Heating a shower tank with portable TCES?

Kragen Javier Sitaker, 02021-08-11 (updated 02021-08-15) (6 minutes)

The shower tank in Mina’s bathroom holds 25 ℓ, though a typical shower is more like 20 ℓ, and the water is preheated by a gas on-demand heater. Unfortunately the plumbing was apparently done by the same idiot or would-be murderer who installed the deadly fake electrical system, because the water arrives at the shower tank at a lukewarm temperature of about 30°. Raising it to a luxurious 41° would be desirable; currently I do this by pouring boiling water into the top from a pot.

If we disregard the variation of water’s specific heat over the relevant range, v₀t₀ + v₁t₁ = 41° 20 ℓ, t₀ = 30°, t₁ = 100°, and v₀ + v₁ = 20 ℓ, so v₁ = 20 ℓ - v₀ and we have 30°v₀ + 100°(20 ℓ - v₀) = 41° 20 ℓ = (30° - 100°)v₀ + 100°20 ℓ, so v₀ = (41° - 100°)20 l / (30° - 100°) = (41° - 100°)/(30° - 100°)20 ℓ = (59/70)20 ℓ = 16.9 ℓ, so 3.1 ℓ is the amount of boiling water to add, and indeed lerp(30°, 100°, 3.1ℓ/20ℓ) is 40.85°. If it’s just a matter of adding energy to 20 ℓ of 30° water, though, it’s 921 kJ.

But maybe we could use a much smaller heating unit using TCES, for example with muriate of lime (see file muriate-thermal-mass.md in Derctuo) sealed in a sturdy plastic bag. The idea is that you have some kind of “heat pack” that you dunk in the tank, then activate, and it adds 921 kJ of heat to the water, and you have a nice shower and then fish it out of the tank and go recharge the heat pack.

How small can 921 kJ be? Fully hydrating the anhydrous salt to the hexahydrate gives you (2608.01 - 795.42 = 1812.59) kJ/mol (at 110.983 g/mol, that’s 16.3321 kJ/g), but I think you can get further heat by dissolving the salt and diluting the solution; I’m not sure. 6 mol of water weighs 108.09 g, 2% less than the mass of the anhydrous salt it would fully hydrate, dropping the energy density of the heat pack to about 8.1 kJ/g.

This would give us a 114-gram heat pack, which is a lot less than the 3.1 kg of boiling water.

It wouldn’t quite work that well, though: the hexahydrate dehydrates to the tetrahydrate above 30°, and the tetrahydrate only has an enthalpy of formation of -2009.99 kJ/mol, leaving only 1214.57 kJ/mol — a third of the stored heat is inaccessible at temperatures above 30°. We need less water, though, only 72.06 g/mol. So you get 1214.57 kJ per 183 g of heat pack, or 6.6 kJ/g, pushing the heat pack mass up to 140 g.

This same phenomenon limits the temperatures the heat pack will expose its envelope to. The various hydration forms have these characteristics, according to wikipedia and my calculations:

| H₂O |           | decomposition    | enthalpy of formation |              |            |            |                |              |
|-----+-----------+------------------+-----------------------+--------------+------------+------------+----------------+--------------|
|   0 | 2.15 g/cc | 772–775° (melts) | -795.42 kJ/mol        | 110.98 g/mol | 0          | 8.274 kJ/g | 72.89 J/mol/K  | 0.6568 J/g/K |
|   1 | 2.24 g/cc | 260°             | -1110.98 kJ/mol       | 129.00 g/mol | 2.446 kJ/g | 5.828 kJ/g | 106.23 J/mol/K | 0.8235 J/g/K |
|   2 | 1.85 g/cc | 175°             | -1403.98 kJ/mol       | 147.01 g/mol | 4.140 kJ/g | 4.134 kJ/g | 172.92 J/mol/K | 1.176 J/g/K  |
|   4 | 1.83 g/cc | 45.5°            | -2009.99 kJ/mol       | 183.04 g/mol | 6.636 kJ/g | 1.638 kJ/g | 251.17 J/mol/K | 1.372 J/g/K  |
|   6 | 1.71 g/cc | 30°              | -2608.01 kJ/mol       | 219.07 g/mol | 8.274 kJ/g | 0          | 300.7 J/mol/K  | 1.373 J/g/K  |

The two reversed columns of energy density say that, for example, the tetrahydrate (plus the water to hydrate it the rest of the way) is an energy store of 1.638 kJ/g, but in hydrating the anhydrous salt to the tetrahydrate we produced 6.636 kJ/g of heat. If that heat couldn’t go anywhere else, it would have raised the temperature of the resulting material by 4837°; the reason this salt doesn’t explode is that it stops absorbing water once it gets warm enough.

In particular, the corresponding calculation for the monohydrate produces a result of 2970°, so if water is limited enough, even in a small region, you should be able to reach 260° by hydrating the muriate of lime.

For a plastic bag, this might be bad; nylon 6 melts at 220° and nylon 6,6 melts at 264°, and those are the likely plastics available in a supermarket oven bag. It would also be a problem if one part of the material reached 100° while nearby some water was still pure — the water might boil, float the bag, and burst the bag with steam pressure. So it might be best to compromise on energy density in order to limit the maximum possible temperature; while in theory you could do this by diluting anhydrous muriate of lime with glass beads or something, I think it’s probably better to mix together two hydration levels to set the maximum temperature they can reach when fully hydrated to below 100°.

Drying the muriate for reuse can be tricky; a 01964 US patent 3,339,618A describes the situation at the time. The guy had come up with a spray-drying process using 370° air to produce anhydrous calcium chloride.

A different source gives a much lower enthalpy for hydrating muriate of lime. A third source mentions that through repeated cycling, some amount of the salt will hydrolyze into marine acid air; I’d think that a small amount of chalk in the mix would be adequate to prevent this, but they seem to think it’s a harder problem.

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