Page 248 - Schaum's Outline of Theory and Problems of Applied Physics
P. 248

CHAPTER 20







                                           Kinetic Theory




                                                               of Matter














        KINETIC THEORYOFGASES

        The kinetic theory of gases holds that a gas is composed of very small particles, called molecules, which are in
        constant random motion. The molecules are far apart relative to their dimensions and do not interact with one
        another except in collisions.
            The pressure a gas exerts is due to the impacts of its molecules; there are so many molecules in even a small
        gas sample that the individual blows appear as a continuous force. Boyle’s law is readily understood in terms
        of the kinetic theory of gases. Expanding a gas sample means that its molecules must travel farther between
        successive impacts on the container walls and that the impacts are spread over a larger area. Hence an increase
        in volume means a decrease in pressure, and vice versa.





        MOLECULAR ENERGY
        According to the kinetic theory of gases, the average kinetic energy of the molecules of a gas is proportional to
        the absolute temperature of the gas. This relationship is usually expressed in the form
                                                      3
                                               KE av = kT
                                                      2
        where k = Boltzmann’s constant = 1.38 × 10 −23  J/K. Actual molecular energies vary considerably on either
        side of KE av .
            At absolute zero, 0 K, gas molecules would be at rest, which is why this is such a significant temperature. At
        any given temperature, all gases have the same average molecular energy. Therefore, in a gas whose molecules
        are heavy, the molecules move more slowly on the average than do those in a gas at the same temperature whose
        molecules are light.
            Charles’s law follows directly from the above interpretation of temperature. Compressing a gas causes its
        temperature to rise because molecules rebound from the inward-moving walls of the container with increased
        energy, just as a tennis ball rebounds with greater energy when it is struck by a moving racket. Similarly,
        expanding a gas causes its temperature to fall because molecules rebound from the outward-moving walls with
        decreased energy.


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