s-Block Chemistry Flashcards
(35 cards)
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%)
Hydrides
Hydrogen forms binary compounds called hydrides with most elements; χH>χR (R is electropositive) the H atom is hydride and has an oxidation state of -1. If χH
Hydridic Hydrides
Hydridic hydrides are formed by group 1 & 2 and are ionic structures, strongly basic
RH + H2O -> ROH + H2
Reactivity with water increases down the group hence they are kept under inert atmospheres.
Protic hydrides
Covalent not ionic as ionisation (1312KJmol-1) »_space; electron gain (-73KJmol-1) hence H+ difficult to produce. Only formed when dissolved in a solvent that can solvate H+; the compound here acts as an acid
Non-polar hydrides
(χH≈χR) may have a small dipole: i.e. in CH4 H=δδ+ and in B2H6 H=δδ-
Nomenclature of hydrides
Hydridic hydrides -> hydridides
Protic hydrides/Non-polar hydrides -> R-ane
Group 16&17 ->hydrogen R-ide
Trivial names - Ammonia, water
Covalent Hydrides
Electron precise compounds - All valance electrons are involved in bonding (group 14)
Electron deficient compounds - 3-centre-2-electron bonds (group 13)
Electron rich compounds - Not all electrons on the central atom are involved in bonding (lone pairs) hence can act as lewis bases (groups 15-17)
Acidity of hydrides
Increases across a period (Δχ increases) and increases down group (decrease in BDE, decreasing attraction between X and H3O+)
HX + H2O –> H3O+ X-
BDE of hydrides
Increases from left to right due to an increase in ionic contribution as χX increases. Decrease down group as valance orbitals get larger and more diffuse as PQN increases therefore ns np interactions with H 1s are reduced.
Isotope effects of hydrides
Protium/deuterium/tritium
H^2 Has twice the mass of H^1 hence its properties will vary considerably, D2O ice sinks as it is more dense,
BDE of D2 443>H2 436 therefore more energy is needed to break X-D that X-H; the lowest vibrational energy state for D2 is lower than for H2