What is Light 1 Waves z Wavelength length

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What is Light? 1

What is Light? 1

Waves z Wavelength ( ) - length of one complete wave z Frequency (

Waves z Wavelength ( ) - length of one complete wave z Frequency ( ) - # of waves that pass a point during a certain time period y hertz (Hz) = 1/s z Amplitude (A) - distance from the origin to the trough or crest 2

Waves crest A greater amplitude (intensity) origin trough A greater frequency (color) 3

Waves crest A greater amplitude (intensity) origin trough A greater frequency (color) 3

EM Spectrum H I G H L O W E N E R G

EM Spectrum H I G H L O W E N E R G Y 4

EM Spectrum H I G H L O W E N E R G

EM Spectrum H I G H L O W E N E R G Y red R O Y G. orange green yellow B blue I indigo V violet E N E R G Y 5

EM Spectrum z Frequency & wavelength are inversely proportional c = c: speed of

EM Spectrum z Frequency & wavelength are inversely proportional c = c: speed of light (3. 00 108 m/s) : wavelength (m, nm, etc. ) : frequency (Hz) 6

EM Spectrum z EX: Find the frequency of a photon with a wavelength of

EM Spectrum z EX: Find the frequency of a photon with a wavelength of 434 nm. GIVEN: WORK: =c =? = 434 nm = 4. 34 10 -7 m = 3. 00 108 m/s -7 m 8 4. 34 10 c = 3. 00 10 m/s = 6. 91 1014 Hz 7

Light is more than waves… z Planck (1900) y Observed - emission of light

Light is more than waves… z Planck (1900) y Observed - emission of light from hot objects y Concluded - energy is emitted in small, specific amounts (quanta) 8

Niels Bohr’s Model (1913) z. Electrons orbit the nucleus in circular paths of fixed

Niels Bohr’s Model (1913) z. Electrons orbit the nucleus in circular paths of fixed energy (energy levels).

Bohr Model Continued z Electrons can jump from energy level to energy level. z

Bohr Model Continued z Electrons can jump from energy level to energy level. z Electrons absorb or emit light energy when they jump from one energy level to another. z A quantum of energy is the amount of energy required to move an electron from one energy level to another.

Energy Levels in Atoms • The energy levels are like the rungs of a

Energy Levels in Atoms • The energy levels are like the rungs of a ladder but are not equally spaced. Photon - bundles of light energy that is emitted by electrons as they go from higher energy levels to lower levels.

Photons z Einstein (1905) y Concluded - light has properties of both waves and

Photons z Einstein (1905) y Concluded - light has properties of both waves and particles “wave-particle duality” 12

Quantum Theory z. The energy of a photon is proportional to its frequency. E

Quantum Theory z. The energy of a photon is proportional to its frequency. E = h E: energy (J, joules) h: Planck’s constant (6. 6262 10 -34 J·s) : frequency (Hz) 13

Quantum Theory z EX: Find the energy of a red photon with a frequency

Quantum Theory z EX: Find the energy of a red photon with a frequency of 4. 57 1014 Hz. GIVEN: E=? = 4. 57 1014 Hz h = 6. 6262 10 -34 J·s WORK: E = h E = (6. 6262 10 -34 J·s) (4. 57 1014 Hz) E = 3. 03 10 -19 J 14

Quantum Theory z. The energy of a photon is inversely proportional to its wavelength.

Quantum Theory z. The energy of a photon is inversely proportional to its wavelength. E: energy (J, joules) h: Planck’s constant (6. 6262 10 -34 J·s) c: speed of light (3. 00 x 108 m/s) 15

Line-Emission Spectrum excited state ENERGY IN PHOTON OUT ground state 16

Line-Emission Spectrum excited state ENERGY IN PHOTON OUT ground state 16

Line-Emission Spectrum z Each element has a unique bright-line emission spectrum. y “Atomic Fingerprint”

Line-Emission Spectrum z Each element has a unique bright-line emission spectrum. y “Atomic Fingerprint” (Helium) The emission lines correspond to photons of discrete energies that are emitted when excited atomic states in the gas make transitions back to lower-lying levels. 17

Hydrogen Line Emission Spectrum Bohr explains the spectrum for Hydrogen, but not for other

Hydrogen Line Emission Spectrum Bohr explains the spectrum for Hydrogen, but not for other elements… Quantum Mechanical Model

Part 2: Quantum Mechanics 19

Part 2: Quantum Mechanics 19

Electrons as Waves z Louis de Broglie (1924) y Applied waveparticle theory to electrons

Electrons as Waves z Louis de Broglie (1924) y Applied waveparticle theory to electrons y Electrons exhibit wave properties QUANTIZED WAVELENGTHS: 20

Quantum Mechanics z Schrödinger and “wavefunction” y The wavefunction helps describes the location of

Quantum Mechanics z Schrödinger and “wavefunction” y The wavefunction helps describes the location of the electron, and its probable location 21

Quantum Mechanics z Orbital (“electron cloud”) y Region in space where there is 90%

Quantum Mechanics z Orbital (“electron cloud”) y Region in space where there is 90% probability of finding an electron Orbital Radial Distribution Curve 22

Quantum Mechanics z Quantum Numbers: y Specify the “address” of each electron in an

Quantum Mechanics z Quantum Numbers: y Specify the “address” of each electron in an atom 23

Quantum Mechanics Energy Level ( n ) y Size of the orbital y n

Quantum Mechanics Energy Level ( n ) y Size of the orbital y n 2 = # of orbitals in the energy level 24

Orbital Types z s-orbital: electrons are found within a sphere around the nucleus. s

Orbital Types z s-orbital: electrons are found within a sphere around the nucleus. s z p-orbital: orbitals that look like “dumbbells or propellers” or tear drops. 25

Orbital Types z d-orbitals: most appear to be the combination of two p-orbitals, “daisy”.

Orbital Types z d-orbitals: most appear to be the combination of two p-orbitals, “daisy”. 26

Orbital Types z f-orbitals: just crazy! 27

Orbital Types z f-orbitals: just crazy! 27

Quantum Numbers zn = # of sublevels per level zn 2 = # of

Quantum Numbers zn = # of sublevels per level zn 2 = # of orbitals per level z. Sublevel sets: 1 s, 3 p, 5 d, 7 f 28

Quantum Numbers y. Atom is the filing cabinet y. Each drawer is an energy

Quantum Numbers y. Atom is the filing cabinet y. Each drawer is an energy level y. Folders are sublevels (s, p, d, etc. ) y. Papers in the folder are orbitals 29

Quantum Numbers - Rules z Aufbau Principle y Electrons fill the lowest energy orbitals

Quantum Numbers - Rules z Aufbau Principle y Electrons fill the lowest energy orbitals first. y “Lazy Tenant Rule” 30

Quantum Numbers z Spin Quantum Number (ms or s) y Electron spin +½ or

Quantum Numbers z Spin Quantum Number (ms or s) y Electron spin +½ or -½ y An orbital can hold 2 electrons that spin in opposite directions. 31

Quantum Numbers - Rules z Pauli Exclusion Principle – Definition 1 y Each orbital

Quantum Numbers - Rules z Pauli Exclusion Principle – Definition 1 y Each orbital can hold TWO electrons, but they must have opposite spins. 32

Quantum Numbers z Pauli Exclusion Principle – Definition 2 y No two electrons in

Quantum Numbers z Pauli Exclusion Principle – Definition 2 y No two electrons in an atom can have the same 4 quantum numbers. y Each electron has a unique “address”: 1. Principal # (n) energy level 2. Ang. Mom. # (l) sublevel (s, p, d, f) 3. Magnetic # (ml) orbital 4. Spin # (ms or s) electron 33

Quantum Numbers - Rules z Hund’s Rule y Within a sublevel, place one e-

Quantum Numbers - Rules z Hund’s Rule y Within a sublevel, place one e- per orbital before pairing them. WRONG RIGHT 34

Notation z Orbital Diagram O 8 e- 1 s 2 s 2 p z.

Notation z Orbital Diagram O 8 e- 1 s 2 s 2 p z. Electron Configuration 2 2 4 1 s 2 s 2 p 35

Notation z Longhand Configuration S 16 e 6 2 2 2 1 s 2

Notation z Longhand Configuration S 16 e 6 2 2 2 1 s 2 s 2 p 3 s Core Electrons 4 3 p Valence Electrons z. Shorthand Configuration S 16 e 2 4 [Ne] 3 s 3 p 36

Periodic Patterns s p 1 2 3 4 5 6 7 f (n-2) d

Periodic Patterns s p 1 2 3 4 5 6 7 f (n-2) d (n-1) 6 7 © 1998 by Harcourt Brace & Company 37

Periodic Patterns z Example - Hydrogen 1 1 s 1 st Period 1 st

Periodic Patterns z Example - Hydrogen 1 1 s 1 st Period 1 st column of s-block 38

Periodic Patterns z Shorthand Configuration y Core e-: Go up one row and over

Periodic Patterns z Shorthand Configuration y Core e-: Go up one row and over to the Noble Gas. y Valence e-: On the next row, fill in the # of e- in each sublevel. 39

Periodic Patterns z Example - Germanium [Ar] 2 4 s 10 3 d 2

Periodic Patterns z Example - Germanium [Ar] 2 4 s 10 3 d 2 4 p 40

Stability z Full energy level z. Full sublevel (s, p, d, f) z. Half-full

Stability z Full energy level z. Full sublevel (s, p, d, f) z. Half-full sublevel 41

Stability z Electron Configuration Exceptions y. Copper EXPECT: [Ar] 4 s 2 3 d

Stability z Electron Configuration Exceptions y. Copper EXPECT: [Ar] 4 s 2 3 d 9 ACTUALLY: [Ar] 4 s 1 3 d 10 y. Copper gains stability with a full d-sublevel. 42

Stability z Electron Configuration Exceptions y. Chromium EXPECT: [Ar] 4 s 2 3 d

Stability z Electron Configuration Exceptions y. Chromium EXPECT: [Ar] 4 s 2 3 d 4 ACTUALLY: [Ar] 4 s 1 3 d 5 y. Chromium gains stability with a half-full d-sublevel. 43

Stability z Ion Formation y Atoms gain or lose electrons to become more stable.

Stability z Ion Formation y Atoms gain or lose electrons to become more stable. y Isoelectronic with the Noble Gases. 44

Stability z Ion Electron Configuration y Write the e- config for the closest Noble

Stability z Ion Electron Configuration y Write the e- config for the closest Noble Gas y EX: Oxygen ion O 2 - Ne 2 O 10 e [He] 2 2 s 6 2 p 45

Quantum Mechanics z Heisenberg Uncertainty Principle y Impossible to know both the velocity and

Quantum Mechanics z Heisenberg Uncertainty Principle y Impossible to know both the velocity and position of an electron at the same time 46