Enthalpy of vaporization

  • temperature-dependency of the heats of vaporization for water, methanol, benzene, and acetone.

    the enthalpy of vaporization, (symbol hvap) also known as the (latent) heat of vaporization or heat of evaporation, is the amount of energy (enthalpy) that must be added to a liquid substance, to transform a quantity of that substance into a gas. the enthalpy of vaporization is a function of the pressure at which that transformation takes place.

    the enthalpy of vaporization is often quoted for the normal boiling temperature of the substance; although tabulated values are usually corrected to 298 k, that correction is often smaller than the uncertainty in the measured value.

    the heat of vaporization is temperature-dependent, though a constant heat of vaporization can be assumed for small temperature ranges and for reduced temperature . the heat of vaporization diminishes with increasing temperature and it vanishes completely at a certain point called the critical temperature (). above the critical temperature, the liquid and vapor phases are indistinguishable, and the substance is called a supercritical fluid.

  • units
  • enthalpy of condensation
  • thermodynamic background
  • vaporization enthalpy of electrolyte solutions
  • selected values
  • see also
  • references

Temperature-dependency of the heats of vaporization for water, methanol, benzene, and acetone.

The enthalpy of vaporization, (symbol Hvap) also known as the (latent) heat of vaporization or heat of evaporation, is the amount of energy (enthalpy) that must be added to a liquid substance, to transform a quantity of that substance into a gas. The enthalpy of vaporization is a function of the pressure at which that transformation takes place.

The enthalpy of vaporization is often quoted for the normal boiling temperature of the substance; although tabulated values are usually corrected to 298 K, that correction is often smaller than the uncertainty in the measured value.

The heat of vaporization is temperature-dependent, though a constant heat of vaporization can be assumed for small temperature ranges and for reduced temperature . The heat of vaporization diminishes with increasing temperature and it vanishes completely at a certain point called the critical temperature (). Above the critical temperature, the liquid and vapor phases are indistinguishable, and the substance is called a supercritical fluid.