Week 5 Flashcards
Core Electrons
- Electrons in these orbitals are unaffected by the presence of neighbouring atomic nuclei
- Their energy is practically the same as in an isolated atom
σ or single covalent bonds.
- Electrons in these orbitals are delocalised between neighbouring nuclei.
- The electron density is highest along the internuclear axis.
Non-bonding (nb) orbitals
are localised on only one atom and do not affect bonding.
π bonds
- Electrons in these orbitals lower the energy of the molecule.
- They are delocalised between multiple nuclei in lobes on opposite sides of the internuclear axis.
- They are responsible for double and triple bonds
Total number of atomic orbitals =
number of molecular orbitals
Bond order =
½ (No. of bonding electrons − No. of antibonding electrons)
From ethane to adamantane
increasing # of atoms, increases # of molecular orbitals.
1 C-C σ anf 1C-C σ star becomes
12 C-C σ and 12 C-C σ star
From adamantine to diamond
Keep growing, so many energy levels it becomes like a continuom.
Refer to the levels as a band
occupied levels = valence band
unoccupied levells = conduction band
Band gap
Gap between the valence and conduction band
* Minimum energy a network solid must absorb to promote an electron from the valence band to the conduction band.
Silicon
- Small band gap
- Absorbs all visible light
- Appears black
Diamond
- Large band gap
- Absorbs no visible light
- Appears transparent
- No conductivity - band gap too big
In order for an electron to conduct electricity…
It must have access to an unoccupied energy level.
Allotropes of Carbon
Graphite (highly conducting, low density) and diamond (insulator, high density)
Conduction in metals
Metals do not have a band gap. Valence and conduction bands overlap, so metals can conduct electricity
Insulator
- Large band gap – electrons cannot be promoted to conduction band
- Does not conduct electricity, no way the electron could jump
Intrinsic semiconductor
Band gap is small, electrons can be promoted to the conduction band, leaving electrons in the conduction band and holes in the valence band.
* e.g. silicon, germanium.
* Allows electrons in the valence band to jump in this hole
* Conductivity in both bands
Extrinsic semiconductor
Many applications require stable conductivity at all temperatures.
* This can be achieved by doping – substituting some atoms (something added to the material).
* There are two types of doping – n-type and p-type
n-type doping
- There are extra negative charge carriers, (i.e. electrons).
- Achieved by substituting with an element to the right on the periodic table, which has more electrons.
- Don’t need as much energy
- Extra electrons reside in donor levels, just below the conduction band, heat moves them into this band
p-type doping
- Fewer electrons, and more positive charge carriers, (i.e. holes).
- Achieved by substituting with an element to the left on the periodic table, which has fewer electrons.
- The electron poor atoms generate acceptor levels, just above the valence band, valence band electrons are promoted here, leaving holes in the valence band.
Solar cells
can be generated by combining an intrinsic semiconductor with both p-type and n-type extrinsic semiconductors
generating solar cells
- Electrons travel to the conduction band of the n-type semiconductor.
- As electrons move, the holes left by electrons in the valence band also change position
- The absorption of light promotes electrons from the valence to the conduction band of the intrinsic semiconductor
Spectroscopy
The study of the interaction of matter with electromagnetic radiation.
white light is
a combination of all colours.
absorb no visible light
black materials
absorb all the visible light shone on them
how we see colours due to absorbance
A solid that absorbs red light and reflects all the other colours will appear green