Chapter 6 Electronic Structure of Atoms - Yolaholcombslab.yolasite.com/resources/WCU Inorganic...

26
6/3/2012 1 Electronic Structure of Atoms © 2009, Prentice-Hall, Inc. Chapter 6 Electronic Structure of Atoms Chemistry, The Central Science, 11th edition Theodore L. Brown; H. Eugene LeMay, Jr.; and Bruce E. Bursten John D. Bookstaver St. Charles Community College Cottleville, MO Electronic Structure of Atoms © 2009, Prentice-Hall, Inc. Chapter 6 Problems Problems 13, 15, 21, 33, 35, 47, 51, 53, 63, 65, 67, 71, 73 Electronic Structure of Atoms © 2009, Prentice-Hall, Inc. Electronic Structure of Atoms To understand the electronic structure of atoms, one must understand the nature of electromagnetic radiation.

Transcript of Chapter 6 Electronic Structure of Atoms - Yolaholcombslab.yolasite.com/resources/WCU Inorganic...

6/3/2012

1

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Chapter 6

Electronic Structure

of Atoms

Chemistry, The Central Science, 11th edition

Theodore L. Brown; H. Eugene LeMay, Jr.;

and Bruce E. Bursten

John D. Bookstaver

St. Charles Community College

Cottleville, MO

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Chapter 6 Problems

• Problems 13, 15, 21, 33, 35, 47, 51, 53,

63, 65, 67, 71, 73

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Electronic Structure of Atoms

• To understand the electronic structure

of atoms, one must understand the

nature of electromagnetic radiation.

6/3/2012

2

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Electromagnetic Radiation

• Electric and magnetic

fields propagate as waves

through empty space or

through a medium.

• A wave transmits energy.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Waves

• The distance between corresponding points

on adjacent waves is the wavelength ().

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Waves

• The number of waves

passing a given point per

unit of time is the

frequency ().

• For waves traveling at

the same velocity, the

longer the wavelength,

the smaller the

frequency.

6/3/2012

3

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

EM Radiation

Low

High

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

• Waves have a frequency • Use the Greek letter “nu”, , for frequency,

and units are “cycles per sec” • All radiation: • = c • c = velocity of light = 3.00 x 108 m/sec

• Long wavelength --> small frequency

• Short wavelength --> high frequency

= c/λ

Electromagnetic Radiation

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Red light has = 700 nm. Calculate the

frequency. = c/λ

Freq = 3.00 x 108 m/s

7.00 x 10-7 m 4.29 x 1014 sec-1

700 nm • 1 x 10 -9 m

1 nm = 7.00 x 10 -7 m

Electromagnetic Radiation

6/3/2012

4

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Electromagnetic Radiation

• All electromagnetic radiation travels at the same velocity: the speed of light (c),

3.00 108 m/s.

• Therefore,

c =

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Electromagnetic Spectrum

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Constructive and Destructive

Interference

6/3/2012

5

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Nature of Energy

• The wave nature of light

does not explain how

an object can glow

when its temperature

increases.

• Max Planck explained it

by assuming that

energy comes in

packets called quanta.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Black Body Radiation

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Quantum Theory Blackbody Radiation:

Max Planck, 1900

є = h Energy, like matter, is discontinuous.

6/3/2012

6

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Long wavelength -->

small frequency

low energy

Short wavelength -->

high frequency

high energy

Electromagnetic Radiation

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Light with a short (large ) has a large E.

Light with large (small ) has a small E.

E = h •

Quantization of Energy

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Photoelectric Effect

• Heinrich Hertz, 1888

– Light striking the surface of certain metals causes ejection of electrons.

– > o

threshold frequency

I Albert Einstein 1905

6/3/2012

7

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Nature of Energy

• Einstein used Planck’s

assumption to explain the

photoelectric effect.

• He concluded that energy is

proportional to frequency:

E = h

where h is Planck’s

constant, 6.626 10−34 J-s.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Nature of Energy

• Therefore, if one knows the

wavelength of light, one

can calculate the energy in

one photon, or packet, of

that light:

c =

E = h

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Sample Exercise 6.3 Energy of a Photon

Calculate the energy of one photon of yellow light with a wavelength of 589 nm.

We can use Equation 6.1 to convert the

wavelength to frequency:

We can then use Equation 6.3 to calculate

energy:

Solve: The frequency, v, is calculated from the

given wavelength.:

:

Use the frequency and Planck’s constant

to calculate the energy of the photon.

Comment: If one photon of radiant energy

supplies 3.37 × 10–19 J, then one mole

of these photons will supply

6/3/2012

8

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Nature of Energy

Another mystery in

the early 20th

century involved the

emission spectra

observed from

energy emitted by

atoms and

molecules.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

9-2 Atomic Spectra

(a) (b) (c) (d) (e)

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Atomic Spectra

Helium

Hydrogen

6/3/2012

9

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Nature of Energy

• For atoms and

molecules one does

not observe a

continuous spectrum,

as one gets from a

white light source.

• Only a line spectrum of

discrete wavelengths

is observed.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Nature of Energy

• Niels Bohr adopted Planck’s

assumption and explained

these phenomena in this

way:

1. Electrons in an atom can only

occupy certain orbits

(corresponding to certain

energies).

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Nature of Energy

• Niels Bohr adopted Planck’s

assumption and explained

these phenomena in this

way:

2. Electrons in permitted orbits

have specific, “allowed”

energies; these energies will

not be radiated from the atom.

6/3/2012

10

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Nature of Energy

• Niels Bohr adopted Planck’s

assumption and explained

these phenomena in this

way:

3. Energy is only absorbed or

emitted in such a way as to

move an electron from one

“allowed” energy state to

another; the energy is defined

by

E = h

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

8-4 The Bohr Atom

E = -RH

n2

RH = 2.179 10-18 J

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Energy-Level Diagram

ΔE = Ef – Ei = -RH

nf2

-RH

ni2

= RH ( ni

2

1

nf2

– 1 ) = h = hc/λ

6/3/2012

11

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Nature of Energy

The energy absorbed or emitted from the process of electron promotion or demotion can be calculated by the equation:

E = RH ( ) 1

ni2

1

nf2

-

where RH is the Rydberg

constant, 2.18 10−18 J, and ni

and nf are the initial and final

energy levels of the electron.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Sample Exercise 6.4 Electronic Transitions in the Hydrogen Atom

Using Figure 6.14, predict which of the following electronic

transitions produces the spectral line having the longest

wavelength: n = 2 to n = 1, n = 3 to n = 2, or n = 4 to n = 3.

Solution

The longest wavelength will be associated with the lowest

frequency.

According to Planck’s equation, E = hv, the lowest frequency

is associated with the lowest energy.

In Figure 6.14 the shortest vertical line represents the smallest

energy change. Thus, the n = 4 to n = 3 transition produces the

longest wavelength (lowest frequency) line.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

6/3/2012

12

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Emission and Absorption Spectroscopy

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Quantum Mechanical View of Electron

• Bohr’s Model only worked for a one-

electron atom.

• Scientists began to view the electron as

a wave.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Two Ideas Leading to a New

Quantum Mechanics

• Wave-Particle Duality

– Einstein suggested particle-like

properties of light could explain the

photoelectric effect.

– Diffraction patterns suggest photons

are wave-like.

• deBroglie, 1924

– Small particles of matter may at

times display wavelike properties. Louis de Broglie

Nobel Prize 1918

6/3/2012

13

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Wave Nature of Matter

• Louis de Broglie posited that if light can

have material properties, matter should

exhibit wave properties.

• He demonstrated that the relationship

between mass and wavelength was

= h

mv

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

The Uncertainty Principle

• Heisenberg showed that the more precisely

the momentum of a particle is known, the less

precisely is its position known:

• In many cases, our uncertainty of the

whereabouts of an electron is greater than the

size of the atom itself!

(x) (mv) h

4

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Quantum Mechanics

• Erwin Schrödinger

developed a

mathematical treatment

into which both the

wave and particle nature

of matter could be

incorporated.

• It is known as quantum

mechanics.

6/3/2012

14

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Quantum Mechanics

• The wave equation is

designated with a lower

case Greek psi ().

• The square of the wave

equation, 2, gives a

probability density map of

where an electron has a

certain statistical likelihood

of being at any given instant

in time.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Wave Functions

• ψ, psi, the wave function.

– Should correspond to a

standing wave within the

boundary of the system

being described.

• Particle in a box.

L

xnsin

L

Slide 28 of 50 General Chemistry: Chapter 8 Prentice-Hall © 2007

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Probability of Finding an Electron

6/3/2012

15

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Wave Functions for Hydrogen

• Schrödinger, 1927 Eψ = H ψ

– H (x,y,z) or H (r,θ,φ)

ψ(r,θ,φ) = R(r) Y(θ,φ)

R(r) is the radial wave function.

Y(θ,φ) is the angular wave function.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Quantum Numbers

• Solving the wave equation gives a set of

wave functions, or orbitals, and their

corresponding energies.

• Each orbital describes a spatial

distribution of electron density.

• An orbital is described by a set of three

quantum numbers.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Principle Shells and Subshells • Principle electronic shell, n = 1, 2, 3…

• Angular momentum quantum number, l = 0, 1, 2…(n-1)

l = 0, s

l = 1, p

l = 2, d

l = 3, f

• Magnetic quantum number, ml= - l …-2, -1, 0,

1, 2…+l

6/3/2012

16

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Principal Quantum Number (n)

• The principal quantum number, n,

describes the energy level on which the

orbital resides.

• The values of n are integers ≥ 1.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Angular Momentum Quantum

Number (l)

• This quantum number defines the

shape of the orbital.

• Allowed values of l are integers ranging

from 0 to n − 1.

• We use letter designations to

communicate the different values of l

and, therefore, the shapes and types of

orbitals.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Angular Momentum Quantum

Number (l)

Value of l 0 1 2 3

Type of orbital s p d f

6/3/2012

17

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Magnetic Quantum Number (ml)

• The magnetic quantum number describes the three-dimensional orientation of the orbital.

• Allowed values of ml are integers ranging from -l to l:

−l ≤ ml ≤ l.

• Therefore, on any given energy level, there can be up to 1 s orbital, 3 p orbitals, 5 d orbitals, 7 f orbitals, etc.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Magnetic Quantum Number (ml)

• Orbitals with the same value of n form a shell.

• Different orbital types within a shell are

subshells.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

s Orbitals

• The value of l for s

orbitals is 0.

• They are spherical in

shape.

• The radius of the

sphere increases with

the value of n.

6/3/2012

18

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

s Orbitals

Observing a graph of probabilities of finding an electron versus distance from the nucleus, we see that s orbitals possess n−1 nodes, or regions where there is 0 probability of finding an electron.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

p Orbitals

• The value of l for p orbitals is 1.

• They have two lobes with a node between

them.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

d Orbitals

• The value of l for a

d orbital is 2.

• Four of the five d

orbitals have 4

lobes; the other

resembles a p

orbital with a

doughnut around

the center.

6/3/2012

19

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Energies of Orbitals

• For a one-electron

hydrogen atom,

orbitals on the same

energy level have

the same energy.

• That is, they are

degenerate.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Energies of Orbitals

• As the number of electrons increases, though, so does the repulsion between them.

• Therefore, in many-electron atoms, orbitals on the same energy level are no longer degenerate.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Spin Quantum Number, ms

• In the 1920s, it was

discovered that two

electrons in the same

orbital do not have

exactly the same energy.

• The “spin” of an electron

describes its magnetic

field, which affects its

energy.

6/3/2012

20

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Spin Quantum Number, ms

• This led to a fourth

quantum number, the

spin quantum number,

ms.

• The spin quantum

number has only 2

allowed values: +1/2

and −1/2.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Pauli Exclusion Principle

• No two electrons in the

same atom can have

exactly the same energy.

• Therefore, no two

electrons in the same

atom can have identical

sets of quantum

numbers.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Electron Configurations

• This shows the

distribution of all

electrons in an atom.

• Each component

consists of

– A number denoting the

energy level,

6/3/2012

21

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Electron Configurations

• This shows the

distribution of all

electrons in an atom

• Each component

consists of

– A number denoting the

energy level,

– A letter denoting the type

of orbital,

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Electron Configurations

• This shows the

distribution of all

electrons in an atom.

• Each component

consists of

– A number denoting the

energy level,

– A letter denoting the type

of orbital,

– A superscript denoting

the number of electrons

in those orbitals.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Orbital Diagrams

• Each box in the

diagram represents

one orbital.

• Half-arrows represent

the electrons.

• The direction of the

arrow represents the

relative spin of the

electron.

6/3/2012

22

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Hund’s Rule

“For degenerate

orbitals, the lowest

energy is attained

when the number of

electrons with the

same spin is

maximized.”

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Electron Configurations

• Aufbau process.

– Build up and minimize energy.

• Pauli exclusion principle.

– No two electrons can have all four

quantum numbers alike.

• Hund’s rule.

– Degenerate orbitals are occupied singly

first.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Orbital Filling

6/3/2012

23

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Aufbau Process and Hunds Rule

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Filling p Orbitals

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Periodic Table

• We fill orbitals in

increasing order of

energy.

• Different blocks on the

periodic table (shaded

in different colors in

this chart) correspond

to different types of

orbitals.

6/3/2012

24

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Some Anomalies

Some

irregularities

occur when there

are enough

electrons to half-

fill s and d

orbitals on a

given row.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Some Anomalies

For instance, the

electron

configuration for

chromium is

[Ar] 4s1 3d5

rather than the

expected

[Ar] 4s2 3d4.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Some Anomalies

For instance, the

electron

configuration for

copper is

[Ar] 4s1 3d10

rather than the

expected

[Ar] 4s2 3d9.

6/3/2012

25

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Some Anomalies

• This occurs

because the 4s

and 3d orbitals

are very close in

energy.

• These anomalies

occur in f-block

atoms, as well.

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Filling the d Orbitals

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

6/3/2012

26

Electronic

Structure

of Atoms

© 2009, Prentice-Hall, Inc.

Electron Configurations and the Periodic Table