Page 62 - Air pollution and greenhouse gases from basic concepts to engineering applications for air emission control
P. 62

36                                            2  Basic Properties of Gases

            Table 2.1 Mean free paths
                                  Pressure (atm)  Temperature (K)  Mean free path (m)
            for ideal gases
                                  1             300            7 × 10 −8
                                  10 −4         300            7 × 10 −4
                                  10 −8         300            7




            Solution

            Gas             Percent by volume (%)  Mole ratio  Partial pressure (Pa)
            Nitrogen        78.084               0.78084     79,118.61
            Oxygen          20.9476              0.209476    21,225.16
            Carbon dioxide   0.0314              0.00314     318.16
            Methane          0.0002              0.000002    0.203

              Sometimes, we need to determine the amount of moisture or water vapor in the
            air. It is useful in air emission monitoring, characterization of the air cleaning
            efficiency, or simply quantification of indoor air quality. It can be expressed by
            either specific humidity or relative humidity of the air. Specific humidity quantifies
            the mass ratio of water molecules to dry air. The specific humidity, w, of air can be
            calculated using

                                         m w   n w M w
                                     w ¼     ¼                           ð2:42Þ
                                         m air  n air M air
              Relative humidity of air is expressed as the ratio of the vapor partial pressure of
            the air to the saturation vapor partial pressure of the air at the actual dry bulb
            temperature.


                                               P w
                                         RH ¼                            ð2:43Þ
                                              P sat
            where P w ¼ vapor partial pressure and P sat ¼ saturation vapor partial pressure at
            the actual dry bulb temperature. They shall carry the same unit to make RH
            dimensionless. Since vapor partial pressure is less than the saturation vapor partial
            pressure, we have 0\RH\1. More practically, relative humidity can also be
            expressed as the ratio of actual mass of water vapor in a given air volume to the
            mass of water vapor required to saturate at this air.

                                              m w
                                         RH ¼                            ð2:44Þ
                                              m w;s
   57   58   59   60   61   62   63   64   65   66   67