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Chapter 4 Electrons In Atoms

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Chapter 4 Electrons In Atoms. Chapter 4 Section 1 New Atomic Model. Objectives. Explain the mathematical relationship among speed, wavelength and frequency of electromagnetic radiation. Discuss the dual wave-particle nature of light. Describe the photoelectric effect. - PowerPoint PPT Presentation

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Page 1: Chapter 4 Electrons In Atoms

Chapter 4

ElectronsIn

Atoms

Page 2: Chapter 4 Electrons In Atoms

Chapter 4Section 1

New AtomicModel

Page 3: Chapter 4 Electrons In Atoms

ObjectivesExplain the mathematical relationship among speed, wavelength and frequency of electromagnetic radiation.

Discuss the dual wave-particle nature of light.

Describe the photoelectric effect.

Describe the Bohr model of the atom.

Page 4: Chapter 4 Electrons In Atoms
Page 5: Chapter 4 Electrons In Atoms

Rutherford Model

Was an improvement over previous models.

Helped to explain the positively charged nucleus.

It did not explain where the atom’s negatively charged electrons are located in space around the nucleus.

Page 6: Chapter 4 Electrons In Atoms
Page 7: Chapter 4 Electrons In Atoms
Page 8: Chapter 4 Electrons In Atoms

Light and Electrons

To begin to grasp the nature of electrons, examining the nature of light is necessary.

We will begin by first introducing some properties of light.

We will then see how these properties are related to the properties of the electron.

Page 9: Chapter 4 Electrons In Atoms

Properties of LightLight behaves as waves and has wave-like properties.

Electromagnetic Radiation – a form of energy that exhibits wavelike behavior as it travels through space.

Kinds of electromagnetic radiation include visible light, X rays, ultraviolet and infrared light, microwaves and radio waves.

Page 10: Chapter 4 Electrons In Atoms

Properties of Light

Electromagnetic Spectrum – includes all forms of electromagnetic radiation.

Page 11: Chapter 4 Electrons In Atoms

Electromagnetic Spectrum

Page 12: Chapter 4 Electrons In Atoms

Properties of Light

All forms of electromagnetic radiation move at a constant speed.

3.0 x 108 m/s

This is considered the speed of light.

Page 13: Chapter 4 Electrons In Atoms

A significant feature of waves is its repetitive nature.

Waves can be characterized by two features:

Wavelength (l) - the distance between corresponding points on adjacent waves.

The units for wavelength are meters, centimeter and nanometer depending on the form of electromagnetic radiation.

Page 14: Chapter 4 Electrons In Atoms

Wavelength

Page 15: Chapter 4 Electrons In Atoms

Frequency (n) – defined as the number of waves that pass a given point in a specific time, usually one second (hertz - Hz).

Page 16: Chapter 4 Electrons In Atoms

Frequency and wavelength are related by the following equation:

c = ln

c = speed of lightl = wavelengthn = frequency

Page 17: Chapter 4 Electrons In Atoms

c = ln

Because c is the same for all electromagnetic radiation, the product ln is a constant.

l is inversely proportional to n

As the wavelength (l) of light increase, its frequency (n) decreases, and vice versa.

Page 18: Chapter 4 Electrons In Atoms
Page 19: Chapter 4 Electrons In Atoms

The Photoelectric EffectPhotoelectric Effect – refers to the emission of electrons from a metal when light shines on the metal.

When light strikes a metal, no electrons were emitted if the light’s frequency was below a certain minimum.

Wave theory of light predicted any frequency of light could eject an electron.

Page 20: Chapter 4 Electrons In Atoms

Photoelectric Effect Experiment

Page 21: Chapter 4 Electrons In Atoms

The Photoelectric EffectThe explanation for the photoelectric effect is attributed to German physicist Max Planck.

Planck proposed that objects emit energy in small, specific amounts called quanta.

Quantum – the minimum quantity of energy that can be lost or gained by an atom.

E = hn

Page 22: Chapter 4 Electrons In Atoms

The Photoelectric Effect

E = hn

E = energyn = frequencyh = Planck’s constant – 6.626 x 10-34 J-s

Page 23: Chapter 4 Electrons In Atoms

The Photoelectric Effect

This energy can also be related to its wavelength by the following equations:

E = hn and c = ln

to get:

E = hc l

Page 24: Chapter 4 Electrons In Atoms

The Photoelectric EffectAlbert Einstein expanded on Planck’s theory by explaining that electromagnetic radiation has a dual wave-particle nature.

Light can also be thought of as a stream of particles.

Each particle of light carries a quantum of energy.

Page 25: Chapter 4 Electrons In Atoms

The Photoelectric EffectEinstein called these particles photons.

Photon – a particle of electromagnetic radiation having zero mass and carrying a quantum of energy.

The energy of a particular photon depends on the frequency of radiation:

Ephoton = hn

Page 26: Chapter 4 Electrons In Atoms

The Photoelectric EffectSummary:

Light has both wave properties (l and n) and particle (photons) properties.

In order for an electron to be ejected from a metal surface, the electron must be struck by a single photon possessing the minimum energy (frequency and wavelength).

Page 27: Chapter 4 Electrons In Atoms

Atom Line Emission Spectrum

Ground State – the lowest energy state of an atom.

Excited State – A state in which an atom has a higher energy than it has in its ground state.

Page 28: Chapter 4 Electrons In Atoms

When an excited atom returns to its ground state, it gives off energy that it gained in the form of electromagnetic radiation.

Ground state energy

Excited state energy

Electromagnetic radiationElectric current

E2

E1

Page 29: Chapter 4 Electrons In Atoms

When an electric current was passed through a tube containing hydrogen gas, a pink glow of light was emitted.

When this pink emitted light was passed through a prism, it was separated into a series of specific wavelengths of visible light.

The bands of light were part of what is known as hydrogen’s line-emission spectrum.

Page 30: Chapter 4 Electrons In Atoms

Hydrogen Atom Line Emission Spectrum

Page 31: Chapter 4 Electrons In Atoms

Why has the hydrogen atoms given off only specific wavelengths of light?

Scientists had expected to observe the emission of a continuous range of wavelengths of electromagnetic radiation, that is a continuous spectrum.

Attempts to explain this observation led to a new theory of the atom call Quantum Theory.

Page 32: Chapter 4 Electrons In Atoms

Whenever an excited hydrogen atom falls back from an excited state to its ground state, it emits a photon of radiation.

The energy of this photon is: Ephoton = hn

This energy is equal to the difference in energy between the atom’s excited state (E2) and its ground state (E1).

E2 – E1 = Ephoton = hn

Page 33: Chapter 4 Electrons In Atoms

Energy difference between ground and excited state

Page 34: Chapter 4 Electrons In Atoms

The fact that hydrogen atoms emit only specific wavelengths of light indicated that the energy differences between the atom’s energy states were fixed.

This suggested that the electron of a hydrogen atom exists only in very specific energy states.

Page 35: Chapter 4 Electrons In Atoms

Bohr Model of the Hydrogen Atom

Niels Bohr, a Danish physicist explained the line spectrum of hydrogen in 1913.

His model combined the concepts of Planck and Einstein. Ephoton = hn

Bohr assumed the atom contained a nucleus and that the electrons circled the nucleus in circular orbits.

Page 36: Chapter 4 Electrons In Atoms
Page 37: Chapter 4 Electrons In Atoms

Bohr Model The three postulates of the Bohr model:

1) The electron in the hydrogen atom may only occupy orbits of certain radii that correspond to certain discrete energies.

2) While an electron is in an allowed energy orbit, it does not radiate energy and it remains in that orbit without crashing into the nucleus.

Page 38: Chapter 4 Electrons In Atoms

Bohr Model 3) An electron may move from one energy state to another by absorbing or releasing energy. The energy needed is the difference between one energy level and another and is equal to a photon,

Ephoton = hn

Page 39: Chapter 4 Electrons In Atoms

+e-

absorb energy

release energyground state

excited state

Bohr Model

Page 40: Chapter 4 Electrons In Atoms

Bohr Model

Page 41: Chapter 4 Electrons In Atoms

Bohr Model Ephoton = hn

By knowing the wavelengths from the hydrogen atom line emission spectrum, Bohr could solve for the energy of the photon using the above equation.

This energy (Ephoton) represents the difference in energy between the different orbits of the hydrogen atom.

Page 42: Chapter 4 Electrons In Atoms

Bohr Model While the Bohr model works well for hydrogen, it does have its limitations:

1) It did not work well with atoms with more than one electron.

2) It does not account for electron-electron repulsions.

3) Additional electron-nucleus interactions present problems.

Page 43: Chapter 4 Electrons In Atoms

Classwork

Section Review, page 97

Questions 1-5

Page 44: Chapter 4 Electrons In Atoms

Homework

Page 118 -119

Questions 1, 6, 9, 31, 33

Collected for a grade

Page 45: Chapter 4 Electrons In Atoms

Lab Demo

light experiments with various gases

Page 46: Chapter 4 Electrons In Atoms

Chapter 4Section 3

Electron Configurations

Page 47: Chapter 4 Electrons In Atoms

ObjectivesList the atomic orbitals of an atom.

List the total number of electrons needed to fully occupy each main energy level.

State the Aufbau principle, the Pauli Exclusion principle and Hund’s rule.

Write the electron configuration for any element.

Page 48: Chapter 4 Electrons In Atoms
Page 49: Chapter 4 Electrons In Atoms

Atomic Orbitals

Quantum Mechanical Model A more complex, highly mathematical model was developed to explain observations of atoms containing more than one electron.

This model works for all the elements and not just for hydrogen as in the Bohr model.

Page 50: Chapter 4 Electrons In Atoms

Electronic Configuration – describes the arrangement of electrons in an atom.

Because atoms of different elements have different number of electrons, a distinct electron configuration exists for each element.

Page 51: Chapter 4 Electrons In Atoms

The electrons will assume arrangements that have the lowest possible energies.

Ground State Configuration – the lowest energy arrangement of the electrons for each element.

Page 52: Chapter 4 Electrons In Atoms

Bohr Model – the orbit of the electron was circular around the nucleus.

In the quantum mechanical model the simple circular orbit was replaced with 3D orbitals (electron clouds) of various shapes in which an electron is likely to be.

Atomic Orbitals

Page 53: Chapter 4 Electrons In Atoms

Atomic Orbitals

There are four main atomic orbitals which describe the electron configuration of the elements:

S orbital - spherical shapeP orbital – dumbbell shapeD orbital – clover shapeF orbital – Too complex to discuss.

Page 54: Chapter 4 Electrons In Atoms

Periodic Table with Orbitals

Page 55: Chapter 4 Electrons In Atoms

S orbital - spherical shape

Page 56: Chapter 4 Electrons In Atoms

P orbital – dumbbell shape

Page 57: Chapter 4 Electrons In Atoms

D orbital – clover shape

Page 58: Chapter 4 Electrons In Atoms

s, p and d orbitals

Page 59: Chapter 4 Electrons In Atoms

Atomic Orbitals

Energy levels of the three orbitals of interest: S orbital – lowest energyP orbital – slightly higher in energyD orbital – higher in energy than P orbital

Page 60: Chapter 4 Electrons In Atoms

Electron Configuration RulesThe number of electrons in an atom is the same as the number of protons.

So the periodic table will be of real value in determining electron configurations.

To build up electron configurations for any particular atom, first energy levels of the orbitals are determined.

Page 61: Chapter 4 Electrons In Atoms

Nucleus

1s

2s

2p

3s

3p

4s

4p

3d

Energy

Page 62: Chapter 4 Electrons In Atoms

Electron Configuration RulesThe electrons are added to the orbitals one by one according to three basic rules:

1) Aufbau Principle – An electron occupies the lowest energy orbital that can receive it.

The orbital with the lowest energy is the 1s orbital. The one electron of hydrogen goes in this orbital.

Page 63: Chapter 4 Electrons In Atoms

Electron Configuration RulesThe 2s orbital is the next highest in energy, then the 2p orbitals.

The numbers 1,2,3 etc. refer to the row of the periodic table the atom is located in.

As can be seen on the diagram there is only 1-s orbital, 3-p orbitals and 5-d orbitals.

These refer to their orientation in space.

Page 64: Chapter 4 Electrons In Atoms

Electron Configuration Rules

Note on the energy level diagram that the 4s orbital is lower in energy than the 3d orbital.

Therefore, the 4s orbital is filled before any electrons enter the 3d orbitals.

Page 65: Chapter 4 Electrons In Atoms

1s

2s

3s

4s

2p

3p

4p

3d

4d

Aufbau Principle

Page 66: Chapter 4 Electrons In Atoms

Electron Configuration Rules2) Pauli Exclusion Principle – no more than two electrons may be present in an orbital and their spins must be paired.

This rule basically states no two atoms can have the same electron configurations.

Page 67: Chapter 4 Electrons In Atoms

Electron Configuration Rules3) Hund’s Rule – orbitals of equal energy are each occupied by one electron before any orbital is occupied by a second electron. The spins of these electrons must be opposite.

This rule is because similarly charged electrons want to be as far away as possible.

2p orbital

Page 68: Chapter 4 Electrons In Atoms

Energy Level Diagram for Oxygen

nucleus

1s

2s

2p

3s

3penergy

Energy level diagram for oxygen

Page 69: Chapter 4 Electrons In Atoms

Electronic Configurations

Electronic configurations are important in chemistry:

1) To predict what type of bonding will occur with a particular element and which electrons are being used in the bonding.

2) Helps explain the properties of elements.

Page 70: Chapter 4 Electrons In Atoms

Nucleus

1s

2s

2p

3s

3p

4s

4p

3d

Energy

Page 71: Chapter 4 Electrons In Atoms

While energy level diagrams are very useful they are bulky to work with.

Electron configuration notations are simpler and give the same information.

Electronic Configurations

Page 72: Chapter 4 Electrons In Atoms

Electronic Configurations

Electron configuration notations eliminate the lines and arrows of the diagrams.

Instead the number of electrons in an energy level is shown by adding a superscript to the energy level designation.

Example: hydrogen - 1S1

Page 73: Chapter 4 Electrons In Atoms

Electronic Configurations

Example: hydrogen - 1S1

The large 1 indicates hydrogen is in the first row of the periodic table. First energy level.

The S indicates the electron is in the s orbital.

The superscript 1 indicates that there is one electron in the 1S orbital.

Page 74: Chapter 4 Electrons In Atoms

Example: helium - 1S2

Electronic Configurations

The superscript 2 indicates that there are two electrons in the 1S orbital.

Problem: Give the electron configuration of boron and explain how the electrons are arranged.

Page 75: Chapter 4 Electrons In Atoms

Elements of the Second Period

In the first period elements, hydrogen and helium, electrons occupy the first energy level – 1s.

After the 1s orbital is filled, the next electron occupies the 2s orbital – Aufbau principle.

Lithium has an electron configuration of 1s22s1

Page 76: Chapter 4 Electrons In Atoms

1s

2s

3s

4s

2p

3p

4p

3d

4d

Aufbau Principle

Page 77: Chapter 4 Electrons In Atoms

Classwork

Page 107 - Problems 1 – 2

Homework

Energy Level Diagram Worksheet

Page 78: Chapter 4 Electrons In Atoms

Elements of the Second PeriodHighest Occupied Level – is the electron containing main energy level with the largest number.

In the case of lithium that is the 2s level.

Inner Shell Electrons – The electrons which are in the levels below the highest occupied level.

In the case of lithium that is the 1s level.

Page 79: Chapter 4 Electrons In Atoms

Elements of the Second Period

Page 80: Chapter 4 Electrons In Atoms

Elements of the Second PeriodWhen you get to neon (Ne) all the 2s and 2p orbitals are full.

Octet Rule – when all of the sublevels (s and p orbitals) of the highest occupied level is filled with eight electrons.

All the elements in the last column of the periodic table obey the octet rule.

Page 81: Chapter 4 Electrons In Atoms

Noble Gases

Neon is a member of the Group 18 elements (last column).

These elements include neon, argon, krypton, xenon and radon).

These elements are known as the noble gases.

Page 82: Chapter 4 Electrons In Atoms

Elements of the Third Period

Page 83: Chapter 4 Electrons In Atoms

Elements of the Third PeriodTo simplify sodium’s notation, the symbol for neon, enclosed in brackets, is used to represent the complete neon configuration.

[Ne] = 1s22s22p6

So the electron configuration for sodium can be written:

[Ne]3s1

This is the noble gas configuration

Page 84: Chapter 4 Electrons In Atoms

Elements of the Fourth PeriodWith the 4s level full (calcium), the 4p and 3d sublevels are next available.

Referring to the Aufbau diagram of energy levels, the 3d sublevel is lower in energy than the 4p sublevel.

There are five 3d orbitals that hold a total of 10 electrons. Elements range from Sc to Zn.

Page 85: Chapter 4 Electrons In Atoms

Elements of the Fourth Period

Page 86: Chapter 4 Electrons In Atoms

Elements of the Fifth Period

Elements in the fifth period start with the 5s orbital.

5s 4d 5p

Page 87: Chapter 4 Electrons In Atoms

Periodic Table with Orbitals

Page 88: Chapter 4 Electrons In Atoms

Problem1) Write the energy level congiguration, the

electron configuration and noble gas configuration for iron (Fe).

2) How many electron containing orbitals are in an atom of iron? How many are filled? How many unpaired electrons are there in an atom of iron?

Page 89: Chapter 4 Electrons In Atoms

Classwork

Page 115

Practice Problems 1 – 3

Page 116

Practice Problem 1

Page 90: Chapter 4 Electrons In Atoms

Homework

Worksheet

Electron Configuration/Noble Gas Configuration