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IIT-JEE 2011 - Career Point

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KEY CONCEPT<br />

Physical<br />

Chemistry<br />

Fundamentals<br />

GASEOUS STATE<br />

& REAL GASES<br />

Real Gases :<br />

Deviation from Ideal Behaviour :<br />

Real gases do not obey the ideal gas laws exactly<br />

under all conditions of temperature and pressure.<br />

Experiments show that at low pressures and<br />

moderately high temperatures, gases obey the laws of<br />

Boyle, Charles and Avogadro approximately, but as<br />

the pressure is increased or the temperature is<br />

decreased, a marked departure from ideal behaviour<br />

is observed.<br />

Ideal gas<br />

p<br />

V<br />

Plot of p versus V of hydrogen, as<br />

compared to that of an ideal gas<br />

The curve for the real gas has a tendency to coincide<br />

with that of an ideal gas at low pressures when the<br />

volume is large. At higher pressures, however,<br />

deviations are observed.<br />

Compressibility Factor :<br />

The deviations can be displayed more clearly, by<br />

plotting the ratio of the observed molar volume V m to<br />

the ideal molar volume V m,ideal (= RT/p) as a function<br />

of pressure at constant temperature. This ratio is<br />

called the compressibility factor Z and can be<br />

expressed as<br />

Z =<br />

V<br />

V<br />

m<br />

m,ideal<br />

p<br />

= RT<br />

Vm<br />

Plots of Compressibility Factor versus Pressure :<br />

For an ideal gas Z = 1 and is independent of pressure<br />

and temperature. For a real gas, Z = f(T, p), a<br />

function of both temperature and pressure.<br />

A graph between Z and p for some gases at 273.15 K,<br />

the pressure range in this graph is very large. It can<br />

be noted that:<br />

(1) Z is always greater than 1 for H 2 .<br />

(2) For N 2 , Z < 1 in the lower pressure range and is<br />

greater than 1 at higher pressures. It decreases with<br />

increase of pressure in the lower pressure region,<br />

passes through a minimum at some pressure and then<br />

H 2<br />

increases continuously with pressure in the higher<br />

pressure region.<br />

(3) For CO 2 , there is a large dip in the beginning. In<br />

fact, for gases which are easily liquefied, Z dips<br />

sharply below the ideal line in the low pressure<br />

region.<br />

1.0<br />

t = 0ºC<br />

H 2<br />

N 2<br />

CH 4<br />

ideal gas<br />

CO 2<br />

Z<br />

0 100 200 300<br />

p/101.325 bar<br />

Plots of Z versus p of a few gases<br />

This graph gives an impression that the nature of the<br />

deviations depend upon the nature of the gas. In fact,<br />

it is not so. The determining factor is the temperature<br />

relative to the critical temperature of the particular<br />

gas; near the critical temperature, the pV curves are<br />

like those for CO 2 , but when far away, the curves are<br />

like those for H 2 (below fig.)<br />

Z<br />

1.0<br />

T 1 >T 2 >T 3 >T 4<br />

ideal gas<br />

0 200 400 600<br />

p/101.325 kPa<br />

T 4<br />

T 3<br />

T 2<br />

Plots of Z versus p of a single gas<br />

at various temperatures<br />

Provided the pressure is of the order of 1 bar or less,<br />

and the temperature is not too near the point of<br />

liquefaction, the observed deviations from the ideal<br />

gas laws are not more than a few percent. Under<br />

these conditions, therefore, the equation pV = nRT<br />

and related expressions may be used.<br />

Van der Waals Equation of state for a Real gas<br />

Causes of Deviations from Ideal Behaviour :<br />

The ideal gas laws can be derived from the kinetic<br />

theory of gases which is based on the following two<br />

important assumptions:<br />

T 1<br />

XtraEdge for <strong>IIT</strong>-<strong>JEE</strong> 33 MAY 2010

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