Binding (or Cohesive) EnergyDenition and Constraints
The binding or cohesive energy c of a substance (either liquid or solid) is theenergy required to break all the bonds associated with one of its constituent
molecules. It is, therefore a measure of the inter-molecular energy for asubstance. We spend time considering these numbers because they form thebasis for many OOM estimates, from density to sound speed to heat capacity.
We know that intra -molecular bonds that hold atoms together in a molecule(e.g. the O-H bond in water) are generally much stronger than inter-molecularbonds. After all, when you heat water, it boils to form water vapor, but thewater molecules do not decompose into, say, O2 and H2 . This means thatthe thermal energy of H2 O even at high temperature is not enough to breakthe intra-molecular bonds, thus implying that these intra-molecular bonds
are stronger than those holding the substance together.
Here's a table of typical energies for such bonds:
Bond Bond energy (eV)
C-C
6.3
H-H
4.5
O-H
4.4
Na-Cl
4.3
Fe-O
4.0
Thus, whatever we estimate to be the cohesive bond strengths for liquids
and solids, the values should be smaller than these!

Liquids
This represents the energy required to separate a molecule from the liquid
phase and transfer it to the vapor phase. This represents almost entirely theinter-molecular binding energy of the liquid molecules, since this energy ingases is extremely small (and in fact zero for ideal gases).

1

Liquid∆Hvap (kJ/mol) c (eV per molecule)
Water
410.4
Ammonia
230.2
Butane210.2
Ethanol39
0.4
Methane8.20.08
Propane16
0.2
From these values, we can estimate the binding energies as shown in theTable, which is simply converting from units of kJ/mol to eV per molecule.
Note that this conversion is almost exactly 10−5 (eV per molecule) / (kJ/mol).
We conclude, then, that the binding energies in liquids range from 0.1 to0.4 eV, depending on the polarity of the molecules. Molecules that havegreater permanent dipoles (i.e. one end strongly positive, one end strongly
negative, as in water where the oxygen is strongly negative and the hydrogenspositive). If you know nothing about the liquid, 0.2 eV is a reasonable ruleof thumb that gets you within a factor of 2. Note that these values aremuch smaller than the intra-molecular bond energies, so we've satised that
constraint. Note that in order to properly compare these values, one should
determine how many neighbors a typical liquid molecule has, and divide thecohesive energies in the table above by that number of neighbors to estimate
the energy of a single molecule-molecule interaction.

SolidsFor solids, we can play the same game, although one disadvantage of thismethod is that for many solids of interest (like rocks), heats of vaporization
are not readily available. Below are some values for elements.
If you focus only on the solid elements, you can see that values range from100 (sodium) to 800 (tungsten) kJ/mol, with typical values in the rangeof 300 to 400 kJ/mol for the most common elements like Al, C, Si, Fe,
Ni and Cu. This gives metal binding energies that are about an order ofmagnitude larger than that for liquids, i.e. c ∼3 to 4 eV. (Note that for atypical molecule in a solid with 6 neighbors, this yields values of ∼0.5 eV
per bond, which again is smaller than the intra-molecular bond energies andtherefore strikes us as reasonable.) In reality, these numbers are a bit high,perhaps because vaporization of many solids occurs at temperatures of order
103 K, which is far enough from room temperature as to make these heats2

of vaporization not directly relevant to room temperature cohesive energies
without some correction. Sanjoy's estimates of c ∼1 to 2 eV for a typicalcohesive energy is probably a bit better, so we can use these as representativevalues for solids.

Figure 1:3