Page 23 - A Working Method Approach For Introductory Physical Chemistry Calculations
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Introduction to Physical Chemistry                         7
       where p  = pressure of the gas (measured in bar); V = volume of the gas
       (measured  in  dm');  n  =  amount  of  gas  (measured in  mol);  T  =
       temperature of the gas (measured in IS); R = Universal Gas Constant
        = 0.08314 dm3 bar K-' mol-'  (or 8.314 J K-'  mol-I).  The above
       equation can also be modified to take into account changes in tempera-
       ture, AT, changes in volume, AV, and changes in the coefficients of
       gaseous reagents, Au, respectively, i.e. pV  = nRAT, pAV  = nRT and
       pV  = Au,RT. ug represents the coefficients in a chemical equation. For
       example,  in  the  reaction  N2(g)  +  3H2(,    4  2NH3(g),
       Aug = C[v(Gaseous products)]-C[u(Gaseous  reactants)]  = [(2)] - [(l)
        + (3)]  = -2.


                               Molar Volume
       1 mole of an ideal gas measured at 25 "C and 1 bar pressure occupies
       24.8 dm3 (where 1 dm'  = 1000 cm3).

         i.e. 1 mole of an ideal gas at 25 "C and 1 bar pressure occupies 24.8
       1 dm3.


         Example:  Calculate the  amount  of  gas in moles in  2000 cm3 at
         25 "C and 1 bar pressure.


       Solution:
       At 25 "C and 1 bar pressure, 1 mole of an ideal gas occupies 24.8 dm3
                   i.e.  24.8 dm'  =  1 mol
                        1 dm3     =  (1/24.8) mol
       2000cm'     =   2dm3       =  (2/24.8) mol  = 0.081 mol
                             Answer: 0.081 mol.


                       KINETIC THEORY OF GASES
       Kinetic  energy  is  the  energy  a  body  possesses  by  virtue  of  its
       motion.  The  molecules of  gases  travel  at  high  velocity  and  hence
       have  high  kinetic  energy.  The  kinetic  theory  of  gases  is  used  to
       explain the observed properties of gases, of which Brownian motion
       provides  good  evidence.  Brownian  motion  is  the  irregular  zigzag
       movement  of  very  small  particles  suspended in  a  liquid  or gas.  If
        tobacco  smoke  is  placed  in  a  small  cell,  well-illuminated  on  a
        microscope stage, the tiny particles appear to be moving at random,
        as  shown  in  Figure  1.2(c).  This  is  due  to  the  smaller  invisible
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