6.2 Quantized Energy and Photons
- German physicist, Max Planck energy can be released by atoms only in "chunks" of some minimum size
- Quantum
smallest quantity of energy that can be emitted or absorbed as electromagnetic radiation
- E=hv (h=plancks constant=6.63 x 10-34 J-s)
6.2.1 The Photoelectric Effect
- photoelectric effect when photons strike a metal surface, electrons are emitted
6.3 Bohrs Model of the Hydrogen Atom
6.3.1 Line Spectra
- monochromatic radiation with a single wavelength
- spectrum created when radiation is divided up into its wavelengths
- continuous wavelength rainbow of colors containing light of all wavelengths
- line spectrum spectrum containing radiation of specific wavelengths
- Johann Balmer:
- n
= C(1/22 1/n2) n = 3,4,5,6
- C = 3.29 x 1015 s-1
6.3.2 Bohrs Model
- electrons could circle the nucleus only orbits of specific radii
- En = (-RH)(1/n2) n = 1,2,3,4
- RH = Rydberg constant = 2.18 x 10-18 J
- n = principle quantum number
- gound state lowest energy level
- excited state electrons in a higher energy level
- E¥
= (-2.18 x 10-18 J)(1/¥
2) = 0
- Electrons can jump to a higher energy state by absorbing energy
- r
E = Ef EI = hn
- ni and nf are the principle quantum numbers of the initial and final states of the atom
- n
is positive when ni <
nf (energy is absorbed)
- v is negative when ni >
nf (electron jumps from higher to lower state)
- frequency of electromagnetic radiation must be a positive number
- "-" sign indicates that light is emitted
6.4 The Wave Behavior of Matter
- De Broglie: wavelength of the electron or any particle depends on its mass, m and velocity, v
- l
= h/mv
- mv = momentum
- matter waves describe the waves characteristics of material particles
6.4.1 The Uncertainty Principle
- it is impossible to know simultaneously both the exact momentum of the electron and its exact location in space
6.5 Quantum Mechanics and Atomic Orbitals
- wave functions - y
(has no physical meaning)
- probability density
- y
2, probability that the electron will be found at the location proposed
- electron density
regions where there is a high probability of finding the electron
6.5.1 Orbitals and Quantum Numbers
- 1) principal quantum number, n, can have integral values of 1,2,3,4
- n increases orbital becomes larger
- 2) azimuthal quantum number, l, can have integral values from 0 to n-1
- defines the shape of the orbital
- 3) magnetic quantum number, ml, can have integral values between l and l, and 0
- describes orientation of orbital
- electron shell
collection of orbitals with the same value of n
- subshell
orbitals that have the same n and l values
- 1) shell with principal quantum number n will consist of exactly n subshells
- 2) each subshell consists of a specific number of orbitals
- 3) the total number of orbitals in a shell is n2, n = principle quantum number of shell
6.6 Representation of Orbitals
6.6.1 The s Orbitals
- spherically symmetric
- nodes
intermediate regions where y
2 goes to zero
- number of nodes increases as n increases
6.6.2 The p Orbitals
- two lobes
- orbitals of a given subshell have same size and shape but differ in spacial orientation
6.6.3 The d and f Orbitals
- 5 d orbitals, 4 of which are "4 leaf clover" shaped
- one has two lobes and a "doughnut" shape in the middle
- 7 f orbitals
6.7 Orbitals in Many-Electron Atoms
6.7.1 Effective Nuclear Charge
- effective nuclear charge net positive charge attracting the electron
- Zeff = Z S (Zeff = effective nuclear charge, Z = number of protons, S = average number of electrons
- Screening effect inner electrons shield outer electrons from full charge of nucleus
6.7.2 Energies of Orbitals
- In a many-electron atom, for a given value of n, Zeff decreases with increasing value of l
- in a many-electron atom, for a given value of n, the energy of an orbital increases with increasing value of l
- degenerate
orbitals with the same energy
6.7.3 Electron Spin and the Pauli Exclusion Principle
- George Uhlenbeck and Samuel Boudsmit proposed the electron spin
- Electron spin quantum number, ms can only have values of +0.5 and 0.5
- Pauli exclusion principle no two electrons in an atom can have the same set of four quantum numbers n, l, m1, and ms
- An orbital can hold a maximum of two electrons, and they must have opposite spins
6.8 Electron Configuration
- electron configuration the way electrons are distributed in orbitals
- orbital diagram
a box with each electron represented by a half arrow (arrow pointing=electron with positive spin, arrow pointing down=electron with negative spin)
6.8.1 Periods 1,2, and 3
- Hunds rule for degenerate orbitals, the lowest energy is attained when the number of electrons with the same spin is maximized
- Valence electrons
outer shell electrons
- Core electrons
electrons in the inner shells
6.8.2 Period 4 and Beyond
- transition elements or transition metals 4th row of the periodic table
- lanthanide elements
- elements 58-71 (rare-earth)
- actinide elements
last row of periodic table
6.9 Electron Configurations and the Periodic Table
- the periodic table is your best guide to the order in which orbitals are filled
- chromium is [Ar]4s13d5 rather than [Ar]4s23d4
- copper [Ar]4s13d10 rather than [Ar]4s23d9