principles of chemistry i chem 1211 chapter 7 dr. augustine ofori agyeman assistant professor of...

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PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state university

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Page 1: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

PRINCIPLES OF CHEMISTRY I

CHEM 1211

CHAPTER 7

DR. AUGUSTINE OFORI AGYEMANAssistant professor of chemistryDepartment of natural sciences

Clayton state university

Page 2: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

CHAPTER 7

ELECTRONIC STRUCTURE OF ATOMS

Page 3: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

ELECTROMAGNETIC RADIATION

- Also known as radiant heat or radiant energy

- One of the ways by which energy travels through space

- Consists of electric and magnetic fields which are perpendicularto each other and to the direction of propagation

Examples

heat energy in microwaveslight from the sun

X-ray radio waves

Page 4: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

- Light properties is a key concept for understandingelectronic structure

- Studies of atomic structure has come from observations of the interaction of visible light and matter

- To study the properties of electrons in atoms, it is helpful to understand waves and electromagnetic radiation

ELECTROMAGNETIC RADIATION

Page 5: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Three Characteristics of Waves

Wavelength (λ) - Distance for a wave to go through a complete cycle

(distance between two consecutive peaks or troughs in a wave)

Frequency (ν)- The number of waves (cycles) per second that pass

a given point in space

Speed (c)- All waves travel at the speed of light in vacuum (3.00 x 108 m/s)

ELECTROMAGNETIC RADIATION

Page 6: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

one second

λ1

λ3

λ2

ν1 = 4 cycles/second

ν2 = 8 cycles/second

ν3 = 16 cycles/second

amplitude

peak

trough

ELECTROMAGNETIC RADIATION

node

Page 7: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

- Inverse relationship between wavelength and frequency

λ α 1/ν

c = λ ν = 3.00 x 108 m/s

λ = wavelength (m)

ν = frequency (cycles/second = 1/s = s-1 = hertz = Hz)

c = speed of light (3.00 x 108 m/s)

ELECTROMAGNETIC RADIATION

Page 8: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Gamma rays

X rays Ultr-violet

Infrared Microwaves Radio frequency FM Shortwave AM

Vis

ible

Visible Light: VIBGYORViolet, Indigo, Blue, Green, Yellow, Orange, Red

400 – 750 nm

- White light is a blend of all visible wavelengths

- Can be separated using a prism

Wavelength (m)

Frequency (s-1)

10-11 103

1020104

ELECTROMAGNETIC RADIATION

Page 9: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

An FM radio station broadcasts at 90.1 MHz. Calculate the wavelength (in m, nm, Ǻ) of the corresponding radio waves

c = λ ν

λ = ?ν = 90.1 MHz = 90.1 x 106 Hz = 9.01 x 107 Hz

c = 3.00 x 108 m/s

λ = c/ ν = [3.00 x 108 m/s]/[9.01 x 107 Hz]

= 3.33 m = 3.33 x 109 nm = 3.33 x 1010 Ǻ

ELECTROMAGNETIC RADIATION

Page 10: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Max Planck’s Postulate

- Energy can be gained or lost by whole-number multiples

- Change in energy (E) = nhν

n = an integer (1, 2, 3, …..)

h = Planck’s constant (6.626 x 10-34 joule-second, J-s)

ν = frequency of electromagnetic radiation absorbed or emitted

QUANTIZATION OF ENERGY

Page 11: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Max Planck’s Postulate

- Energy is quantized and can occur only in discrete units of size, hν

- Matter is allowed to emit or absorb energy only in whole-number multiples

- Each of these small quantities (packets) of energy is the quantum

- Many scientists dismissed Planck’s idea

QUANTIZATION OF ENERGY

Page 12: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Albert Einstein’s Proposal

- Electromagnetic radiation is itself quantized

- Electromagnetic radiation can be viewed as a stream of‘tiny particles’ called photons

h = Planck’s constant (6.626 x 10-34 joule-second, J-s)ν = frequency of the radiation

λ = wavelength of the radiation

QUANTIZATION OF ENERGY

λ

hchνEphoton

Page 13: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Photoelectric Effect

- A phenomenon in which electrons are emitted from the surface of a solid metal when light strikes

Eo = hνo

Eo = minimum energy required to remove an electron

νo = threshold frequency below which electrons are not emitted

by a given metal

QUANTIZATION OF ENERGY

Page 14: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Photoelectric Effect

Below νo - No electrons are emitted irrespective of the light intensity

Above νo - Number of electrons emitted increases with light intensity

- Kinetic energy increases linearly with frequency

QUANTIZATION OF ENERGY

Page 15: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

o2

)k(electron hνhνmv2

1E

m = mass of electron (kg)

v = velocity of electron (m/s)

hν = energy of incident electron (J)

hνo = energy required to remove electron from metal’s surface (J)

Photoelectric Effect

QUANTIZATION OF ENERGY

Page 16: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

E = mc2

E = energy

m = mass

c = speed of light

Einstein’s Equation

QUANTIZATION OF ENERGY

Page 17: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

λc

h

c

hc/λ

c

Em

22

The Dual Nature of Light- Electromagnetic radiation exhibits wave properties and

particulate properties

Einstein’s Equation

QUANTIZATION OF ENERGY

Page 18: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

λv

h

λc

hm

mv

For a particle with velocity, v

- Particles have wavelength associated with them- Wavelength is inversely proportional to mass

- In conclusion, matter and energy are not distinct

De Broglie’s Equation

QUANTIZATION OF ENERGY

Page 19: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

mv

Calculate the wavelength of an electron of mass 8.81 x 10-31 kg,traveling at a speed of 1.5 x 107 m/s

λ = ? v = 1.5 x 107 m/s m = 8.81 x 10-31 kg

λ = (6.626 x 10-34 j-s)/[(8.81 x 10-31 kg)(1.5 x 107 m/s)]

= 5.0 x 10-11 m

De Broglie’s Equation

QUANTIZATION OF ENERGY

Page 20: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

THE ATOMIC SPECTRUM

SpectrumIntensity of light as a function of wavelength

Transmission- Electromagnetic radiation (EM) passes through matter

without interaction

Absorption- An atom (or ion or molecule) absorbs EM and

moves to a higher energy state (excited)

Emission- An atom (or ion or molecule) releases energy and

moves to a lower energy state

Page 21: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

THE ATOMIC SPECTRUM

- The excited atoms release energy by emitting light

- The emitted light has various wavelengths called emission spectrum

- The emission spectrum of an atom is called line spectrum

- Lines corresponding to discrete wavelengths are seen when passed through a prism

- Implies electron energy levels are quantized

- The emission spectrum of the sun (white light) is a continuous spectrum when passed through a prism (ROYGBIV-rainbow)

Page 22: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

RYDBERG EQUATION

- A study of the wavelengths from the line spectra of the hydrogen atom

22

21

H n

1

n

1R

λ

1

RH = Rydberg constant = 1.097 x 107 m-1

n1 and n2 are positive integers

n1 < n2

Page 23: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

THE BOHR MODEL

- An electron in a hydrogen atom moves around the nucleus in certain allowed circular orbits

- Negatively charged electrons are attracted to the positively charged nucleus

- Electrons are charged particles under acceleration and hence radiate energy (emit light and lose energy)

Page 24: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

2

218

n

ZJ10x2.178E

n = integer (the larger the n value, the larger the orbital radius)Z = nuclear charge (Z = 1 for hydrogen, one photon)

- If n is infinitely large (n = ∞), E = 0

As the electron gets closer to the nucleus- E becomes more negative

- Energy is released from the system

THE BOHR MODEL

Page 25: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

- Energy required to excite the H electron from one level to another level

(Z = 1)

E = Efinal – Einitial

= energy level n2 – energy level n1

21

22

18

n

1

n

1J10x2.178E

THE BOHR MODEL

Page 26: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Limitations

- Bohr’s model does not work for any other atoms apart from H

- Electrons do not move in circular orbits around the nucleus

THE BOHR MODEL

Page 27: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Calculate the energy required to excite the hydrogen electronfrom level n = 1 to level n = 3. Calculate the wavelength oflight that must be absorbed by a H atom in its ground state

to reach its excited state

THE BOHR MODEL

Page 28: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

21

22

18

n

1

n

1J10x2.178E

J10x1.9361

1

3

1J10x2.178ΔE 18

2218

m10x1.03J)10x(1.936

m/s)10xs)(3.00J10x(6.626

ΔE

hcλ 7

18

834

THE BOHR MODEL

Page 29: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

QUANTUM MECHANICS

- Developed by Heisenberg, de Broglie, and Schrödinger

- An electron bound to a nucleus seems to be a standing wave (stationary waves such as those from guitar strings)

Page 30: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

QUANTUM MECHANICS

Schrödinger’s Equation

Ĥψ = Eψ

ψ = wave function (coordinates x, y, z function)

ψ2 = probability of finding an electron at a given point in space

Ĥ = operator

E = total energy of atom (sum of potential and kinetic energies)

Page 31: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

THE WAVE FUNCTION

- A specific wave function is called the orbital

- It is difficult to know precisely the pathway (position and momentum) of an electron in a given time

Page 32: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

THE WAVE FUNCTION

Heisenberg Uncertainty Principle

hΔ(mv)Δx

x = uncertainty in a particle’s position

(mv) = uncertainty in a particle’s momentum

Momentum = product of mass and velocity of an object

Page 33: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

QUANTUM NUMBERS

- Describes various properties of the orbital

Principal Quantum Number (n)- Called the electron shell

- Related to the size and energy of the atomic orbital- Has integral values 1, 2, 3, ……

- Orbital becomes larger as n increases (electron is farther from the nucleus)

- Electron energy increases with increasing n (electron is less tightly bound and energy is less negative)- Orbitals with the same energy (same n value) are said to

be degenerate

Page 34: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

- Describes various properties of the orbital

Angular Momentum (Azimuthal) Quantum Number (l)- Called electron subshell

- Related to the shape of the atomic orbitals- Has integral values 0, 1, 2, 3, ……, n-1 (for each value of n)

- The values of l are assigned letters

Value of l 0 1 2 3 4

Letter used s p d f g

QUANTUM NUMBERS

Page 35: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

- Describes various properties of the orbital

Magnetic Quantum Number (ml)- Related to the orientation of the orbital in space relative to

the other orbitals in the atom- Has integral values between l and –l, including 0 (ml = 2l + 1)

Value of l 0 1 2 3 4

Letter used s p d f g

# of orbitals (ml) 1 3 5 7 9

QUANTUM NUMBERS

Page 36: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

- Describes various properties of the orbital

Electron Spin Quantum Number (ms)

- Can have only one of the two values +1/2 and -1/2

- Electrons can spin in one of two opposite directions

- Two electrons with the same spin are parallel

- Two electrons with different spins are paired(one +1/2 and the other -1/2)

QUANTUM NUMBERS

Page 37: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Shell 1 1 subshell 1s 2 electrons

Shell 2 2 subshells

3 subshells

4 subshells

Shell 3

Shell 4

2s2p

2 electrons6 electrons10 electrons14 electrons

2 electrons 6 electrons2 electrons6 electrons10 electrons

3s3p3d

4s4p4d4f

- The value of n and the letter for l are used to designate orbitals

n l

0

01

012

0123

Orbitaldesignation

ml

0

0-1,0,+1

0-1,0,+1

-2,-1,0,+1,+2

0-1,0,+1

-2,-1,0,+1,+2-3,-2,-1,0,+1,+2,+3

# of subshells

# ofelectrons

QUANTUM NUMBERS

Page 38: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

For shell n

- The number of orbitals = n2

- The maximum number of electrons = 2n2

QUANTUM NUMBERS

Page 39: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

n

1

2

3

4

Subshell

s

s, p

s, p, d

s, p, d, f

Number of orbitals

1

1 + 3 = 4

1 + 3 + 5 = 9

1 + 3 + 5 + 7 = 16

Maximum numberof electrons

2

8

18

32

QUANTUM NUMBERS

Page 40: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

PAULI EXCLUSION PRINCIPLE

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

- Electrons in the same orbital has the same n, l, and ml

- These electrons should have different values of ms

- Implies an orbital can hold a maximum of two electrons

- The two electrons in any orbital must have opposite spins

Page 41: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

ORBITAL SHAPES AND ENERGIES

- An orbital is a region of space within an electron subshell

- The electron with a specific energy has a high probability of being found

- An orbital can accommodate a maximum of 2 electrons

- The orbitals contain areas of high probability separated by areas of low probability

- The areas of low probability are called nodes

Page 42: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

The s orbital

- The number of nodes for s orbitals = n-1

- The s orbital is spherical

- Its function always has a positive sign

ORBITAL SHAPES AND ENERGIES

Page 43: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

The p orbital

- Note that there are no 1p orbitals

- p orbitals have 2 lobes separated by a node at the nucleus

- Labeled according to the xyz cordinate axis system 2p orbital with lobes centered along the x-axis is 2px orbital 2p orbital with lobes centered along the y-axis is 2py orbital 2p orbital with lobes centered along the z-axis is 2pz orbital

- The p orbital has positive and negative signs (phases)

- Size of lobes increase with increasing n

ORBITAL SHAPES AND ENERGIES

Page 44: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

The d orbital

- Note that there are no 1d nor 2d orbitals

- The d orbitals have two different fundamental shapes

- dxy, dxz, dyz, dx2-y2: four lobes centered in the indicated planes- dz2: two lobes along the z axis and a belt centered in the xy plane

- Size of lobes increase with increasing n

ORBITAL SHAPES AND ENERGIES

Page 45: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

The f orbital

- Note that there are no 1f, 2f, nor 3f orbitals

- Shapes are more complex than the d orbitals

ORBITAL SHAPES AND ENERGIES

Page 46: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

POLYELECTRONIC ATOMS

- Atoms with more than one electron

Three energy contributions- The kinetic energy of the electrons as they move around the

nucleus- The potenital energy of attraction between the nucleus and the

electrons- The potenital energy of repulsion between the electrons

- Electron repulsion cannot be calculated exactly since electron pathways are not exactly known (electron correlation problem)

Page 47: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

- Orbitals in a given principal quantum level for H atoms are degenerate

- No orbitals are degenerate in polyelectronic atoms

- Order of increasing energy levels s < p < d < f

POLYELECTRONIC ATOMS

Page 48: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

ELECTRON CONFIGURATION

- Elements in the periodic table are arranged in order of increasing atomic number (number of protons)

- Similar to protons, electrons are added one by one to the nucleus to build up elements (Aufbau Principle)

Page 49: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Rules for assigning electrons

- Electron subshells are filled in order of increasing energy (s, p, d, f)

- All orbitals of a subshell acquire single electrons before any orbital acquire a second electron (Hund’s rule)

- All electrons in singly occupied orbitals must have the same spin

- A maximum of 2 electrons can exist in a given orbital and must have opposite spins (Pauli principle)

ELECTRON CONFIGURATION

Page 50: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

- Ordering of electron subshells is often complicated due to overlapsFor instance, the 3d subshell has higher energy than the 4s subshell

- Use of mnemonic for subshell filling is essential

1s

2s 2p

3s 3p 3d

4s

5s

4p 4d 4f

5p 5d 5f

6s

7s

6p 6d

7p

The (n+1)s orbitals alwaysfill before the nd orbitals

ELECTRON CONFIGURATION

Page 51: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

- Subshells containing electrons are designated using the sunshell numbers and letters (types)

- The number of electrons in a given subshell is indicated by a superscript

Carbon has 6 electrons: 1s22s22p2

Nitrogen has 7 electrons: 1s22s22p3

Sodium has 11 electrons: 1s22s22p63s1

ELECTRON CONFIGURATION

Page 52: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

ORBITAL DIAGRAMS

Hydrogen has electronic configuration written as 1s1

The orbital diagram is

H:

1s

Helium has electronic configuration written as 1s2

The orbital diagram is1s

He:

Page 53: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Lithium has electronic configuration written as 1s22s1

The orbital diagram is Li:1s

Boron has electronic configuration written as 1s22s22p1

The orbital diagram is1s

B:

Beryllium has electronic configuration written as 1s22s2

The orbital diagram is

2s

2s1s

2p2s

Be:

ORBITAL DIAGRAMS

Page 54: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Carbon has electronic configuration written as 1s22s22p2

The orbital diagram is C:

1s

Sodium has electronic configuration written as 1s22s22p63s1

The orbital diagram is1s

Na:

Nitrogen has electronic configuration written as 1s22s22p3

The orbital diagram is

2p2s

2s1s 2p

2p2s 3s

N:

ORBITAL DIAGRAMS

Page 55: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Neon has electronic configuration written as 1s22s22p6

The orbital diagram is Ne:

1s 2p2s

The electron configuration for sodium (Na) can be abbreviated as

[Ne]3s1

Magnesium (Mg) is abbreviated as [Ne]3s2

ABBREVIATED ELECTRON CONFIGURATION

Page 56: PRINCIPLES OF CHEMISTRY I CHEM 1211 CHAPTER 7 DR. AUGUSTINE OFORI AGYEMAN Assistant professor of chemistry Department of natural sciences Clayton state

Chromium (Cr) is expected to be [Ar]4s23d4

But is [Ar]4s13d5

Copper (Cu) is expected to be [Ar]4s23d9

But is [Ar]4s13d10

Tungsten (W) is expected to be [Xe]6s24f145d4

But is [Xe]6s14f145d5

Gold (Au) is expected to be [Xe]6s24f145d9

But is [Xe]6s14f145d10

ANOMALOUS ELECTRON CONFIGURATION