hstmr.watson chapter 7 quantum theory of the atom

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HST Mr.Wats on Chapter 7 Chapter 7 Quantum Theory of the Atom

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Page 1: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Chapter 7Chapter 7

Quantum Theory of the Atom

Page 2: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Electromagnetic RadiationElectromagnetic Radiation

Electromagnetic waveA wave of energy having a frequency

within the electromagnetic spectrum and propagated as a periodic disturbance of the electromagnetic field when an electric charge oscillates or accelerates.

Page 3: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Electromagnetic RadiationElectromagnetic Radiation

Electromagnetic wavewavelengthfrequency amplitude

Page 4: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Electromagnetic RadiationElectromagnetic Radiation

= c

where=> frequency

=> wavelength

c => speed of light

Page 5: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Wave Nature of the ElectronWave Nature of the Electron

Page 6: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Electromagnetic SpectrumElectromagnetic Spectrum

Page 7: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Line Emission SpectrumLine Emission Spectrum

Page 8: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Line SpectrumLine Spectrum

A spectrum produced by a luminous gas or vapor and appearing as distinct lines characteristic of the various elements constituting the gas.

Page 9: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Emission SpectrumEmission Spectrum

The spectrum of bright lines, bands, or continuous radiation characteristic of and determined by a specific emitting substance subjected to a specific kind of excitation.

Page 10: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Ground StateGround State

The state of least possible energy in a physical system, as of elementary particles. Also called ground level.

Page 11: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Excited StateExcited State

Being at an energy level higher than the ground state.

Page 12: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Photoelectric EffectPhotoelectric Effect

the emission of electrons by substances, especially metals, when light falls on their surfaces.

Page 13: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Photoelectric EffectPhotoelectric Effect

Page 14: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Quantum MechanicsQuantum Mechanics

Quantum theorythe theory of the structure and behavior of

atoms and molecules.

Page 15: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Black Body RadiationBlack Body Radiation

http://www.cbu.edu/~mcondren/C11599/BBvis.mov

Page 16: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Electromagnetic RadiationElectromagnetic Radiation

Ehi - Elo = hc/where E => energy

h => Planck's constant

c => speed of light

=> wavelength

Page 17: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

PhotonsPhotons

The quantum of electromagnetic energy, generally regarded as a discrete particle having zero mass, no electric charge, and an indefinitely long lifetime.

Page 18: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Dispersion of White LightDispersion of White Light

Page 19: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

The Atomic Spectrum of The Atomic Spectrum of HydrogenHydrogen

and the Bohr Model and the Bohr ModelBohr Model for the Hydrogen Atom

mnr = nh/2p

Page 20: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Bohr AtomBohr Atom

Page 21: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Bohr ModelBohr Model

E = -B/n2

where n => quantum number

1, 2, 3, 4, 5, 6, 7, etc

Page 22: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Bohr ModelBohr Model

for hydrogen

ground state: n = 1

excited state: n > 1

Page 23: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Bohr ModelBohr Model

E = (-2.179 X 10-18 J/part.)

(6.022 X 1023 part./mole)

(1 kJ/103 J)/n2

= (-1312 kJ/mol)(1/n2)

Page 24: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Electron Transition in a Hydrogen Electron Transition in a Hydrogen AtomAtom

Lyman series => ultraviolet

n > 1 ==> n = 1

Balmer series => visible light

n > 2 ==> n = 2

Paschen series => infrared

n > 3 ==> n = 3

Page 25: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Line SpectraLine Spectra

See CHEMWORKS software

Page 26: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Absorption SpectrumAbsorption Spectrum

Light shinning on a sample causes electrons to be excited from the ground state to an excited state

wavelengths of that energy are removed from transmitted spectra

Page 27: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Knowing diamond is transparent, which curve best represents the absorption spectrum of diamond (see below)?

A, B, C

Page 28: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

According to the energy diagram below for the Bohr model of the hydrogen atom, if an electron jumps from E1 to E2, energy is

absorbed

emitted

not involved

Page 29: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Heisenberg, WernerHeisenberg, Werner1901–76, German physicist1901–76, German physicist

1932 Nobel Prize in physics1932 Nobel Prize in physics

A founder of QUANTUM MECHANICS, he is famous for his uncertainty principle, which states that it is impossible to determine both the position and momentum of a subatomic particle (such as the electron) with arbitrarily high accuracy.

Page 30: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Heissenberg Uncertainty Heissenberg Uncertainty PrinciplePrinciple

“it is impossible to determine both the position and momentum of a subatomic particle (such as the electron) with arbitrarily high accuracy”

The effect of this principle is to convert the laws of physics into statements about relative, instead of absolute, certainties.

Page 31: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

OrbitalsOrbitals

region of probability of finding an electron around the nucleus

4 types => s p d fmaximum of 2 electrons per orbital

Page 32: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Pure Atomic OrbitalsPure Atomic Orbitals

shape # of orbitals / energy level

s spherical 1

p dumbbell 3

d complex 5

f very complex 7

Page 33: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Atomic Orbitals, s-Atomic Orbitals, s-typetype

Page 34: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Atomic Orbitals, p-Atomic Orbitals, p-typetype

Page 35: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Atomic Orbitals, d-typeAtomic Orbitals, d-type

Page 36: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Atomic Orbitals, f-typeAtomic Orbitals, f-type

Page 37: HSTMr.Watson Chapter 7 Quantum Theory of the Atom

HSTMr.Watson

Shapes of OrbitalsShapes of Orbitals

http://www.colby.edu/chemistry/OChem/DEMOS/Orbitals.html