A gas consists of particles that would move freely in an ideal gas, but which in a real gas are subject to small intermolecular forces known as van der Waal's forces. Gas particles move randomly at a wide range of speeds of the order of several hundred meters per second.
Kinetic theoryThe molecules of a gas are usually a large distance apart compared with their diameter and there is no regularity in their arrangement in space. Given the positions of two or three molecules, it is not possible to predict where a further one will be with any precision – the molecules are distributed at random throughout the whole volume. Gas molecules move randomly with a mean velocity comparable with that of sound, of the order of 10 m/s. Occasionally two or three of them may be found very close to one another so that their electron clouds overlap and they bind together. Such clusters are common at high pressures but they are usually short-lived.
At 0°C and a pressure of 760mm of mercury, known as standard temperature and pressure (STP), a liter of oxygen is known to contain and 3 × 1022 (30,000 million trillion) molecules. They move with a speed of about 430 m/s (1,410 ft/s). Each oxygen molecule is 3.35 × 10-10m. The molecules are on average 70 × 10-10m apart and they travel about 905 × 10-10m between collisions; this distance is called the mean free path.
The low density of a gas can be readily understood in terms of the comparatively small number of molecules per unit volume, and the high compressibility follows from the fact that the average distance between molecules can be altered over wide limits. The lack of rigidity can be explained by the molecules being able to take up any configuration with equal ease. Further, the molecules can move long distances without encountering one another, so that there is little resistance to motion of any kind, which is the basis of the explanation of the low viscosity.
Ideal gas equationFor a given temperature and pressure, equal volumes of gas contain the same number of molecules (2.7 × 1025 m-3 at room temperature and atmospheric pressure). The impacts of the molecules on the walls of the container are responsible for the pressure exerted by gases, which is much larger than is often appreciated: the atmosphere exerts on everything a pressure many times larger than a person's weight and without it we would simply boil and burst.
For a given mass of ideal gas, the product of the pressure (P) and the volume (V) is proportional to the absolute temperature (T):
PV = RT (the general gas law).The constant of proportionality (R) is known as the universal gas constant and has the value 8.314 J/K-mole. The general gas law and most of the other properties of gases can be explained in terms of the kinetic theory without reference to the internal structure of the molecules.
Boyle's law, Avagadro's principle and other outcomes of kinetic theoryAs temperature rises the kinetic energy of the molecules (their energy of motion) increases by an amount that is proportional to the change in absolute temperature. In a mixture of gases the average kinetic energy becomes the same for each kind of molecule. When a gas is compressed, the volume is inversely proportional to the pressure. This relationship is known as Boyle's law, after its discoverer Robert Boyle. It exists because, when the volume is reduced, collisions with the container walls become more frequent and the pressure rises. If the temperature of a gas rises but it is not allowed to expand (its volume is held constant), the pressure again increases because molecular collisions with the walls become more forceful as well as more frequent.
Another basic gas law is called Avagadro's law (see Avagadro). It states that, at the same temperature and pressure, equal volumes of all gases contain the same number of molecules. A liter of a dense gas such as carbon dioxide contains the same number of molecules as a liter of a light gas such as hydrogen.
Gases slowly diffuse through the walls of a porous vessel because their molecules are smaller than the minute holes in the walls of the container. The rate at which they do so is inversely proportional to the square root of their density. Discovered by the British physicist Thomas Graham it is called Graham's law of diffusion. It is explained by the kinetic theory: if different gas molecules have the same average kinetic energy, the lighter ones must move more quickly. Thus light gases diffuse through pores more quickly than dense ones. More direct evidence for the kinetic theory is provided by the phenomenon of Brownian motion.
Adiabatic expansion and coolingWhen a gas expands it has to do work against the external pressure. As a result it becomes cooler because the necessary energy must come from the kinetic energy of the gas. This phenomenon accounts for the coldness of the air escaping from a car tire, for example. When such a change in pressure or volume occurs without heat entering or leaving the gas it is called adiabatic change. The pressure changes in air as a sound wave passes are adiabatic.
The amount of heat needed to raise the temperature of unit mass of a substance through 1°C is called its specific heat capacity. A gas has two principal ones: that measured at constant pressure (cp), and one at constant volume (cv).
Subjected to sufficient pressure most gases turn into a liquid. But above a certain critical temperature it is impossible to liquefy a gas using pressure alone. This is because, above this temperature, the kinetic energy of the molecules is sufficient to overcome the intermolecular attractions of their neighbors. Scientists therefore apply the cooling effects of adiabatic expansion in order to liquefy gases.
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