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Transcript
CHAPTER 9
Molecules
Why do molecules form?
Molecular bonds
Rotations
Vibrations
Spectra
Complex planar molecules
Johannes Diderik van der Waals
(1837 – 1923)
“Life ... is a relationship between molecules.”
Linus Pauling
Remember: homework due this Wednesday by 2:30pm in room 144
Molecules are combinations of atoms.
When more than one atom is involved, the potential and the wave
function are functions of way more than one position (a position
vector for each nucleus and electron):
V  V (r1 , r2 ,..., rN ; r1, r2,..., rM )
  (r1 , r2 ,..., rN ; r1, r2,..., rM , t )
Electrons’ positions
Solving the Schrodinger Equation in
this case is even harder than for
multi-electron atoms.
Serious approximation methods are
required.
This is called Chemistry!
Nuclei positions
Molecular Bonding and Spectra
Nucleus
The only force
that binds atoms
together in
molecules is the
Coulomb force.
Nucleus
E 0
Electron cloud
Electron cloud
But aren’t most atoms electrically neutral? Yes!
Indeed, there is no attraction between spherically symmetrical
molecules—the positive and negative charges both behave like
point sources and so their fields cancel out perfectly!
So how do molecules form?
Why Molecules Form
Most atoms are not spherically
symmetrical.
For example, these two “atoms”
attract each other:
Atom #1
Atom #2
+
+
-
This is because the distance between opposite charges is less
than that between charges of the same sign.
The combination of attractive and repulsive forces creates a
stable molecular structure.
Force is related to the potential energy surface, F = −dV/dr, where
r is the position.
Charge is distributed very unevenly in
most atoms.
The probability density for the hydrogen atom for three different
electron states.
Closed shells of electrons are very
stable.
Atoms with closed shells (noble gases) don’t form molecules.
Ionization energy (eV)
Noble gases (difficult to
remove an electron)
Atomic number (Z)
Atoms with closed shells
(noble gases) also have the
smallest atomic radii.
Atomic radius (nm)
Atoms like closed
electron shells.
Atomic number (Z)
But add an extra electron, and it’s weakly bound and far away.
An extra electron or two outside a
closed shell are very easy to liberate.
Atoms with one or two (or even more) extra electrons will
give them up to another atom that requires one or two to
close a shell.
Atoms with extra
electrons are said to
be electropositive.
Those in need of
electrons are
electronegative.
Ionic Bonds
An electropositive atom gives up
an electron to an
electronegative one.
Example: Sodium (1s22s22p63s1)
readily gives up its 3s electron
to become Na+, while chlorine
(1s22s22p63s23p5) easily gains
an electron to become Cl−.
Covalent Bonds
Two electronegative atoms
share one or more electrons.
Example: Diatomic molecules
formed by the combination of
two identical electronegative
atoms tend to be covalent.
Larger molecules are formed
with covalent bonds.
Diamond
Metallic Bonds
In metals, in which electrons are very weakly bound, valence
electrons are essentially free and may be shared by a number of
atoms. The Drude model for a metal: a free-electron gas!
Molecular Potential
Energy Curve
The potential depends on the
charge distributions of the atoms
involved, but there is always an
equilibrium separation
between two atoms in a
molecule.
The energy required to separate
the two atoms completely is the
binding energy, roughly equal
to the depth of the potential well.
Vibrations are excited thermally, that is, by collisions with other
molecules, or by light, creating superpositions of ground plus an
excited state(s).
Molecular Potential
An approximation of the force felt by one
atom in the vicinity of another atom is:
A B
V n- m
r
r
where A and B are positive constants.
Because of the complicated shielding effects of the various electron
shells, n and m are not equal to 1. One example is the Lennard-Jones
potential in which n = 12 and m = 6.
The shape of the
curve depends on
the parameters
A, B, n, and m.
Vibrational Motion: A Simple Harmonic
Oscillator
The Schrödinger Equation can be
separated into equations for the positions
of the electrons and those of the nuclei.
The simple harmonic oscillator accurately
describes the nuclear positions of a
diatomic molecule, as well as more
complex molecules.
Vibrational States
The energy levels are
those of a quantummechanical oscillator.
Evibr  (n  1 2) 
n is called the
vibrational quantum
number. Don’t
confuse it for n, the
principal quantum
number of the
electronic state.
Vibrational-transition
selection rule:
Dn = ±1
The only spectral line is  !
However, deviations from a perfect
parabolic potential allow other
transitions (~2, ~3, …), called
overtones, but they’re much weaker.
Vibrational Frequencies for Various Bonds
Different bonds have different vibrational frequencies (which are
also affected by other nearby atoms).
← Higher energy (frequency)
Wavenumber (cm-1)
Notice that bonds containing Hydrogen vibrate faster because H is
lighter.
Water’s Vibrations