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CH1120 Electronic Structure

of the Atom

Quantum Mechanics The Behavior of the Very Small

Electrons are incredibly small.

Electron behavior determines much of the behavior of atoms.

Directly observing electrons in the atom is impossible, the electron is so small that

observing it changes its behavior.

The Electromagnetic Spectrum

Light is a form of electromagnetic radiation composed of perpendicular oscillating waves, one for the electric field and one for the magnetic field.

Characterizing Waves

The frequency (ν) is the number of waves that pass a point in a given period of time.

The number of waves = number of cycles units are hertz (Hz) or cycles/s = s−1

1 Hz = 1 s−1 or 1/s

The total energy is proportional to the amplitude of the waves and the frequency.

The larger the amplitude, the more force it has. The more frequently the waves strike, the more total force .

low frequency long wavelength

higher frequency

higher frequency short wavelength

low amplitude

higher amplitude

higher amplitude

Characterizing Waves

Increasing energy

The field of quantum mechanics began with the studies of physicists in the early the 20th century.

Max Planck (1918) Albert Einstein (1921)

Neils Bohr (1922)Arthur Compton (1927)Louis de Broglie (1929)

Werner Heisenberg (1932)P. A. M. Dirac (1933)

Erwin Schrödinger (1933)

The Beginnings of Quantum Mechanics

The Relationship Between Wavelength and Frequency

The shorter the wavelength, the more frequently waves pass, and the higher the frequency.

Wavelength and frequency of electromagnetic waves are inversely proportional.

Because the speed of light is constant (3.00 x 108 m/sec), if we know wavelength we can find the frequency, and

vice versa.

ν =cλ

ν ∝ 1 λ

The proportionality constant is c, the speed

of light.

The Relationship Between Wavelength and Frequency

c = 3 x 108 m/s

1. Calculate the frequency (in MHz) of a radio signal with a wavelength of 2.98 m.

ν = 3.00 x 108 m/s2.98 m

= 1.01 x 108 s-1

= 1.01 x 108 Hz

1.00 MHz106 Hz

1.01 x 108 Hz x = 101 MHz

2. Calculate the wavelength of red light with a frequency of 4.62 x 1014 s−1 .

=

3.00 x 108 m/s4.62 x 1014 /s = 6.49 x 10-7 m

6.49 x 10-7 m x 1 nm1 x 10-9 m = 6.49 x 102 nm

RedOrangeYellowGreenBlueViolet

The Electromagnetic Spectrum

The Electromagnetic Spectrum

Energy Increases

Shorter wavelengths of electromagnetic radiation have more energy than longer wavelengths:

Radiowaves have the lowest energy. Gamma rays have the highest energy.

3. Order the following types of electromagnetic radiation:microwaves, gamma rays, green light, red light, ultraviolet light.

By wavelength (short to long)

By frequency (low to high)

By energy (least to most)

gamma < UV < green < red < microwaves

microwaves < red < green < UV < gamma

microwaves < red < green < UV < gamma

White Light Produces a “Continuous” Spectrum

Atomic Spectra

When atoms or molecules absorb energy, that energy is often released as light energy.

When that emitted light is passed through a prism, a pattern of particular wavelengths of

light is seen that is unique to that type of atom or molecule – the pattern is called an

emission spectrum.

non-continuous can be used to identify the material

Emission Spectrum

Red line 𝛌 = 656.3 nm

Green line 𝛌 = 486 nm

Blue line 𝛌 = 434 nm

Violet line 𝛌 = 410.1 nm

Identifying Elements with Flame Tests

Na K Li Ba

Rutherford’s Nuclear Model

The atom contains a tiny dense center called the nucleus.

The nucleus is essentially the entire mass of the atom.

The nucleus is positively charged.

The positive charge balances the negative charge of the electrons.

The electrons move around in the empty space of the atom surrounding the nucleus.

Problems with Rutherford’s Nuclear Model of the Atom

Electrons are moving charged particles.

Moving charged particles give off energy.

Therefore electrons should constantly be giving off energy.

The electrons should lose energy, crash into the

nucleus, and the atom should collapse!!

The Bohr Model of the AtomNeils Bohr (1885–1962)

The energy of the atom is quantized.

The amount of energy in the atom is related to the electron’s position in the atom.

Quantized means that the atom could only have very specific amounts of energy.

Bohr correlated these allowed energy levels with allowed radii of electron orbits.

Bohr Model The energy of each Bohr orbit, specified by a quantum number, n = 1, 2, 3 is fixed, or quantized.

It is impossible for an electron to exist between orbits in the Bohr model.

Bohr orbits are like steps of a ladder, each at a specific distance from the nucleus.

Bohr’s Model

The electrons travel in orbits that are at a fixed distance from the nucleus (stationary states).

The energy of the electron is proportional to the distance the orbit was from the nucleus.

Electrons emit and absorb radiation when they move between orbits.

Emitted radiation is a photon of light. The distance between the orbits determines the

energy of the photon of light produced.

Bohr’s Model

n=1

n=2

n=3 n=4 n=5

When an atom

absorbs energy, an electron is excited to a

higher-energy orbit.

The electron relaxes to a

lower energy level, emitting a photon of light.

Energy is absorbed !!

Energy is emitted !!

Excitation and Emission

Emission vs. Absorption Spectra

Spectra of Mercury

Emission Spectrum

Red line 𝛌 = 656.3 nm

Green line 𝛌 = 486 nm

Blue line 𝛌 = 434 nm

Violet line 𝛌 = 410.1 nm

1

The energy of photons is related to wavelength by another equation:

ℏ = 6.626 x 10-34 Jᐧs

Bohr’s equations related energy of photons to

basic energy shells (n):

n=1

n=2

n=3 n=4 n=5 n=6

Red line 𝛌 = 656.3 nm

Green line 𝛌 = 486 nm

Blue line 𝛌 = 434 nm

Violet line 𝛌 = 410.1 nm

Balmer Series

The Hydrogen Spectrum

Bohr Model The Bohr model also showed that each “principal” energy level could hold a maximum number of electrons.

This explains the increasing length of the “rows” of the

periodic table.

Bohr Model ---> Increasing Length of Periods

Bohr Model ---> Increasing Length of Periods

28

1832

Behavior of main-group elements can be explained in terms of “outer” electrons.

I II III IV V VI VII VIII

adding electrons

The Bohr Model: Atoms with Orbits

The great success of the Bohr model of the atom was thatit predicted the lines of the hydrogen emission spectrum.

However, it failed to predict the emission spectra of other elements that contained more than one electron.

For this and other reasons, the Bohr model was replaced with a more sophisticated model called the quantum-mechanical or

wave-mechanical model.  

In the quantum-mechanical model, electrons do not behave like particles flying through space.

We cannot, in general, describe their exact paths.

An orbital is a probability map (a mathematical

model)that shows where the electron is likely to be found when the atom is probed. It does not represent an exact path

that an electron takes.

Electrons reside in principal energy levels which are subdivided into energy sublevels.

The principal energy levels (1-7) can “theoretically” contain 2,8,18,32,50,72, and 98 electrons each.

The Quantum-Mechanical Model: Atoms with “Orbitals”

The number of subshells in a given principal shell is equal to the value of n.

Principal Energy Levels are Divided Into Subshells

Subshells Hold Different Numbers of Electrons

Principal quantum number

Electrons in primary

shell

Electrons in subshells}

Electrons in subshells}

Electrons in subshells}

Electrons in subshells}

n=4

n=3

n=2

n=1

Primary energy shells

Principal Energy Levels

f d p s

d p s

p s

s

n=4

n=3

n=2

n=1

Primary energy shells

Energy subshells

Energy

1s

2s

2p

3s

3p

3d

4s

4p

4d

4f

5s

5p

5d

5f

6s

6p

6d

“Degenerate” Orbital Energies

Energy

1s

2s

2p

3s

3p

3d 4s

4p

4d

4f

5s

5p

5d

5f

6s

6p

6d 7s

“Real” Orbital Energies

Bohr Model (shells)

n=1

n=2

n=3n=4

Modified Bohr Model (subshells)

1s

2s

2p3s3p4s3d4p4d4f

Increasing Energy

5s lower in energy than 4d

6s lower in energy than 4f

4s lower in energy than 3d

]

Filling the Orbitals with ElectronsEnergy levels and sublevels fill from lowest energy to high.

s → p → d →f Aufbau Principle

Orbitals that are in the same sublevel have the same energy

No more than two electrons per orbital

Pauli Exclusion Principle

When filling orbitals that have the same energy, place one electron in each before completing pairs.

Hund’s Rule

Electron Configuration & the Periodic Table

s

f

dp

1 2 3 4 5 6 7

Electron Configuration & the Periodic Table

s

f

dp

1 2 3 4 5 6 7

Electron Configuration & the Periodic Table

s

f

d

p

1 2 3 4 5 6 7

Shell being filled = (period number-1)

Shell being filled = (period number-2)

Shell being filled = period number

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Electron Configuration & the Periodic Table

s

f

d p

1 2 3 4 5 6 7

Shell being filled = period number

Shell being filled = (period number-1)

Shell being filled = (period number-2)

He K Pd Be Co Si Pt U

1s 4s 4d 2s 3d 3p 5d 5f

4. What is the highest energy sublevel being filled for each of the following atoms ?

Electron Configuration & the Periodic Table

s

f

d

p

1 2 3 4 5 6 7

118