What Does the Latent Heat of Vaporization Measure?

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The latent heat of vaporization is the amount of heat energy that has to be added to a liquid at the boiling point to vaporize it. The heat is called latent because it does not heat up the liquid. It merely overcomes the intermolecular forces present in the liquid and holding the molecules together, preventing them from escaping as a gas. When enough heat energy is added to the liquid to break the intermolecular forces, the molecules are free to leave the surface of the liquid and become the vapor state of the material being heated.

TL;DR (Too Long; Didn't Read)

The latent heat of vaporization does not heat up the liquid but rather breaks intermolecular bonds to allow the formation of the vapor state of the material. The molecules of liquids are bound by intermolecular forces that prevent them from becoming a gas when the liquid reaches its boiling point. The amount of heat energy that must be added to break these bonds is the latent heat of vaporization.

Intermolecular Bonds in Liquids

The molecules of a liquid can experience four types of intermolecular forces that hold the molecules together and affect the heat of vaporization. These forces that form bonds in liquid molecules are called Van der Waals forces after the Dutch physicist Johannes van der Waals who developed an equation of state for liquids and gases.

Polar molecules have a slightly positive charge on one end of the molecule and a slightly negative charge on the other end. They are called dipoles, and they can form several types of intermolecular bonds. Dipoles that include a hydrogen atom can form hydrogen bonds. Neutral molecules can become temporary dipoles and experience a force called the London dispersion force. Breaking these bonds requires energy corresponding to the heat of vaporization.

Hydrogen Bonds

The hydrogen bond is a dipole-dipole bond that involves a hydrogen atom. Hydrogen atoms form especially strong bonds because the hydrogen atom in a molecule is a proton without an inner shell of electrons, which allows the positively charged proton to approach a negatively charged dipole closely. The electrostatic force of attraction of the proton to the negative dipole is comparatively high, and the resulting bond is the strongest of the four intermolecular bonds of a liquid.

Dipole-Dipole Bonds

When the positively charged end of a polar molecule bonds with the negatively charged end of another molecule, it is a dipole-dipole bond. Liquids made up of dipole molecules continuously form and break dipole-dipole bonds with multiple molecules. These bonds are the second strongest of the four types.

Dipole-Induced Dipole Bonds

When a dipole molecule approaches a neutral molecule, the neutral molecule becomes slightly charged at the point closest to the dipole molecule. Positive dipoles induce a negative charge in the neutral molecule while negative dipoles induce a positive charge. The resulting opposite charges attract, and the weak bond that is created is called a dipole-induced dipole bond.

London Dispersion Forces

When two neutral molecules become temporary dipoles because their electrons have by chance collected on one side, the two molecules may form a weak temporary electrostatic bond with the positive side of one molecule attracted to the negative side of another molecule. These forces are called London dispersion forces, and they form the weakest of the four types of intermolecular bonds of a liquid.

Bonds and Heat of Vaporization

When a liquid has many strong bonds, the molecules tend to stay together, and the latent heat of vaporization is elevated. Water, for example, has dipole molecules with the oxygen atom negatively charged and the hydrogen atoms positively charged. The molecules form strong hydrogen bonds, and water has a correspondingly high latent heat of vaporization. When no strong bonds are present, heating a liquid can easily free the molecules to form a gas, and the latent heat of vaporization is low.

References

About the Author

Bert Markgraf is a freelance writer with a strong science and engineering background. He has written for scientific publications such as the HVDC Newsletter and the Energy and Automation Journal. Online he has written extensively on science-related topics in math, physics, chemistry and biology and has been published on sites such as Digital Landing and Reference.com He holds a Bachelor of Science degree from McGill University.

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