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Static & Safety Equipment · Heat-Pump Series 4/6

Thermal storage: ice banks, chilled-water tanks & shifting the load

A chiller and the building it cools rarely agree on timing. The cooling load peaks on a hot afternoon, exactly when electricity is dearest and the condenser is hottest โ€” the worst possible moment to be running flat out. Thermal storage breaks that coupling: make the cold when it is cheap and easy, keep it in an insulated tank of ice or chilled water, and pour it back out when the building screams for it. The reward is a smaller chiller, a flatter demand curve, and a fatter bill saving โ€” with an interactive model that flattens a 24-hour load in front of you.

Ice storageChilled-water storageLoad shiftingTon-hoursPeak shaving
★ Heat-pump & refrigeration series
  1. 1. The cycle, COP & the Carnot ceiling
  2. 2. Types & systems: air/water/ground, mini-splits, VRF, large water-to-water
  3. 3. Cooling towers & heat rejection
  4. 4. Thermal storage: ice banks & chilled-water — you are here
  5. 5. Refrigerants: GWP, phase-downs & charging
  6. 6. Condition monitoring & failure modes
⚡ TL;DR

Thermal storage decouples making cold from needing cold. Run the chiller at night โ€” on cheaper power and into a cooler condenser โ€” to charge a store, then discharge that store through the afternoon peak. You get to downsize the chiller toward the average load instead of the peak, and you flatten the demand charge.

Two ways to hold the cold. Chilled water stores sensible heat (a temperature swing) โ€” simple, but a small usable ฮ”T means big tanks. Ice stores latent heat of fusion (334 kJ/kg) โ€” far denser for the same volume, but you must run the evaporator colder to freeze it, which costs a little COP.

Everything is sized in ton-hours (or kWh-thermal). The economics are a straight trade: the tariff arbitrage and demand-charge cut on one side, the ice-making COP penalty on the other. The model below shows a chiller shrinking as you add storage.

1 · Why store cold (or heat)

A conventional plant makes cooling at the exact instant it is used. That sounds efficient until you look at when the use happens: cooling load tracks the sun and the working day, so it climbs through the morning and peaks in the mid-to-late afternoon. Unfortunately that is also when electricity is most expensive (peak time-of-use tariffs and demand charges) and when the outdoor air โ€” the sink the condenser rejects into โ€” is at its hottest, so the machine's COP is at its worst. You are asked to make the most cooling at the moment it is hardest and dearest to make.

Storage rearranges the schedule. If you can make cold ahead of time and bank it, three good things follow at once:

The same logic runs in reverse for heat โ€” a stratified hot-water buffer, a phase-change "thermal battery", or the sensible mass of a district-heating network all let a heat pump charge when conditions favour it and discharge when the building calls. Cold simply happens to be where the money and the equipment are most concentrated, so this guide leans on the cooling case.

2 · Sensible vs latent storage

There are only two physical ways to park thermal energy in a material: change its temperature (sensible heat) or change its phase (latent heat). Every cold store is one or the other.

Qsensible = m · cp · ΔT    Qlatent = m · hsf Water: cp ≈ 4.19 kJ/kg·K, so a usable 8 K swing stores only ~33 kJ/kg. Ice: latent heat of fusion hsf = 334 kJ/kg at 0 ยฐC โ€” about ten times as much energy per kilogram, at constant temperature. That density difference is the whole reason ice storage exists.

Chilled-water storage is sensible. You cool a big volume of water down and let it warm back up on discharge. The catch is the usable temperature difference: chilled-water systems typically supply around 4โ€“7 ยฐC and return around 12โ€“15 ยฐC, so you only have a swing of roughly 6โ€“10 K to work with. A modest ฮ”T means you need a large mass of water โ€” thousands of cubic metres for a serious store โ€” but the water is cheap, benign, and the chiller runs at its normal, efficient evaporator temperature.

Ice storage is latent. Freeze water to ice and you bank 334 kJ for every kilogram, all of it released back at a steady 0 ยฐC as the ice melts. For the same stored energy an ice store is roughly a quarter to a fifth of the volume of a chilled-water tank โ€” decisive when floor space or tank height is tight. The price of that compactness is thermodynamic: to make ice the evaporator must run several degrees below freezing (refrigerant around โˆ’5 to โˆ’10 ยฐC instead of the +1 to +3 ยฐC a chilled-water plant enjoys), and as the Carnot ceiling guarantees, a colder evaporator means a bigger lift and a lower COP. Ice-making typically costs on the order of 10โ€“20 % more energy per ton-hour than chilled-water making โ€” a penalty you accept in exchange for density, tariff arbitrage and a much smaller chiller.

PropertyChilled-water (sensible)Ice (latent)
Stores energy byWarming/cooling water over a ฮ”TFreezing/melting water at 0 ยฐC
Usable densityLow โ€” ~6โ€“10 K swing onlyHigh โ€” ~5× more compact
Evaporator temp neededNormal (~+1 to +3 ยฐC)Sub-freezing (~โˆ’5 to โˆ’10 ยฐC)
Charging COPFull โ€” no penalty~10โ€“20 % penalty
Tank size for a given ton-hourLargeSmall
Best whenSpace is available; COP is pricelessSpace is tight; tariff/demand spread is wide

Why phase change wins on density. This is the same latent-heat idea that carries the refrigerant around the cycle in guide 1 โ€” boiling and condensing move enormous energy at constant temperature. Ice storage simply borrows the trick for the storage medium instead of the working fluid: melt one kilogram of ice and you have absorbed the heat it would take to warm eighty kilograms of water by one degree.

3 · Ice storage: static and dynamic

Because ice is the dense option, it is where most of the interesting engineering sits. There are two families, split by how the ice is formed and released.

Static ice โ€” ice-on-coil / ice bank

The classic and most common form. Submerged coils sit in a tank of water; a cold secondary fluid (usually a glycol/water brine at around โˆ’5 ยฐC) circulates through the coils during charging, and ice grows outward on the coil surface until much of the tank is frozen into a solid block around the tubes. To discharge, you reverse the heat flow โ€” warm return fluid runs through the same coils (or the building's chilled water passes through a heat exchanger) and melts the ice from the inside out, delivering near-0 ยฐC cooling. Nothing physically moves except the fluid; the ice stays put. It is robust, simple, and forgiving, which is why "ice bank" is almost a generic term.

The one subtlety is that ice is a poor conductor. As the ice layer thickens on the coil, it insulates the fresh water beyond it, so the charging rate slows and the brine has to run colder to keep freezing โ€” the COP penalty grows toward the end of the charge. Good designs stop short of a total freeze-up to keep that penalty in check.

Dynamic ice โ€” harvesting and slurry

Dynamic systems keep the ice thin or fluid so the insulating-layer problem never bites. Ice harvesting freezes a thin sheet on a plate evaporator, then briefly reverses to hot gas to shear the sheet off; the flakes drop into a storage tank of water below. Because the ice is always thin at the moment of formation, the evaporator can stay comparatively warm and the charging COP holds up better than a fully-frozen ice bank. Ice slurry systems go further and generate a pumpable suspension of micro-crystals in water or brine โ€” effectively a "cold fluid" you can move through pipes and meter precisely, with a very high heat-transfer rate on discharge. The trade is mechanical complexity: harvesters cycle a defrost, and slurry generators need scraped-surface or supercooling hardware, so there is simply more to maintain than a tank of coils.

Why the COP penalty is still worth paying. Making ice costs you maybe 15 % more energy per ton-hour โ€” but that energy is bought at the night tariff (often less than half the peak rate) and made at a higher COP than a hot-afternoon condenser would allow, and it lets you cut the demand charge and buy a smaller chiller. In most commercial tariffs the arbitrage and demand savings dwarf the efficiency penalty. The model in section 6 lets you see where that balance tips.

4 · Chilled-water & stratified tanks

Where floor space allows and the COP penalty of ice is unwelcome, a plain tank of chilled water is the elegant answer โ€” and its central trick is stratification. Cold water is denser than warm water, so if you feed and draw carefully it will layer itself: cold at the bottom, warm at the top, with a thin transition zone between them called the thermocline. Charge by pushing cold supply in at the bottom and drawing warm off the top; discharge by doing the reverse. A single tank thus behaves like two โ€” a cold reservoir and a warm reservoir separated only by that mobile boundary โ€” with no membrane or moving part.

The whole art is keeping the thermocline thin. A sharp boundary means almost all the stored water is delivered at full useful coldness; a thick, mixed thermocline blurs cold and warm together and wastes capacity. That is why stratified tanks use carefully engineered low-velocity diffusers at top and bottom to spread the flow gently and avoid stirring. A tall, slim tank stratifies better than a short, wide one, because the buoyant boundary has less area to smear across.

Buffer tanks โ€” a reliability win, not just storage

Not every tank exists to shift load by hours. A much smaller buffer tank (or "volumiser") solves a different and very common problem: on a light cooling load, a chiller with too little water in its loop satisfies the setpoint almost instantly, shuts off, then restarts moments later โ€” short-cycling. Every start is hard on a compressor: inrush current, poor oil return, and thermal cycling all accelerate wear, and the machine never runs long enough to reach steady efficiency. A buffer tank adds thermal mass and flywheels the loop, so the chiller runs in longer, smoother cycles and starts far less often.

That makes the humble buffer tank a genuine reliability component, not merely an energy one. Short-cycle count is one of the cleanest early-warning signals a condition-monitoring platform can trend: a rising start frequency on a compressor is often the first sign of an undersized loop, a failing control, or a load that has drifted away from the design point โ€” a theme the final guide in this series picks up in full.

5 · "Ice chests" in the real world

The idea of a big insulated box of cold that you fill and draw down is everywhere once you look for it. Some run for hours, some for months:

All of them are sized in the same currency: ton-hours (one ton of refrigeration sustained for one hour, โ‰ˆ 3.517 kWh-thermal) or directly in kWh-thermal. A store rated at 2,000 ton-hours can deliver 500 tons for four hours, or 250 tons for eight โ€” capacity and discharge rate are separate specifications, and both matter. A store that holds plenty of energy but cannot discharge it fast enough to cover the peak is as useless as one that discharges fast but empties in twenty minutes.

6 · The economics — where the trade tips

Strip away the hardware and thermal storage is a financial instrument: you are arbitraging the price of electricity across the day and buying down your demand charge, and paying for it with a modest efficiency penalty and some capital. Three numbers decide whether it pays:

There is a fourth, harder to price but real: resilience. A charged store is a few hours of cooling you already own โ€” a ride-through if the grid dips or a chiller trips, and a hedge against demand-response events. Put the first three on a 24-hour profile and watch the peak flatten:

Interactive — flattening the day with storage

Live model
The afternoon spike a no-storage plant must be sized for
Ton-hours the store can hold and discharge
Cheap-power hours from 22:00 for charging
Chiller needed
โ€”t
was โ€” t
Chiller downsized
โ€”%
โˆ’ โ€” t of peak
Storage used
โ€”t·h
of โ€” tยทh
Daily bill saving
โ€”%
energy + demand
The 24-hour load, flattened
Store charges at night, discharges through the peak
cooling loadchiller outputchargedischarge
Daily cost: no storage vs storage
Energy shifts to night; demand shrinks
energydemand charge
Model: a fixed afternoon-peaking load profile is scaled to the peak-load slider. With storage the chiller output is capped at the smallest size C* whose stored shortfall Σmax(loadโˆ’C*,0) fits the store; the deficit is discharged at the peak and recharged during the cheapest hours (greedy price dispatch), with a 1.10× ice-making energy penalty on charging. Cost = energy (night rate 0.45× day) + a demand charge set at 40 % of the no-storage bill. Illustrative โ€” real projects model real tariffs, part-load COP and storage losses.

Two patterns show up as you play. Add storage and the chiller line drops toward the average load while the blue night-charging block grows and the red afternoon-discharge block does the peak-shaving work. Widen the night-tariff window and more of that charging lands on cheap power, so the saving climbs even though the chiller size does not change. There is a knee, though: past the point where the store can fully level the day, extra ton-hours stop shrinking the chiller and only buy a little more arbitrage โ€” the classic partial-storage sweet spot, where a store sized to shave the peak (not to carry the entire load) gives most of the benefit for a fraction of the tank.

7 · Maintenance & monitoring

A thermal store is mostly a tank, a heat exchanger, and a control scheme โ€” which means its failure modes are quiet and slow, and easy to miss until capacity has silently bled away. The things to watch:

Key takeaways

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