ENGINEERING THERMODYNAMICS
-II
           Debre Markos University
            Institute of Technology
School of Mechanical and Industrial Engineering
                                        primed by:
                                        Lijalem A.
2. Gas-steam mixtures and air conditioning
                                                 1
                 process
Objectives
 Differentiate between dry air and atmospheric air.
 Define and calculate the specific and relative humidity of
  atmospheric air.
 Calculate the dew-point temperature of atmospheric air.
 Relate the adiabatic saturation temperature and wet-bulb
  temperatures of atmospheric air.
 Use the psychrometric chart as a tool to determine the
  properties of atmospheric air.
 Apply the principles of the conservation of mass and energy to
  various air-conditioning processes.
                                                               2
 Introduction
• Atmospheric air makes up the environment in almost every type
  of air conditioning system. Hence a thorough understanding of
  the properties of atmospheric air and the ability to analyze
  various processes involving air is fundamental to air conditioning
  design.
• Psychrometry is the study of the properties of mixtures of air and
  water vapor.
• Atmospheric air is a mixture of many gases plus water vapor and
  a number of pollutants (Fig. below). The amount of water vapor
  and pollutants vary from place to place.
• The concentration of water vapor and pollutants decrease with
  altitude, and above an altitude of about 10 km, atmospheric air
  consists of only dry air. The pollutants have to be filtered out
  before processing the air. Hence, what we process is essentially a
  mixture of various gases that constitute air and water vapor. This
                                                                     3
  mixture is known as moist air.
                       4
Fig. Atmospheric air
 Introduction
• The moist air can be thought of as a mixture of dry air and
  moisture. For all practical purposes, the composition of dry air
  can be considered as constant. The composition of dry air is
  given table below.
• Based on the above composition the molecular weight of dry
  air is found to be 28.966 and the gas constant R is 287.035
  J/kg.K.
                                                                 5
 Introduction
• As mentioned before the air to be processed in air conditioning
  systems is a mixture of dry air and water vapor.
• While the composition of dry air is constant, the amount of
  water vapor present in the air may vary from zero to a
  maximum depending upon the temperature and pressure of the
  mixture (dry air + water vapor).
• At a given temperature and pressure the dry air can only hold a
  certain maximum amount of moisture.
• When the moisture content is maximum, then the air is known
  as saturated air, which is established by a neutral equilibrium
  between the moist air and the liquid or solid phases of water.
• For calculation purposes, the molecular weight of water vapor
  is taken as 18.015 and its gas constant is 461.52 J/kg.K.
                                                                6
DRY AND ATMOSPHERIC AIR
Atmospheric air: Air in the atmosphere containing
some water vapor (or moisture).
Dry air: Air that contains no water vapor.
Water vapor in the air plays a major role in human
comfort. Therefore, it is an important consideration
in air-conditioning applications.
Water vapor in air behaves as if it existed alone      The cp of air can be
and obeys the ideal-gas relation Pv = RT. Then the     assumed to be constant
atmospheric air can be treated as an ideal-gas         at 1.005 kJ/kg·°C in the
mixture:                                               temperature range 10
                                                       to 50°C with an error
                                                       under 0.2%.
 Pa Partial pressure of dry air
 Pv Partial pressure of vapor (vapor pressure)
                                                                              7
   Dry and Atmospheric Air
 The assumption that the water vapor is an ideal gas is valid when the mixture
   temperature is below 50oC.
 This means that the saturation pressure of the water vapor in the air-vapor mixture
   is below 12.3 kPa.
 For these conditions, the enthalpy of the water vapor is approximated by
     hv(T) = hg at mixture temperature T.
The following T-s diagram for water illustrates the ideal-gas behavior at low vapor
pressures.
 The saturated vapor value of the enthalpy
  is a function of temperature and can be
  expressed as
Note: Average Cp value in range of -10 to 50oC is 1.82 KJ/kg-K and The enthalpy of
vapor at 0oc is 2501.3KJ/kg.                                                   8
                Dry and Atmospheric Air
• Note: For the dry air-water vapor mixture, the partial pressure
  of the water vapor in the mixture is less that its saturation
  pressure at the temperature.
                      Pv  Psat @Tmix
• Then the atmospheric air can be treated as an ideal-gas mixture
  whose pressure is the sum of the partial pressure of dry air Pa
  and that of water vapor Pv:
           p = pa + pv
                                                                    9
         Important psychrometric properties:
• Dry bulb temperature (DBT) is the temperature of the moist air as
  measured by a standard thermometer or other temperature measuring
  instruments.
• Saturated vapor pressure (psat) is the saturated partial pressure of
  water vapor at the dry bulb temperature. This is readily available in
  thermodynamic tables and charts.
• ASHRAE suggests the following regression equation for saturated
  vapor pressure of water, which is valid for 0 to 100oC
• where psat = saturated vapor pressure of water in kilopascals
• T = temperature in K
• The regression coefficients c1 to c6 are given by:
• c1 = -5.80022006E+03, c2 = -5.516256E+00, c3 = -4.8640239E-02
• c4 = 4.1764768E-05, c5 = -1.4452093E-08, c6 = 6.5459673E+00
                                                                     10
        Specific and Relative Humidity of Air
 The amount of water vapor in the air can be specified in various
  ways.
 Probably the most logical way is to specify directly the mass of
  water vapor present in a unit mass of dry air.
 This is called absolute or specific humidity (also called humidity
ratio) and is denoted by ω:
           Mass of water vapor in air mv
                                   
                Mass of dry air        ma
          PVM  v / ( Ru T )   Pv M v
          v
                            
          PaVM a / ( Ru T ) Pa M a
               P            Pv
                                            (kg water vapor/kg dry air)
         0.622 v  0.622
               Pa         P  Pv
                                                                    11
        Specific and Relative Humidity of Air
 Consider 1 kg of dry air. By definition, dry air contains no water
  vapor, and thus its specific humidity is zero.
 Now let us add some water vapor to this dry air. The specific
  humidity will increase. As more vapor or moisture is added, the
  specific humidity will keep increasing until the air can hold no
  more moisture.
 At this point, the air is said to be saturated with moisture,
  and it is called saturated air.
 Any moisture introduced into saturated air will condense.
 The amount of water vapor in saturated air at a specified
  temperature and pressure can be determined from above equation
  by replacing Pv by Pg, the saturation pressure of water at that
  temperature
                                                                  12
        Specific and Relative Humidity of Air
 The amount of moisture in the air has a definite effect on how
  comfortable we feel in an environment.
 However, the comfort level depends more on the amount of moisture
  the air holds (mv) relative to the maximum amount of moisture the
  air can hold at the same temperature (mg).
The ratio of these two quantities is called the relative humidity (ϕ)
                      Mass of vapor in air     mv
                                           
                     Mass of in saturated air mg
                      Pv
                    
                      Pg         where: pg   =   psat @T
                                       Pv 1491
                                           .   kPa
          Pg  Pv ,   1 or 100%,               0.47       13
                                       Pg 3169
                                           .   kPa
 Using the definition of the specific humidity, the relative humidity may be expressed
 as
                          P                 0.622Pg
                                   and  
                     (0.622   ) Pg          P  Pg
Volume of mixture per mass of dry air, v
                                     V    mm RmTm / Pm
                                  v    
                                     ma       ma
 After several steps, we can show (you should try this)
                                           V        RT
                                      v       va  a m
                                           ma        Pa                           14
               Specific and Relative Humidity of Air
 So the volume of the mixture per unit mass of dry air is the specific volume of
 the dry air calculated at the mixture temperature and the partial pressure of
 the dry air.
                                             mv
 Mass of mixture:       m  ma  mv  ma (1  )  ma (1   )
                                             ma
Mass flow rate of dry air (m’a):
   Based on the volume flow rate of mixture at a given state, the
   mass flow rate of dry air is
                                   V3
                                                  m /s     kga
                            m a                 3
                                                         
                                    v            m / kga    s
  Enthalpy of mixture per mass dry air, h
                                        Hm Ha  Hv ma ha  mv hv
                                   h            
                                        ma   ma         ma
                                     ha  hv                             15
                  Dew-Point Temperature
 Dry Bulb Temperature Tdb: the temperature measured by a thermometer
   placed in a mixture of air and water-vapor.
 Dew Point Temperature Tdp:
• Dew on the grass in morning !!! Water vapors on your car windscreen!!!
• is the temperature at which condensation begins when the air is cooled at
   constant pressure.
• Tdp is the saturation temperature of water corresponding to the vapor
   pressure:
         Tdp = Tsat@Pv
                                                                              16
EXAMPLE 2.1:
A 5m X 5m X 3m room shown in Fig. below contains air at 25°C and 100kPa
    at a relative humidity of 75 percent. Determine
(a) the partial pressure of dry air,
 (b) the specific humidity,
 (c) the enthalpy per unit mass of the dry air, and
 (d ) the masses of the dry air and water vapor in the room.
Assignment: 1
 Atmospheric air is at 25oC, 0.1MPa, 50 percent relative humidity. If the
    mixture is cooled at constant pressure to 10oC, find ,
a) dew point temperature,
b) humidity ratio,
c) Enthalpy of the mixture per mass of dry air, and
 d) the amount of water removed per mass of dry air.
                                                                       17
  The Adiabatic Saturation Process and Wet-Bulb Temperatures
 Air having a relative humidity less than 100 percent flows over water contained in
a well-insulated duct.
Since the air has ϕ < 100 percent, some of the water will evaporate and the
temperature of the air-vapor mixture will decrease.
                                                                               18
If the mixture leaving the duct is saturated and if the process is
adiabatic, the temperature of the mixture on leaving the device is
known as the adiabatic saturation temperature.
For this to be a steady-flow process, makeup water at the adiabatic
saturation temperature is added at the same rate at which water is
evaporated.
We assume that the total pressure is constant during the process.
Apply the conservation of energy to the steady-flow control volume
                                          2                                2
                                         V                                 V
                    Q net   m i (h       gz) i  Wnet   m e (h       gz) e
                             inlets       2                    exits        2
Neglecting the kinetic and potential energies and noting that the heat transfer and work are
zero, we get
                       m a1ha1  m v1hv1  m l 2 hl 2  m a 2 ha 2  m v 2 hv 2
Conservation of mass for the steady-flow control volume is
                                            m   m
                                          inlets
                                                   i
                                                       exits
                                                               e
                                                                                          19
  For the dry air:                m a1  m a 2  m a
 For the water vapor:
                                    m v1  m l 2  m v 2
The mass flow rate water that must be supplied to maintain steady-flow is,
                                  l2  m
                                 m       v2  m v1
                                      m a ( 2   1 )
 Divide the conservation of energy equation by m a , then
                     ha1   1hv1  ( 2   1 )hl 2  ha 2   2 hv 2
  What are the known's and unknowns in this equation?
                                                                             20
Solving for 1               ha 2  ha1   2 (hv 2  hl 2 )
                        1 
                                     (hv1  hl 2 )
                                C pa (T2  T1 )   2 h fg 2
                            
                                       (hg1  h f 2 )
                                                 Pv1
Since 1 is also defined by        1  0.622
                                              P1  Pv1
                                               1 P1
We can solve for Pv1.            Pv1 
                                          0.622   1
                                                 Pv1
 Then, the relative humidity at state 1 is  1 
                                                 Pg1
                                                               21
Wet-Bulb and Dry-Bulb Temperatures
Any temperature you measure with thermometer is dry bulb temperature.
The wet-bulb temperature is the temperature a parcel of air would have if
it were cooled to saturation by the evaporation of water into it, with the latent
heat being supplied by the parcel.
These temperatures are measured by using a device called a
psychrometer.      The psychrometer is composed of two thermometers
mounted on a sling. One thermometer is fitted with a wet gauze and reads
the wet-bulb temperature. The other thermometer reads the dry-bulb, or
ordinary, temperature. As the psychrometer is slung through the air, water
vaporizes from the wet gauze, resulting in a lower temperature to be
registered by the thermometer.
 The wet-bulb temperature is approximately equal to the adiabatic
saturation temperature.
                                                                            22
Example 2.2
  For the adiabatic saturation process shown below, determine the relative
  humidity, humidity ratio (specific humidity), and enthalpy of the
  atmospheric air per mass of dry air at state 1.
Assignment:2 Given the inlet and exit conditions to an air conditioner shown below. What
is the heat transfer to be removed per kg dry air flowing through the device? If the volume
flow rate of the inlet atmospheric air is 17 m3/min, determine the required rate of heat
transfer.                                        Cooling fluid
                                                In      Out       Insulated flow duct
                               Atmospheric
                               air
                              T1 = 30oC                                     T2 = 20oC
                              P1 =100 kPa            Condensate             P2 = 98 kPa
                              ϕ 1 = 80%              at 20oC                ϕ2 = 95%      23
                              v 1=   17m3/min
                         The Psychrometric Chart
The state of the atmospheric air at a specified pressure is completely specified by
two independent intensive properties.
Psychrometric charts present the moist air properties; they are used extensively in
air-conditioning applications.
For a given, fixed, total air-vapor pressure, the properties of the mixture are given
in graphical form on a psychrometric chart.
                                                                                  24
Basic features of psychrometric chart are:
 The dry bulb temperatures are shown on the horizontal axis.
 The specific humidity ω is shown on the vertical axis.
 The curved line at the left end of the chart is the saturation line. All the saturated air
  states are located on this curve. Thus, it also represents the curve of relative
  humidity 100%. Other constant relative humidity curves have the same general
  shape.
 Lines of constant wet-bulb temperature have a downhill appearance to the right.
 Lines of specific volume also have downhill appearance to the right with steeper
  slopes.
 Lines of constant enthalpy lie very near to the constant wet-bulb temperature, thus
  (in some charts) lines of constant wet-bulbs are used as constant-enthalpies.
 For saturated air, the dry-bulb, wet-bulb, and dew-point temperatures are identical.
 Thus the dew-point temperature of atmospheric air can be determined by drawing a
   horizontal line to the saturated curve   .
                                                                                      25
                                                                                                                             26
Reprinted by permission of the Society of Heating and Air-Conditioning Engineers, Inc., Atlanta, Ga; used with permission.
Example 2.3
Consider air at 1 atm, 35°C and 40% relative humidity. Using
  psychrometric chart, determine a) the specific humidity, b) the
  enthalpy, c) the wet-bulb temperature, d) the dew-point
  temperature and e) the specific volume of the air.
Assignment :3
The air in a room has a pressure of 1atm, a dry-bulb temperature
  of 24°C, and a wet-bulb temperature of 17°C. Using the
  psychrometric chart, determine (a) the specific humidity, (b)
  the enthalpy (in kJ/kg dry air), (c) the relative humidity, (d )
  the dew-point temperature, and (e) the specific volume of the
  air (in m3/kg dry air).
                                                                27
             Human Comfort and Air-Conditioning
 Depending on the type of activity, part of the rejected body heat is
  dissipated through latent heat (sweating and breathing).
 The comfort of human body depends on three factors:
 Temperature: most important index of comfort, most people feel
  comfortable when temperature is between 22 and 27°C.
 Relative humidity: it affects the amount of heat that body can
  dissipate through evaporation. Relative humidity is a measure of
  air’s ability to absorb moisture. Most people prefer relative
  humidity of 40 to 60%.
 Air motion: it removes the warm, moist air that builds up around
  body and replaces it with fresh air. Most people feel comfortable
  at an airspeed of 15 m/min (0.25m/s).
                                                                 28
          Air-Conditioning processes
HVAC Processes:
Maintaining a living space or an industrial facility at the desired
temperature and humidity requires some processes called air
   conditioning; including:
a) Simple heating: raising the air temperature.
b) Simple cooling: lowering the air temperature.
c) Humidifying: adding moisture.
d) Dehumidifying: removing moisture.
In many applications, a combination of these processes is needed to
  bring the air to a desired condition.
                                                              29
    Air-Conditioning processes
The air-conditioning processes:
                                  30
           Air-Conditioning processes
1) Simple Heating and Cooling (ω = Constant)
The amount of moisture in the air remains constant during this process
   since no moisture is added or removed to or from the air.
Notice:
 the relative humidity of air decreases during a heating process and
   increases in a cooling process.
 This is because the relative humidity is the ratio of the moisture
   capacity of the air and it increases with increasing the air
   temperature.
                                                                   31
               Air-Conditioning processes
The conservation of mass reduces to:
                  ma1 = ma2 = ma
                     ω1 = ω2
Neglecting any fan work, the conservation of energy yields:
    Q’ = m’ (h2 – h1) or q = (h2 – h1)
Where: h1 and h2 are enthalpies per unit mass of dry air at the inlet and exit
  of the heating/cooling section, respectively.
                                                                          32
         Air-Conditioning processes
2. Heating with Humidification
• To maintain comfortable relative humidity, simple heating is
  typically accompanied with humidification, Fig. below. That is
  accomplished by passing the air through a humidifying section.
• If steam is used in the humidifier, we will have additional heating;
  thus T3 > T2.
• If water is sprayed in the humidifier section, part of the latent heat
  of vaporization comes from the air which results in the cooling of
  the air; thus T3 < T2.
                                                                  33
Fig.: Heating with humidification, using water spray or steam.
                                                                 34
                   Air-Conditioning processes
3. Cooling with Dehumidification
 To remove some moisture from the air, it should be cooled below its dew-point
  temperature.
 Passing through cooling coil, air temperature decreases and its relative humidity
  increases at constant specific humidity until air temperature reaches its dew point
  temperature.
 Any further cooling results in condensation of part of the moisture in the air.
 Note that air remains saturated during the entire condensation process.
                                                                                  35
           Air-Conditioning processes
4. Evaporative Cooling
 Evaporative cooling is based on a simple principle: as water evaporates, the
   latent heat of vaporization is absorbed from the water body and the surrounding
   air.
 As a result, both water and air are cooled.
 The evaporative cooling is essentially identical to the adiabatic saturation
   process. Thus the evaporative cooling process follows a line of constant wet-
   bulb temperature on the psychrometric chart.
                                                                             36
           Air-Conditioning processes
5. Adiabatic Mixing of Air streams
 Mixing processes normally involve no work interactions.
 Then the mass and energy balances for the adiabatic mixing of two
  airstreams reduce to:
                                                                 37
Fig: Adiabatic mixing of two streams
                                       38
Example 2.4
An air-conditioning system is to take in outdoor air at 10°C and 30
  percent relative humidity at a steady rate of 45 m3/min and to
  condition it to 25°C and 60 percent relative humidity. The outdoor
  air is first heated to 22°C in the heating section and then humidified
  by the injection of hot steam in the humidifying section. Assuming
  the entire process takes place at a pressure of 100 kPa, determine
  (a) the rate of heat supply in the heating section and (b) the mass
  flow rate of the steam required in the humidifying section.
Example 2.5
Saturated air at 14°C at a rate of 50 m3/min is mixed adiabatically with
  the outside air at 32°C and 60% relative humidity at a rate of 20
  m3/min. Assuming that the mixing occurs at 1atm, determine: a) The
  specific humidity, b) The relative humidity, c) The dry-bulb, and d)
  The wet-bulb of the mixture.
                                                                   39
Assignment:4
For the air-conditioning system shown below in which atmospheric air is first
   heated and then humidified with a steam spray, determine the required heat
   transfer rate in the heating section and the required steam temperature in the
   humidification section when the steam pressure is 1MPa.
                                                                            40
41