Calculus-Based Physics by Jeffrey W. Schnick - HTML preview

PLEASE NOTE: This is an HTML preview only and some elements such as links or page numbers may be incorrect.
Download the book in PDF, Kindle for a complete version.

Chapter 36 Heat: Phase Changes

Q = mL

m

Note the absence of a ∆T in the expression Q = mL

m . There is no ∆T in the expressio n because

there is no temperature change in the process. The whole phase change takes place at one

temperature.

So far, we have talked about the case of a solid sample, at the melting temperature, which is in

contact with a hotter object. Heat flows into the sample, melting it. Now consider a sample of

the same substance in liquid form at the same temperature but in contact with a colder object. In

this case, heat will flow from the sample to the colder object. This heat loss from the sample

does not result in a decrease in the temperature. Rather, it results in a phase change of the

substance of which the sample consists, from liquid to solid. This phase change is called

freezing. It also goes by the name of solidification. The temperature at which freezing takes

place is called the freezing temperature, but it is important to remember that the freezing

temperature has the same value as the melting temperature. The heat-per-mass that must flow

out of the substance to freeze it (assuming the substance to be at the freezing temperature

already) is called the latent heat of fusion, or L f . The latent heat of fusion for a given substance

has the same value as the latent heat of melting for that substance:

L f = L m

The amount of heat that must flow out of a sample of mass m in order to convert the entire

sample from liquid to solid is given by:

Q = mL

f

Again, there is no temperature change.

The other two phase changes we need to consider are vaporization and condensation.

Vaporization is also known as boiling. It is the phase change in which liquid turns into gas. It

too (as in the case of freezing and melting), occurs at a single temperature, but for a given

substance, the boiling temperature is higher than the freezing temperature. The heat-per-mass

that must flow into a liquid to convert it to gas is called the latent heat of vaporization L v . The

heat that must flow into mass m of a liquid that is already at its boiling temperature (a.k.a. its

vaporization temperature) to convert it entirely into gas is given by:

Q = mL

v

Condensation is the phase change in which gas turns into liquid. In order for condensation to

occur, the gas must be at the condensation temperature, the same temperature as the boiling

temperature (a.k.a. the vaporization temperature). Furthermore, heat must flow out of the gas, as

it does when the gas is in contact with a colder object. Condensation takes place at a fixed

temperature known as the condensation temperature. (The melting temperature, the freezing

temperature, the boiling temperature, and the condensation temperature are also referred to as the

melting point, the freezing point, the boiling point, and the condensation point, respectively.)

The heat-per-mass that must be extracted from a particular kind of gas that is already at the

2

63