quantum theory chang chapter 7 bylikin et al. chapter 2

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Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

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Page 1: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Theory

Chang Chapter 7

Bylikin et al. Chapter 2

Page 2: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Chapter 7 Outline

• Review of Classical Physics• Quantization of Energy• Emission Spectra• Particle/Wave Duality• Quantum Mechanics

• Heisenberg• Schrodinger• Quantum Numbers• Electron Configurations

Page 3: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Review of Classical Physics

• Waves: vibrating disturbance that transmits energy

– Speed of a wave = wavelength (l) ∙ frequency (n)Frequency = number of waves that pass through a particular point in 1 second (units = Hz)

Wavelength has units of nanometers (nm)

UNIT FACTOR: 1 nm = 1x10-9m

Page 4: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Review of Classical Physics

• Radiation: Emission and transmission of energy through space via Electromagnetic (EM) waves– EM radiation = radiant energy = light– Speed of light= 3.00x108 m/s = l∙ = n c

Page 5: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Review of Classical Physics

• Example: The yellow light given off by a sodium vapor lamp used for public lighting has a wavelength of 589 nm. What is the frequency of this radiation?

Page 6: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Review of Classical Physics

Page 7: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantization of Energy

• Before 1900: energy is continuous, any amount of energy can be released or absorbed

• In 1900 Max Plank proposed energy is quantized–Quantum= smallest amount of EM energy

that can be absorbed or released

Page 8: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantization of Energy

• Energy of ONE quantum = E = h∙n• h = Plank’s Constant = 6.626x10-34 J∙s

• Energy that can be released or absorbed• E = n∙h∙n (where n = 1, 2, 3…)• “energy can be absorbed or released only in

integer units of quantum”

Page 9: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantization of Energy

• Example: Calculate the energy of one photon of yellow light with wavelength 589 nm. Repeat for 1 mol of photons.

Page 10: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Emission Spectra

• Continuous or line spectra of radiation emitted by substances–Energize via heat or high-voltage discharge–Element line spectra will emit only specific l–Every element has a unique spectrum

• Example: Hydrogen

Page 11: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Emission Spectra

• In 1913 Bohr proposed an explanation for the emission spectrum of H–Proposed a new model of atom

• Massive proton at center • Light electron orbit around

– The electron can only occupy certain orbits– Each orbit has a distinct energy (quantized)

Page 12: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Particle/Wave Duality

• Why can the H e- only orbit at certain distances?–De Broglie proposed that e- in atoms

behaved like standing waves• The length of the wave must fit the circumference

of the orbit exactly

Page 13: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Particle/Wave Duality

• De Broglie’s reasoning led to the conclusion that waves can behave like particles and particles can have wave-like properties–Deduced that the particle-wave properties

are related by:

l = h_

m∙u

l = wavelength (m)h = Plank’s constant (J∙s)m = particle mass (kg)u = particle velocity (m/s)

Page 14: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Particle/Wave Duality

• Example: What is the wavelength of an electron moving with a speed of 5.97x106m/s?

Page 15: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Bohr’s model only works for one electron species (H, He+, Li+2…)–The problem is with location

• Particles have locations• Waves do not have locations

– If an electron acts as a wave, it’s location must be uncertain…

Page 16: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Heisenberg Uncertainty principal– It is impossible to know both the position (x)

and the momentum (p) of an e- at the same time with unlimited precision.

–Therefore the well-defined orbits of the Bohr Model are incorrect

Page 17: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Schrödinger Equation (1926)–Advanced mathematical description of the

behavior and energies of submicroscopic particles

HY = EY–Solution yields

• Energy levels available to a particular e-

• Wave functions (Y) that correspond to those energies

–Cannot be solved exactly for atoms with more than one e-

Page 18: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Y2 = e- density

= probability of finding the e- in a given region of space

–Atomic Orbital = the wave function of an electron in an atom (no longer use “orbit”)

Page 19: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Quantum Numbers–Used to describe the distribution of electrons

in atoms• Derived from the Schrödinger equation for H

–Each electron can be described by a unique set of 4 numbers• (1) principal quantum number, n• (2) angular momentum quantum number, l• (3) magnetic quantum number, ml

• (4) electron spin quantum number, ms

Page 20: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Principal Quantum Number (n)–n = 1, 2, 3…–n is related to the average distance between

the e- and the nucleus–For the H atom, n specifies the energy of the

orbital

Page 21: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Angular Momentum Quantum Number (l)– l = 0, 1, 2, 3, …, (n-1)– l indicates the shape of the orbital– Indicate the value of l with letters:

–Example: What are the values of l if n=3?• l can be: 0 (s), 1 (p) or 2 (d)

l 0 1 2 3

Orbital type s p d f

Page 22: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Magnetic Quantum Number (ml)–ml describes the orientation of the orbital in

space–For a given values of l, (2l+1) values

possible for ml

–ml= -l, (-l+1), (-l+2)…0…(l-2), (l-1), l

–Example: If l=2, what are the values of ml?• ml = [-2, -1, 0, 1, 2]

Page 23: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Electron Spin Quantum Number–ms indicates the spin on the e-

–ms = +1/2 or -1/2

–Spinning e- acts like tiny magnets and generate magnetic fields

Page 24: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Quantum Number Summary

Page 25: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Atomic Orbitals – s– l=0, ml=0–s orbitals have spherical shapes

Page 26: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Atomic orbitals – p– l=1, ml=-1,0,1

Page 27: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Atomic Orbitals – d– l= 2, ml=-2,-1,0,1,2

Page 28: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Electron Configurations–How the electrons are distributed among the

various atomic orbitals• described by the quantum numbers

–The four quantum numbers allow us to label any electron in any orbital (like an address)• Example: Write the four quantum numbers for

an electron in a 4p orbital

Page 29: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Orbital Energies• In hydrogen, energy of the orbital determined by

n only

Page 30: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Orbital Energies– In atoms w/ multiple electrons, energy of the

orbital determined by n & l

Page 31: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Electron configuration for H

1s1

• Orbital Diagram (shows spin)

__

1s

Principal Quantum Number

AngularMomentumQuantumNumber

Number ofElectrons inthe Orbital or Subshell

Page 32: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• For atoms with more than one electrons, we need more tools to determine how electrons fill their orbitals

–Aufbau Principle- as protons are added one by one to the nucleus to build up the elements, electrons are similarly added to the atomic orbitals

Page 33: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

–Pauli Exclusionary Principle: no two electrons in the same atom can have the same set of quantum numbers

–Hund’s Rule: the most stable arrangement of electrons in subshells is the one with the maximum numbers of parallel electron spins

Page 34: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

Page 35: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Electron Configuration of N (Z=7)

• Orbital Diagram

• Energy Level Diagram

Page 36: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Example: Show the electron configuration, the orbital diagram, and the energy level diagram for Al

Page 37: Quantum Theory Chang Chapter 7 Bylikin et al. Chapter 2

Quantum Mechanics

• Transition Metals–some give rise to unusual electron

configurations• Example: Chromium-

[Ar] 4s13d5 instead of [Ar] 4s23d4

• Example: Copper-

[Ar] 4s13d10 instead of [Ar] 4s23d9

–This occurs because the 4s and 3d orbitals are so close in energy