Title: Honors Chemistry
1Honors Chemistry
- Chapter 7 Quantum Mechanics
27.1 Wave Properties
- Wavelength (l) distance between two in-phase
points - Measured in meters
- Frequency (n) number of waves per second
- Measured in Hertz (Hz)
- Amplitude (y) distance of maximum displacement
from rest position - Amplitude corresponds to wave energy
37.1 The Wave Equation
- v ln
- Find the wavelength of a 256 HZ (middle C) sound
wave traveling at 343 m/s. - v ln
- 343 m/s l (256 Hz)
- l 1.34 m
- Try this.
- Find the frequency of a 25.0 cm wave traveling at
0.75 m/s.
47.1 Electromagnetic Radiation
- James Clerk Maxwell (1873)
- Mathematical description of light waves
- Light is an electromagnetic wave
- Speed of light (c) is constant
- c 2.99792458 x 108 m/s
- To 3 sig dig, 3.00 x 108 m/s is fine
- Try this.
- Find the frequency of a 250 nm light wave.
(Dont forget about the nano prefix!)
57.1 Electromagnetic Spectrum
- Radio, micro, IR, ROYGBIV, UV, X, g
- long l ------------------------------- short l
- low n -------------------------------- high n
- Radio wave end of the spectrum is low energy
radiation - Gamma ray end is high energy radiation
- Black body radiation
- Wave theory fails to account for this!
67.1 Quantum Theory
- Max Planck (1900)
- Energy is emitted and absorbed only in small,
discrete packets called quanta - Energy of a quantum of energy given byE hn
- h 6.626 x 10-34 Js (Plancks constant)
- Correctly accounts for blackbody curves
- Planck has no idea why it works!
77.1 Quantum Theory
- Find the energy of a 2.50 x 1014 Hz light wave.
- E hn
- E (6.626 x 10-34 Js)(2.50 x 1014 Hz)
- E 1.66 x 10-19 J
- A quantum holds a tiny amount of energy!
- Try this.
- Find the energy of a 475 nm light wave.
- Hint Use the wave equation first!
87.2 The Photoelectric Effect
- Albert Einstein (1905)
- Electrons ejected from surface of metal exposed
to light - Depends on frequency of light
- Electrons ejected at a certain cutoff frequency
- Above cutoff n, electrons leave with more energy
- Bright light ejects more electrons
- Quantum theory explains results
- Light is made of quanta called photons
97.3 Spectroscopy
- Emission spectra light given off by glowing
objects - Can be continuous or discontinuous
- Line spectra series of bright lines emitted by
gas phase atoms - Pattern of bright lines is characteristic of the
element that is glowing - Absorption spectra dark lines in spectrum as
light passes through a gas
107.3 Bohrs Model
- Niels Bohr (1913)
- Electron energies are quantized
- Only certain orbits are allowed
- - RHEn ------ n2
- RH 2.18 x 10-18 J (Rydberg constant)
- n 1, 2, 3, 4, .
117.3 Bohrs Model
- DE Ef E0
- -RH -RHDE ----- - -----
nf2 n02 - Factor out RH
- 1 1 DE RH (----- -
----- ) n02 nf2
Link to Hydrogen energy states
127.3 Bohrs Model
- Find the energy of a photon of light emitted by
an electron jumping from level 5 down to level 2. - DE RH (1/n52 1/n22)
- DE (2.18 x 10-18 J)(1/25 1/4)
- DE -4.58 x 10-19 J
- Try this.
- Find the energy of the jump from level 1 to level
4. - Find the frequency of the light produced.
137.4 Duality
- Louis de Broglie (1924)
- Electrons can be treated as waves
- Each orbit must contain a whole number of
wavesexplains orbit quantization! - h l ---- mv
- mv is momentum (p), so we can write l h/p
- Verified by Davisson, Germer, and Thomson
Link to quantum atom model
147.4 Duality
- Find the wavelength of a 3.00 kg duck flying at
5.00 m/s. - l h/mv
- l (6.626 x 10-34 Js) / (3.00 kg)(5.00 m/s)
- l 4.42 x 10-35 m
- Try this.
- Find the wavelength of an electron traveling at
500,000 m/s. (me 9.11 x 10-31 kg)
157.5 Uncertainty Principle
- Werner Heisenberg (1926)
- Complementary variables cannot be known to
arbitrary precision - dp dq h/2
- Minimum limits to uncertainties in values are
inversely proportional - Position and momentum are an important
complementary pair - dx dpx h/2
167.5 Uncertainty Principle
- Find the uncertainty in velocity of an electron
confined to a hydrogen atom (dx 0.037 nm). - dx dpx h/2
- (3.7 x 10-11 m) dp 5.27 x 10-35 Js
- dp 1.4 x 10-24 kg m/s
- p mv
- 1.4 x 10-24 kg m/s (9.11 x 10-31 kg) dv
- dv 1.5 x 106 m/s
177.5 Uncertainty Principle
- Try this
- Find the uncertainty in position of a 20.0 mg fly
whose position is known to within 0.5 mm. - Uncertainty limits are not significant for
macroscopic objects, but they are significant to
subatomic particles - Cannot know the position and momentum of an
electron at the same time! - Concept of orbits will not work
187.5 Quantum Mechanics
- Erwin Schrödinger (1926)
- Schrödinger equation treat electron as a
standing wave surrounding the nucleus - Schrödinger equation is ugly!
- Solve for amplitude function (y)
- Remember amplitude is energy
- Produces an energy diagram like Bohrs, but this
one actually works - Wave function has no physical meaning
197.5 Copenhagen Interpretation
- Max Born (1926)
- y2 denotes probability
- Electron is delocalized
- Wave function collapses on observation
- electron density refers to magnitude of the
probability wave for the electron - Orbital spatial probability distribution
- Electron clouds
- Objections Schrödingers Cat
- Other interpretations
207.6 Quantum Numbers
- Set of numbers that describe the distribution of
electrons in the atom - Principal Quantum Number (n)
- n 1, 2, 3, 4,
- Corresponds to the n value used by Bohr
- Describes energy level of the shell
- Defines the size of the electron cloud
217.6 Quantum Numbers
- Angular Momentum Quantum Number (l)
- l 0, 1, 2, , n 1
- There are a total of n values
- Sublevels of the energy level
- Angular distribution of electron cloud
- For hydrogen, sublevels are degenerate
- Correspond to fine structure spectral lines
- l 0 is s orbital l 2 is d orbital
- l 1 is p orbital l 3 is f orbital
227.6 Quantum Numbers
- Magnetic Quantum Number (ml)
- ml -l, , 0, , l
- There are a total of 2l 1 values
- Number of degenerate orbitals in sublevel
- Spatial orientation of the orbital
- Zeeman Effect
- Electron Spin Quantum Number (ms)
- ms ½, -½
- Two possible electron spin states
- Spin up, spin down
237.7 Atomic Orbitals
- s, p, d, f orbitals
- Radial probability distributions
- distance from nucleus of high e- probability
247.7 Atomic Orbitals
- Angular probability distributions
- Show regions of high e- probability
- Cool 3d pictures
257.7 Orbital Energies
- n determines energy
- For H, all subshells are degenerate
- Multielectron atomseach subshell liesat a
different energy - Shielding effect
- Fill lowest energyorbitals first
267.7 The Diagonal Rule
- Rule of thumb
- Shows the orderin which orbitalsare filled
- Paramagnetic
- Unpaired e-
- Attracted to mag
- Diamagnetic
- Paired e-
- Not attracted
277.8 Electron Configurations
- H has 1 electron
- Put it in 1s
- Write it 1s1
- Read one-s-one
- What about He?
- You got it1s2
- Keep filling 1s until it is full
- But when is it full?
287.8 Pauli Exclusion Principle
- No two electrons may share the exact set of
quantum numbers - Consider Heliums 1s2 configuration
- First electron n 1, l 0, ml 0, ms ½
- Second electron same n, l, ml
- ms must be -½
- No room for more electrons in 1s orbital
- Each orbital can hold only two electrons!
297.8 Electron Configurations
- What is the electron configuration of Li?
- 1s2 2s1
- What about N?
- 1s2 2s2 2p3
- But how are p electrons organized?
- Hunds Rule arrange electrons in such a way as
to maximize total spin state - Put e-s in separate orbitals, same spin
307.9 Aufbau Principle
- Build up on previous e- configurations
- Each atom adds one more e-
- Express configuration with noble gas core
- Al 1s2 2s2 2p6 3s2 3p1
- First 3 terms are the same as Ne config.
- Write it as Ne 3s2 3p1
317.9 Exceptions
- Particularly stable configurations
- Full sublevel
- Half-full sublevel
- Some transition metals rearrange
- Cr Ar 4s2 3d4
- Just missed the stable half-full 3d5
- Kick one e- up to d to get Ar 4s1 3d5
- What other family would do this?
- Cu Ar 4s2 3d9 ? Ar 4s1 3d10
327.9 Periodicity of Electron Configuration