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kinetic theory of gas气体动力学理论kinetic theory of gas气体动力学理论
Chapter 16 Kinetic Theory of Gases
16-1 The Ideal Gas Law and the
Molecular Interpretation of Temperature
16-2 Distribution of Molecular Speeds
16-6 Mean Free Path
16-1 The Ideal Gas Law and the
Molecular Interpretation of Temperature
Our first model of a many-particle system: the Ideal Gas
Models of matter: gas models (random motion of particles)
Air at normal conditions:
~ 2.7×1019 molecules in 1 cm3 of air
Size of the molecules ~ (2-3) × 10-10 m,
Distance between the molecules ~ 3 × 10-9 m
The average speed - 500 m/s
The mean free path - 10-7 m (0.1 micron)
The number of collisions in 1 second - 5 × 109
1. The ideal gas model
1) Assumptions about the molecules in an ideal gas
The ideal gas model - works well at low densities (diluted
gases)
• all the molecules are identical, N is huge;
• the molecules are tiny compared to their average separation
(point masses);
• the molecules do not interact with each other;
• the molecules obey Newton’s laws of motion, their motion is
random;
• collisions between the molecules and the container walls are
elastic.
2) Statistical assumptions about an ideal gas
In an equilibrium state, the distribution of molecules on the
position is uniform, which means that the density of number of
molecules is the same everywhere,
dN N
n
d V V
Velocities of molecules are different. Each molecule has
its velocity, which may be changed due to collisions. In an
equilibrium state, velocity of each molecule has the same
probability to point to any directions. That is, the distribution
of velocity of molecules is uniform in direction, which leads to
the mean-square speeds of all components of velocity are same.
Let v2 be the average value of vx2
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