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13.6: Humidity, Evaporation, and Boiling

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    1584
  • [ "article:topic", "authorname:openstax", "dew point", "saturation", "percent relative humidity", "relative humidity" ]

    The expression “it’s not the heat, it’s the humidity” makes a valid point. We keep cool in hot weather by evaporating sweat from our skin and water from our breathing passages. Because evaporation is inhibited by high humidity, we feel hotter at a given temperature when the humidity is high. Low humidity, on the other hand, can cause discomfort from excessive drying of mucous membranes and can lead to an increased risk of respiratory infections.

    Figure \(\PageIndex{1}\):Figure_14_06_00.jpg

    Figure \(\PageIndex{1}\): Dew drops like these, on a banana leaf photographed just after sunrise, form when the air temperature drops to or below the dew point. At the dew point, the rate at which water molecules join together is greater than the rate at which they separate, and some of the water condenses to form droplets. (credit: Aaron Escobar, Flickr)

    When we say humidity, we really mean relative humidity. Relative humidity tells us how much water vapor is in the air compared with the maximum possible. At its maximum, denoted as saturation, the relative humidity is 100%, and evaporation is inhibited. The amount of water vapor in the air depends on temperature. For example, relative humidity rises in the evening, as air temperature declines, sometimes reaching the dew point. At the dew point temperature, relative humidity is 100%, and fog may result from the condensation of water droplets if they are small enough to stay in suspension. Conversely, if you wish to dry something (perhaps your hair), it is more effective to blow hot air over it rather than cold air, because, among other things, the increase in temperature increases the energy of the molecules, so the rate of evaporation increases.

    The amount of water vapor in the air depends on the vapor pressure of water. The liquid and solid phases are continuously giving off vapor because some of the molecules have high enough speeds to enter the gas phase; see Figure(a). If a lid is placed over the container, as in Figure(b), evaporation continues, increasing the pressure, until sufficient vapor has built up for condensation to balance evaporation. Then equilibrium has been achieved, and the vapor pressure is equal to the partial pressure of water in the container. Vapor pressure increases with temperature because molecular speeds are higher as temperature increases. Table gives representative values of water vapor pressure over a range of temperatures.

    Two containers, each filled two-thirds with water. One is open to the atmosphere and the other is sealed at the top. The water molecules are depicted as circles with vector arrows of different lengths and directions to indicate velocity. In the sealed container the density of molecules in the air above the water is greater than in the unsealed container. In the sealed container, water is condensing along the walls and top of the upper part of the container.

    Figure \(\PageIndex{2}\): (a) Because of the distribution of speeds and kinetic energies, some water molecules can break away to the vapor phase even at temperatures below the ordinary boiling point. (b) If the container is sealed, evaporation will continue until there is enough vapor density for the condensation rate to equal the evaporation rate. This vapor density and the partial pressure it creates are the saturation values. They increase with temperature and are independent of the presence of other gases, such as air. They depend only on the vapor pressure of water.

    Relative humidity is related to the partial pressure of water vapor in the air. At 100% humidity, the partial pressure is equal to the vapor pressure, and no more water can enter the vapor phase. If the partial pressure is less than the vapor pressure, then evaporation will take place, as humidity is less than 100%. If the partial pressure is greater than the vapor pressure, condensation takes place. In everyday language, people sometimes refer to the capacity of air to “hold” water vapor, but this is not actually what happens. The water vapor is not held by the air. The amount of water in air is determined by the vapor pressure of water and has nothing to do with the properties of air.

    Temperature \(^oC\) Vapor Pressure \((Pa)\) Saturation vapor density \(g/m^3\)
    −50 4.0 0.039
    -20 \(1.04 \times 10^2\) 0.89
    -10 \(2.60 \times 10^2\) 2.36
    0 \(6.10 \times 10^2\) 4.84
    5 \(8.68 \times 10^2\) 6.80
    10 \(1.19 \times 10^3\) 9.40
    15 \(1.69 \times 10^3\) 12.8
    20 \(2.33 \times 10^3\) 17.2
    25 \(3.17 \times 10^3\) 23.0
    30 \(4.24 \times 10^3\) 30.4
    37 \(6.31 \times 10^3\) 44.0
    40 \(7.34 \times 10^3\) 51.1
    50 \(1.23 \times 10^4\) 82.4
    60 \(1.99 \times 10^4\) 130
    70 \(3.12 \times 10^4\) 197
    80 \(4.73 \times 10^4\) 294
    90 \(7.01 \times 10^4\) 418
    95 \(8.59 \times 10^4\) 505
    100 \(1.01 \times 10^5\) 598
    120 \(1.99 \times 10^5\) 1095
    150 \(4.76 \times 10^5\) 2430
    200 \(1.55 \times 10^6\) 7090
    220 \(2.32 \times 10^6\) 10,200

    Saturation Vapor Density of Water

    Example \(\PageIndex{1}\): Calculating Density Using Vapor Pressure

    Table gives the vapor pressure of water at .\(20.0^oC\) as \(2.33 \times 10^3 \space Pa\). Use the ideal gas law to calculate the density of water vapor in \(g/m^3\) that would create a partial pressure equal to this vapor pressure. Compare the result with the saturation vapor density given in the table.

    Strategy

    To solve this problem, we need to break it down into a two steps. The partial pressure follows the ideal gas law,

    \[PV = nRT,\]

    where \(n\) is the number of moles. If we solve this equation for \(n/V\)

    to calculate the number of moles per cubic meter, we can then convert this quantity to grams per cubic meter as requested. To do this, we need to use the molecular mass of water, which is given in the periodic table.

    Solution

    1. Identify the knowns and convert them to the proper units:

    1. temperature \(T = 20^oC = 203 \space K\)
    2. vapor pressure \(P\) of water at \(20^oC\) is \(2.33 \times 10^3 \space Pa\)
    3. molecular mass of water is \(18.0 \space g/m\)

    2. Solve the ideal gas law for \(n?V\).

    \[\dfrac{n}{V} = \dfrac{P}{RT}\]

    3. Substitute known values into the equation and solve for \(n/V\).

    \[\dfrac{n}{V} = \dfrac{P}{RT} = \dfrac{2.33 \times 10^3 \space Pa}{(8.31 \space J/mol \cdot K)(293 \space K)} = 0.957 \space mol/m^3\]

    4. Convert the density in moles per cubic meter to grams per cubic meter.

    \[\rho = \left(0.957\dfrac{mol}{m^3}\right)\left(\dfrac{18.0 \space g}{mol}\right) = 17.2 \space g/m^3\]

    Discussion

    The density is obtained by assuming a pressure equal to the vapor pressure of water at \(20.0^oC\). The density found is identical to the value in Table, which means that a vapor density of \(17.2 \space g/m^3\) at \(20.9^oC\) creates a partial pressure of \(2.33 \times 10^3 \space Pa\), equal to the vapor pressure of water at that temperature. If the partial pressure is equal to the vapor pressure, then the liquid and vapor phases are in equilibrium, and the relative humidity is 100%. Thus, there can be no more than 17.2 g of water vapor per \(m^3\) at \(20.0^oC\), so that this value is the saturation vapor density at that temperature. This example illustrates how water vapor behaves like an ideal gas: the pressure and density are consistent with the ideal gas law (assuming the density in the table is correct). The saturation vapor densities listed in Table are the maximum amounts of water vapor that air can hold at various temperatures.

    Percent Relative Humidity

    We define percent relative humidity as the ratio of vapor density to saturation vapor density, or

    \[percent \space relative \space humidity = \dfrac{vapor \space density}{saturation \space vapor \space density} \times 100\]

    We can use this and the data in Table to do a variety of interesting calculations, keeping in mind that relative humidity is based on the comparison of the partial pressure of water vapor in air and ice.

    We can use this and the data in Table to do a variety of interesting calculations, keeping in mind that relative humidity is based on the comparison of the partial pressure of water vapor in air and ice.

    Exampl \(\PageIndex{2}\): Calculating Humidity and Dew Point

    (a) Calculate the percent relative humidity on a day when the temperature is \(25.0^oC\) and the air contains 9.40 g of vapor per \(m^3\). (b) At what temperature will this air reach 100% relative humidity (the saturation density)? This temperature is the dew point. (c) What is the humidity when the air temperature is \(25.0^oC\) and the dew point is \(-10.0^oC\)?

    Strategy and Solution

    (a) Percent relative humidity is defined as the ratio of vapor density to saturation vapor density.

    \[percent \space relative \space humidity = \dfrac{vapor \space density}{saturation \space vapor \space density} \times 100\]

    The first is given to be \(9.40 \space g/m^3\), and the second is found in Table to be \(23.0 \space g/m^3\). Thus,

    \[percent \space relative \space humidity = \dfrac{9.40 \space g/m^3}{23.0 \space g/m^3} \times 100 = 40.9 \%\]

    (b) The air contains \(9.40 \space g/m^3\) of water vapor. The relative humidity will be 100% at a temperature where \(9.40 \space g/m^3\) is the saturation density. Inspection of Table reveals this to be the case at \(10.0^oC\),

    where the relative humidity will be 100%. That temperature is called the dew point for air with this concentration of water vapor.

    (c) Here, the dew point temperature is given to be \(10.0^oC\). Using Table, we see that the vapor density is \(2.36 \space g/m^3\), because this value is the saturation vapor density at \(-10.0^oC\). The saturation vapor density at \(25.0^oC\) is seen to be \(23.0 \space g/m^3\). Thus, the relative humidity at \(25.0^oC\) is

    \[percent \space relative \space humidity = \dfrac{2.36 \space g/m^3}{23.0 \space g/m^3} \times 100 = 10.3 \%\]

    Discussion

    The importance of dew point is that air temperature cannot drop below \(10.0^oC\) in part (b), or \(-10.0^oC\) in part (c), without water vapor condensing out of the air. If condensation occurs, considerable transfer of heat occurs (discussed in Heat and Heat Transfer Methods), which prevents the temperature from further dropping. When dew points are below \(0^oC\), freezing temperatures are a greater possibility, which explains why farmers keep track of the dew point. Low humidity in deserts means low dew-point temperatures. Thus condensation is unlikely. If the temperature drops, vapor does not condense in liquid drops. Because no heat is released into the air, the air temperature drops more rapidly compared to air with higher humidity. Likewise, at high temperatures, liquid droplets do not evaporate, so that no heat is removed from the gas to the liquid phase. This explains the large range of temperature in arid regions.

    Why does water boil at \(100^oC\)? You will note from Table that the vapor pressure of water at \(100^oC\) is \(1.01 \times 10^5 \space Pa\), or 1.00 atm. Thus, it can evaporate without limit at this temperature and pressure. But why does it form bubbles when it boils? This is because water ordinarily contains significant amounts of dissolved air and other impurities, which are observed as small bubbles of air in a glass of water. If a bubble starts out at the bottom of the container at \(20^oC\), it contains water vapor (about 2.30%). The pressure inside the bubble is fixed at 1.00 atm (we ignore the slight pressure exerted by the water around it). As the temperature rises, the amount of air in the bubble stays the same, but the water vapor increases; the bubble expands to keep the pressure at 1.00 atm. At \(100^oC\), water vapor enters the bubble continuously since the partial pressure of water is equal to 1.00 atm in equilibrium. It cannot reach this pressure, however, since the bubble also contains air and total pressure is 1.00 atm. The bubble grows in size and thereby increases the buoyant force. The bubble breaks away and rises rapidly to the surface—we call this boiling! (See Figure.)

    A beaker of water being heated over a flame. The beaker is shown at three different times. In the first, at twenty degrees C, a small bubble sits on the bottom of the beaker. In the second step, the water temperature is fifty degrees C and the bubble is larger, though still sitting on the bottom of the beaker. In the third step, the water temperature is one hundred degrees C. The bubble is larger and is rising toward the surface.

    Figure \(\PageIndex{3}\): (a) An air bubble in water starts out saturated with water vapor at \(20^oC\). (b) As the temperature rises, water vapor enters the bubble because its vapor pressure increases. The bubble expands to keep its pressure at 1.00 atm. (c) At \(100^oC\), water vapor enters the bubble continuously because water’s vapor pressure exceeds its partial pressure in the bubble, which must be less than 1.00 atm. The bubble grows and rises to the surface.

    Check Your Understanding

    • Freeze drying is a process in which substances, such as foods, are dried by placing them in a vacuum chamber and lowering the atmospheric pressure around them. How does the lowered atmospheric pressure speed the drying process, and why does it cause the temperature of the food to drop?

    [Hide Solution]

    Decreased the atmospheric pressure results in decreased partial pressure of water, hence a lower humidity. So evaporation of water from food, for example, will be enhanced. The molecules of water most likely to break away from the food will be those with the greatest velocities. Those remaining thus have a lower average velocity and a lower temperature. This can (and does) result in the freezing and drying of the food; hence the process is aptly named freeze drying.

    PHET EXPLORATIONS: STATES OF MATTER

    Watch different types of molecules form a solid, liquid, or gas. Add or remove heat and watch the phase change. Change the temperature or volume of a container and see a pressure-temperature diagram respond in real time. Relate the interaction potential to the forces between molecules.

    Figure \(\PageIndex{4}\): States of Matter: Basics

    Summary

    • Relative humidity is the fraction of water vapor in a gas compared to the saturation value.
    • The saturation vapor density can be determined from the vapor pressure for a given temperature.
    • Percent relative humidity is defined to be \[percent \space relative \space humidity = \dfrac{vapor \space density}{saturation \space vapor \space density} \times 100\%\]
    • The dew point is the temperature at which air reaches 100% relative humidity.

    Glossary

    dew point
    the temperature at which relative humidity is 100%; the temperature at which water starts to condense out of the air
    saturation
    the condition of 100% relative humidity
    percent relative humidity
    the ratio of vapor density to saturation vapor density
    relative humidity
    the amount of water in the air relative to the maximum amount the air can hold

    Contributors

    Paul Peter Urone (Professor Emeritus at California State University, Sacramento) and Roger Hinrichs (State University of New York, College at Oswego) with Contributing Authors: Kim Dirks (University of Auckland) and Manjula Sharma (University of Sydney). This work is licensed by OpenStax University Physics under a Creative Commons Attribution License (by 4.0).