s-Block Chemistry Flashcards
Ionic model
Ions re assumed to be hard spheres with fixed sizes held together by electrostatic interactions, the radii of spheres are known as ionic radii.
Internuclear distance
Can be measured by x-ray crystallography but it is hard to determine individual radii as hard to know when electron density stops and starts. Ionic radii change depending on the compound.
Trends in ionic radii
Anions>cations
Increase down a group; Increase in PQN
Dicationmonoanion
Lattice Enthalpy
Enthalpy change for the conversion of 1 mol of the ionic solid into the gaseous state
ΔU in the ionic model:
-ΔlattH° in the ionic model comes from electrostatic interactions between ions, by considering these interactions in an ionic solid you can obtain a theoretical value
ΔU = -(z- z+ e^2)/(4 π εo r)
Madelung constant
in a crystal there are repulsive and attractive interactions in all directions to account for this the Madelung constant is introduced as well as Avogadro’s number
ΔUlatt = +(A Na z- z+ e^2)/(4 π εo r)
Lattice energy is the -ve of this potential so the +ve sign is now included
Born-Lande Equation
The prior expression assumes ions are point charges; additional short range forces need to be included from overlapping electron clouds, these increase as)decreases.
+(A Na z- z+ e^2)/(4 π εo r)(1-1/n)
The born exponent is an average of an n value obtained by comparing the compressibility of a solid based on its occupied orbitals.
ΔU/ΔH
All prior calculations give internal energy changes, ΔU, however ΔH is heat change at constant pressure, they are related by: ΔH = ΔU + pV; the difference is so small hence can be ignored
Calculating the Madelung constant
The first attractive energy equation is used, times by the # of nearest neighbours, r is calculate during extended Pythagoras theorem. Include sign +/- !!!
d = (2r^2)^1/2 d = (3r^2)^1/2
ΔU = ΔU1 + ΔU2 + ΔU3 …
The terms alternate in sign and are of high but decreasing magnitude.
Deviations from the ionic model
+ve charges distort electron clouds of anions, large and small charged ions are more easily polarisable. highly charged small cations bonded to large charge diffuse anions have the greatest degree of covalent character.
The BL eq. underestimates ΔUlatt high covalent character compounds.
ΔUlatt(BH) ≈ ΔUlatt(BL) -> low covalency
ΔUlatt(BH) > ΔUlatt(BL) -> high covalency
Kapustinskii Equation
A simplification of the Born-Lande equation;
ΔUlatt = (k ν z+ z-)/(r+ + r-)
Where k = 107900, ν = no. ions in the formula units
Thermochemical radii of polyatomic ions can be calculated in this way
van Arkel-Ketelaar triangles
Predict the bonding type for a binary compound;
Metallic ^^ Ionic ^^ Covalent
X-axis - Average electronegativity
Y-axis - Difference in electronegativity
When both χ’s are high –> covalent, when high Δχ –> ionic
Hydrogen
H2 is colourless and odourless, MP: -259°C, BP: -253°C (low/weak IM forces), low Mr, lowest density of all gases (0.082gdm-3). Unreactive at RTP (H-H 436JKmol-1) with the exception of O2, F2 and Cl2.
Production of H2
Steam reforming: methane + water -> carbon monoxide + 3hydrogen (NiO/850°C)
Shift reaction: CO + H2O -> CO2 + H2 (Fe/450°C)
Electrolysis of H2O: 2H20 -> 2H2 + O2
Use of hydrogen
Mainly used in the Haber process (53%), in the petrochemical industry, for extraction of metals from ores and in ethanol production (17%)