This calculator estimates the thermal energy that can be stored in a phase change material (PCM) as it is heated from an initial temperature, passes through its melting point, and reaches a higher final temperature. It combines sensible heat (temperature change in solid and liquid phases) with latent heat (the energy absorbed during melting) and then applies an optional efficiency factor to account for real-world losses.
Use it to compare different PCMs, size storage for building or equipment applications, or sanity-check manufacturer datasheet values. The tool assumes that the material starts fully solid below its melting temperature and ends fully liquid at or above its melting temperature.
The total ideal thermal energy stored in a PCM that is heated from an initial temperature below its melting point to a final temperature at or above its melting point is:
Eideal = m [ cs(Tm − Ti) + L + cl(Tf − Tm) ]
where:
The usable stored energy accounts for losses such as imperfect heat transfer, tank insulation, and control strategy. It is approximated by:
Eusable = η · Eideal
where η is the storage efficiency (between 0 and 1).
The same relationship in accessible MathML form is:
The calculator reports energy in kilojoules (kJ) and converts to kilowatt-hours (kWh) using:
1 kWh = 3,600 kJ
The output gives you an estimate of the total thermal energy that can be stored during one full charge cycle under the stated temperature range.
In many applications, the latent term is the main reason for using a PCM. A high latent heat value allows significant storage over a narrow temperature range, which is useful when you need stable operating temperatures (for example, around room temperature in buildings or around specific setpoints in electronics).
Consider 100 kg of a paraffin wax PCM used for building thermal storage. Assume:
Step 1: sensible heating in solid phase:
ΔTsolid = Tm − Ti = 60 − 20 = 40 °C
Esolid = m · cs · ΔTsolid = 100 · 2.1 · 40 = 8,400 kJ
Step 2: latent heat at melting:
Elatent = m · L = 100 · 200 = 20,000 kJ
Step 3: sensible heating in liquid phase:
ΔTliq = Tf − Tm = 70 − 60 = 10 °C
Eliq = m · cl · ΔTliq = 100 · 2.4 · 10 = 2,400 kJ
Step 4: total ideal stored energy:
Eideal = 8,400 + 20,000 + 2,400 = 30,800 kJ
Step 5: usable stored energy with efficiency:
Eusable = η · Eideal = 0.8 · 30,800 = 24,640 kJ
Convert to kWh:
Eusable,kWh = 24,640 / 3,600 ≈ 6.84 kWh
This means that, under these conditions, the PCM bank can store roughly the same energy as a 1 kW electric heater running for almost 7 hours. You can adjust mass, temperature range, or material properties in the calculator to explore different designs.
The table below shows indicative properties for a few common PCMs. Actual values depend on grade, additives, and supplier data, so always consult product datasheets before final design.
| Material | Melting point (°C) | Latent heat (kJ/kg) | Typical use case |
|---|---|---|---|
| Paraffin wax | 50–60 | 180–220 | Building envelopes, wallboards, compact thermal storage near room temperature |
| Sodium acetate trihydrate | ≈ 58 | 240–270 | Reusable heat packs, low-temperature storage, comfort heating |
| Calcium chloride hexahydrate | ≈ 29 | 170–200 | Cooling and comfort conditioning slightly above freezing |
| Erythritol | ≈ 118 | 300–360 | Higher-temperature storage, solar thermal, industrial processes |
Organic PCMs like paraffin waxes are chemically stable and non-corrosive but have low thermal conductivity. Salt hydrates provide higher volumetric storage but may need additives or encapsulation to control issues such as phase separation or supercooling. The efficiency factor in the calculator lets you experiment with how such practical limitations might reduce usable energy.
PCMs are often compared with conventional sensible heat storage (for example, water tanks or concrete slabs). A simplified comparison is shown below.
| Aspect | Phase change materials | Sensible heat materials (water, concrete) |
|---|---|---|
| Energy density near setpoint | High, due to latent heat at nearly constant temperature | Moderate; requires larger temperature swings |
| Operating temperature range | Narrow around melting point, tunable via material choice | Broad; energy stored over wide temperature differences |
| Control of output temperature | Good; temperature remains close to melting point during phase change | Varies; outlet temperature depends strongly on charge level |
| Design complexity | Higher; may need encapsulation, additives, and careful integration | Lower; uses well-known materials and system designs |
| Typical applications | Building temperature smoothing, electronics cooling, compact storage | Hot water systems, large thermal tanks, building thermal mass |
The calculator focuses on the PCM case, but you can conceptually compare the kWh results with a sensible-heat-only system using E = m·c·ΔT for a reference material such as water.
The model behind this tool is intentionally simple and has important assumptions:
Because of these simplifications, the results should be treated as a first-order estimate. For critical systems, use detailed thermal modeling and experimental validation.
Pick a melting temperature close to the desired operating temperature range of your system. For building applications, that may be between 20 °C and 30 °C. For process or solar thermal storage, higher melting points may be appropriate. The closer the melting point is to your target temperature, the more useful the latent heat will be.
Inputs for mass are in kilograms (kg), temperatures in degrees Celsius (°C), specific heats in kJ/kg·°C, and latent heat in kJ/kg. The outputs are given in kilojoules (kJ) and kilowatt-hours (kWh).
For many conceptual designs, the estimate will be within the right order of magnitude. Real systems often store less usable energy than the ideal value because of heat losses, incomplete phase change, or property variations. Adjusting the efficiency factor downward (for example, 0.6–0.9) can approximate these effects, but detailed design should use more advanced models.
Yes. The underlying energy balance is the same whether you charge the PCM with heat or cold. As long as the material moves through its phase change over your temperature range and the inputs are consistent, the calculated kWh represent the magnitude of energy stored or released.