool Mendeleev was)

Page 70: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

70

Aufbau Principle

As protons are added one by one to the nucleus to build up the elements, electrons are similarly added to these hydrogen-like orbitals.

“ an electron occupies the lowest energy orbital that can receive it”

Page 71: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

71

Hund’s Rule

The lowest energy configuration for an atom is the one having the maximum number of unpaired electrons allowed by the Pauli principle in a particular set of degenerate orbitals.

“in the p, d, f, orbitals, spread out before you pair up”

Page 72: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

72

The Electron Configurations in the Type of Orbital Occupied Last for the First 18

Elements

Note: elements in same group have number valence electrons (valence: The electrons in the outermost principle quantum level of The electrons in the outermost principle quantum level of

an atom.an atom. ((Core electron: other than valence)

Ex:Cl 1s22s22p63s23p5 or [Ne] 3s23p5

# valence = ?

Page 73: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

73

Figure 7.25Electron Configurations for Potassium Through Krypton

Why doe the 4s fill before the 3d? Penetration effect

Notice Cr, Cu columns.

Page 74: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

74

Figure 7.26The Orbitals Being Filled for Elements in Various Parts of the Periodic Table

After lathanum [Xe] 6s25d1 , go to lathanide series, fill the 4fs (fig 7.27: note anomalies)

After Actinium [Rn]7s26d1, fill actinide series with 5fs.

Page 75: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

75

Figure 7.27 The Periodic Table With Atomic Symbols, Atomic Numbers, and Partial Electron

Configurations

Page 76: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

76

Figure 7.36 Special Names for Groups in the Periodic Table

Main-group elements or

representative elements:

1A 2A 3A 4A 5A 6A

7A 8A or 1,2, 13-18

M-g e: each group has same #valence

Page 77: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

77

Broad Periodic Table Classifications

Representative Elements (main group): filling s and p orbitals (Na, Al, Ne, O)

Transition Elements: filling d orbitals (Fe, Co, Ni)

Lanthanide and Actinide Series (inner transition elements): filling 4f and 5f orbitals (Eu, Am, Es)

Page 78: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

78

Figure 7.30The Positions of the Elements

Considered in Sample Exercise 7.7

Page 79: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

79

Ionization Energy

The quantity of energy required to remove one electron from the gaseous atom or ion.

X(g) → X+(g) + e-

Page 80: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

80

Periodic Trends

First ionization energy: increases from left to right across a period (increase +, no shielding)decreases going down a group.

( increase n, more shielding)

Page 81: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

81

Figure 7.31The Values of First Ionization Energy for the

Elements in the First Six Periods

Page 82: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

82

Trends in Ionization Energies for the Representative Elements

Who has the highest IE? Who has the lowest? Do metals or nonmetals have higher IE? What does IE tell us about metal reactivity

Page 83: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

83

Periodic Trends: IE

Al(g) --> Al+ + e- I1= 580 kJ/mol

Al+(g) --> Al2+ + e- I2= 1815 kJ/mol

Al2+(g) --> Al3+ + e- I3= 2740 kJ/mol

Al3+(g) --> Al4+ + e- I4= 11,600 kJ/mol

Why the differences? Indicates something about the electron structure.

Page 84: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

84

Practice: 1s22s22p63s1

1s22s22p6

1s22s22p63s2

Which atom has the largest first I.E.?

Which one has the smallest second I.E.?

Explain.

Page 85: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

85

More Practice

IE increases across the period.

Check IE of P and S on pg 329. Explain the anomaly

Page 86: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

86

Electron Affinity

The energy change associated with the addition of an electron to a gaseous atom or ion.

X(g) + e X(g)If change is exothermic, then E.A. is

negative.

Page 87: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

87

Figure 7.33The Electronic Affinity Values for Atoms Among the First 20 Elements that Form

Stable, Isolated X- Ions

Page 88: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

88

Electron Affinity

Left to right mostly more neg kJ, more energy released. (note the missing elements: why C, but not N? write o.d. for both and t.t.y.n)Down a group, usually less neg kJ, less energy released. (see table 7.7. Notice anomaly. T.t.y.n.)

Page 89: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

89

E.A.

Who has more neg EA, metals or nonmetals?

What does this say about the reactivity of nonmetals?

Page 90: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

90

Radius trend

Data usually from distance between nuclei in a compound.

Page 91: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

91

Radius trend

Data usually from distance between nuclei in a compound.

Page 92: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

92

Figure 7.35Atomic Radii for Selected Atoms

Period trend?Group trend?

Why?

Page 93: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

93

Periodic Trends

Atomic Radii:decrease going from left to right across a period: increase + draws in valence.

increase going down a group: increase in orbital sizes with n.

Page 94: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

94

Alkali Metals Trends look at pg 335.

Note trends down the group in:

1. IE, radius

2. Density. Why?

3. mp/bp

Page 95: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

95

Alkali metals

Reaction with water. Write the balanced equation for Na(s) with water.

List alkali from most to least reactive (think I.E.) Cs > Rb > K > Na > LiBut in water,Li > K > Na , even though K loses electrons the easiest.

why? Hydration energy (see table 7.9) Li is small, higher charge density, better at attracting water.But there is more:

Page 96: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

96

Alkali metals

What we observe when they react with water:K > Na > Li

Look at mp. K and Na melt, increasing reaction rate.

Page 97: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

97

Waves

Waves have 3 primary characteristics:

1. Wavelength: distance between two peaks in a wave.

2. Frequency: number of waves per second that pass a given point in space.

3. Speed: speed of light is 3.00 108 m/s.

Page 98: Copyright©2000 by Houghton Mifflin Company. All rights reserved. 1 Ch 7 Atomic Structure

Copyright©2000 by Houghton Mifflin Company. All rights reserved.

98

Figure 7.1 The Nature of Waves