Phase Diagrams of Water and Carbon Dioxide

Interactive pressure-temperature phase diagrams for water and carbon dioxide. Click or tap anywhere to identify the phase at that temperature and pressure; points on a curve read as the two-phase equilibrium, and the triple and critical points announce themselves. Vapor curves are Clausius-Clapeyron fits through measured reference points; fusion lines are anchored linear fits.

Water (H₂O)

Pressure-temperature phase diagram of Water (H₂O). Click or use arrow keys to identify the phase at any temperature and pressure. The numeric anchor data appears in the table below. 010020030040010⁻¹10⁰10¹10²10³10⁴Temperature (°C)Pressure (kPa, log scale)SolidLiquidGasSupercritical fluidTriple ptCritical pt

Carbon dioxide (CO₂)

Pressure-temperature phase diagram of Carbon dioxide (CO₂). Click or use arrow keys to identify the phase at any temperature and pressure. The numeric anchor data appears in the table below. −100−5005010¹10²10³10⁴Temperature (°C)Pressure (kPa, log scale)SolidLiquidGasSupercritical fluidTriple ptCritical pt
Sublimation (solid ⇌ gas) Fusion (solid ⇌ liquid) Vaporization (liquid ⇌ gas)Click or tap anywhere on a diagram to identify the phase at that temperature and pressure; drag to explore, or focus a diagram and use the arrow keys (Shift for larger steps).

Triple Points, Critical Points, and Behavior at 1 atm

Click the interactive diagram to identify the phase; the table lists the key points for water and CO₂.

Triple Points, Critical Points, and Behavior at 1 atm
Water (H⁠2O)0.01 °C, 0.61 kPa374 °C, 22060 kPaMelts at 0 °C, boils at 100 °CNegative (ice is less dense than liquid water)
Carbon dioxide (CO⁠2)−56.6 °C, 518 kPa31 °C, 7370 kPaSublimes at −78.5 °C (no liquid at 1 atm)Positive (solid denser than liquid, the usual case)

Important Notes

  • Reading the diagram: each curve is a two-phase equilibrium; crossing a curve is a phase transition. The three curves meet at the TRIPLE POINT (all three phases coexist); the liquid-gas curve ENDS at the CRITICAL POINT, beyond which liquid and gas merge into a supercritical fluid.
  • Dry ice sublimes at 1 atm because CO₂'s triple-point pressure (518 kPa, about 5.1 atm) sits ABOVE atmospheric pressure: at 1 atm there is no temperature at which liquid CO₂ exists. Liquid CO₂ appears only above 518 kPa.
  • Water's fusion line leans slightly LEFT (negative slope): higher pressure melts ice, because ice is less dense than liquid water. CO₂'s fusion line leans right, the usual case.
  • The pressure axis is logarithmic; it spans from below 1 kPa to beyond the critical pressures.
  • Water's vaporization curve below 100 °C follows the tabulated vapor pressures of water (see the Water Vapor Pressure reference); the 100 °C to critical stretch, both sublimation curves, and CO₂'s vaporization curve are Clausius-Clapeyron fits through the reference points. The fusion lines are linear fits through the 1 atm transition points, with CO₂'s melting slope anchored to the NIST melting curve.
Source:
  • Triple- and critical-point data and enthalpies of transition (ΔHvap = 40.7 kJ/mol, ΔHfus = 6.02 kJ/mol) from standard thermochemical tables; water vapor pressures below 100 °C from the Water Vapor Pressure reference. Vaporization and sublimation curves are Clausius-Clapeyron fits through these points; fusion lines are linear fits through the 1 atm transition points, with the CO₂ melting slope anchored to the NIST melting curve (NIST IR 8608).