Title: Periodicity and Atomic Structure
1Chapter 5
- Periodicity and Atomic Structure
2Development of the Periodic Table
- The periodic table is the most important
organizing principle in chemistry. - Periodic table powerpoint elements of a group
have similar properties - Chapter 2 elements in a group form similar
formulas - Predict the properties of an element by knowing
the properties of other elements in the group
3Light and the Electromagnetic Spectrum
- Radiation (light) composed waves of energy
- Waves were continuous and spanned the
electromagnetic spectrum
4Light and the Electromagnetic Spectrum
5Light and the Electromagnetic Spectrum
6Light and the Electromagnetic Spectrum
- Speed of a wave is the wavelength (in meters)
multiplied by its frequency in reciprocal
seconds. - Wavelength x Frequency Speed
- ? (m) x ? (s1) c (m/s1)
- C speed of light - 2.9979 x 108 m/s1
7Electromagnetic Radiation and Atomic Spectra
- Classical Physics does not explain
- Black-body radiation
- Photoelectric effect
- Atomic Line Spectra
8Particlelike Properties of Electromagnetic
Radiation The Plank Equation
- Blackbody radiation is the visible glow that
solid objects emit when heated. - Max Planck (18581947) Developed a formula to
fit the observations. He proposed that energy is
only emitted in discrete packets called quanta. - The amount of energy depends on the frequency
9Particlelike Properties of Electromagnetic
Radiation The Plank Equation
- A photons energy must exceed a minimum threshold
for electrons to be ejected. - Energy of a photon depends only on the frequency.
10Electromagnetic Radiation and Atomic Spectra
- Atomic spectra Result from excited atoms
emitting light. - Line spectra Result from electron transitions
between specific energy levels.
11Electromagnetic Radiation and Atomic Spectra
1/? R 1/m2 1/n2
12Quantum Mechanics and the Heisenburg Uncertainty
Principle
- Niels Bohr (18851962) Described atom as
electrons circling around a nucleus and concluded
that electrons have specific energy levels. - Erwin Schrödinger (18871961) Proposed quantum
mechanical model of atom, which focuses on
wavelike properties of electrons.
13Quantum Mechanics and the Heisenburg Uncertainty
Principle
- Werner Heisenberg (19011976) Showed that it is
impossible to know (or measure) precisely both
the position and velocity (or the momentum) at
the same time. - The simple act of seeing an electron would
change its energy and therefore its position.
14Wave Functions and Quantum Mechanics
- Erwin Schrödinger (18871961) Developed a
compromise which calculates both the energy of an
electron and the probability of finding an
electron at any point in the molecule. - This is accomplished by solving the Schrödinger
equation, resulting in the wave function, ?.
15Wave Functions and Quantum Mechanics
- Wave functions describe the behavior of
electrons. - Each wave function contains three variables
called quantum numbers - Principal Quantum Number (n)
- Angular-Momentum Quantum Number (l)
- Magnetic Quantum Number (ml)
16Wave Functions and Quantum Mechanics
- Principal Quantum Number (n) Defines the size
and energy level of the orbital. n 1, 2, 3,
??? - As n increases, the electrons get farther from
the nucleus. - As n increases, the electrons energy increases.
- Each value of n is generally called a shell.
17Wave Functions and Quantum Mechanics
- Angular-Momentum Quantum Number (l) Defines the
three-dimensional shape of the orbital. - For an orbital of principal quantum number n, the
value of l can have an integer value from 0 to n
1. - This gives the subshell notation l 0 s
orbital l 1 p orbital l 2 d
orbital l 3 f orbital l 4 g orbital
18Wave Functions and Quantum Mechanics
- Magnetic Quantum Number (ml) Defines the spatial
orientation of the orbital. - For orbital of angular-momentum quantum number,
l, the value of ml has integer values from l to
l. - This gives a spatial orientation ofl 0 giving
ml 0 l 1 giving ml 1, 0, 1l 2 giving
ml 2, 1, 0, 1, 2, and so on...
19Wave Functions and Quantum Mechanics
20Problem
- Why cant an electron have the following quantum
numbers? - (a) n 2, l 2, ml 1 (b) n 3, l 0, ml
3 - (c) n 5, l 2, ml 1
- Give orbital notations for electrons with the
following quantum numbers - (a) n 2, l 1, ml 1 (b) n 4, l 3, ml
2 - (c) n 3, l 2, ml 1
21The Shapes of Orbitals
22The Shapes of Orbitals
23The Shape of Orbitals
24Orbital Energy Levels in Multielectron Atoms
25Orbital Energy Levels in Multielectron Atoms
- Zeff is lower than actual nuclear charge.
- Zeff increases toward nucleus ns gt np gt nd gt
nf - This explains certain periodic changes observed.
26Orbital Energy Levels in Multielectron Atoms
- Electron shielding leads to energy differences
among orbitals within a shell. - Net nuclear charge felt by an electron is called
the effective nuclear charge (Zeff).
27Wave Functions and Quantum Mechanics
- Spin Quantum Number
- The Pauli Exclusion Principle states that no two
electrons can have the same four quantum
numbers.x
28Electron Configurations of Multielectron Atoms
- Pauli Exclusion Principle No two electrons in an
atom can have the same quantum numbers (n, l, ml,
ms). - Hunds Rule When filling orbitals in the same
subshell, maximize the number of parallel spins.
29Electron Configurations of Multielectron Atoms
- Rules of Aufbau Principle
- Lower n orbitals fill first.
- Each orbital holds two electrons each with
different ms. - Half-fill degenerate orbitals before
pairingelectrons.
30Electron Configurations and Multielectron Atoms
Li ?? ? 1s2 2s1 1s 2s Be
?? ?? 1s2 2s2 1s 2s B
?? ?? ? 1s2 2s2 2p1
1s 2s 2px 2py 2pz C ?? ??
? ? 1s2 2s2 2p2 1s 2s
2px 2py 2pz
31Electron Configurations and Multielectron Atoms
N ?? ?? ? ? ? 1s2 2s2 2p3
1s 2s 2px 2py 2pz O ?? ?? ?? ?
? 1s2 2s2 2p4 1s 2s 2px 2py
2pz Ne ?? ?? ?? ?? ?? 1s2 2s2 2p5
1s 2s 2px 2py 2pz S Ne ?? ?? ?
? Ne 3s2 3p4 3s 3px
3py 3pz
32Problems
- Give the ground-state electron configurations
for - Ne (Z 10) Mn (Z 25) Zn (Z 30)
- Eu (Z 63) W (Z 74) Lw (Z 103)
- Identify elements with ground-state
configurations - 1s2 2s2 2p4 1s2 2s2 2p6 3s2 3p6 3d10 4s2 4p6 5s2
4d6 - 1s2 2s2 2p6 Ar 4s2 3d1 Xe 6s2 4f14 5d10 6p5
33Electron Configurations and the Periodic Table
34Some Anomalous Electron Configurations
- Anomalous Electron Configurations Result from
unusual stability of half-filled full-filled
subshells. - Chromium should be Ar 4s2 3d4, but is Ar 4s1
3d5 - Copper should be Ar 4s2 3d9, but is Ar 4s1
3d10 - In the second transition series this is even more
pronounced, with Nb, Mo, Ru, Rh, Pd, and Ag
having anomalous configurations (Figure 5.20).
35Electron Configurations and Periodic Properties
Atomic Radii
36Optional Homework
- Text 5.24, 5.26, 5.28, 5.30, 5.32, 5.34, 5.44,
5.56, 5.58, 5.66, 5.68, 5.70, 5.72, 5.76, 5.78,
5.82, 5.84, 5.94, 5.98, 5.108 - Chapter 5 Homework online
37Required Homework