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Direct Energy, 2018a

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178 8.4 Ideal Gas Law<br />

8.4 Ideal Gas Law<br />

In most materials, if we know three of the four thermodynamic properties,<br />

volume, pressure, temperature, and entropy, we can derive the fourth property<br />

as well as other thermodynamic measures. Such materials are called<br />

simple compressible systems [109, 102]. For such materials, the ideal gas<br />

law relates pressure, volume, and temperature.<br />

PV = NRT. (8.14)<br />

While this is not a mathematical law, it is a good description of gases, and<br />

it can be used as a rough approximation for liquids and solids. Consider<br />

a container lled with a gas. If the volume of the container is compressed<br />

while the temperature is kept constant, the pressure increases. If the gas is<br />

heated and the pressure is kept constant, the volume increases. The energy<br />

stored in a gas that undergoes change in volume at constant temperature<br />

is given by<br />

ˆ<br />

E = PdV (8.15)<br />

where the change in energy is specied by<br />

ΔE = PΔV. (8.16)<br />

The ideal gas law can be written incorporating entropy as<br />

PV = ST. (8.17)<br />

For example, consider a 10 L tank that holds 5 mol of argon atoms. The<br />

argon gas is at a temperature of T =15 ◦ C. Find the pressure in the tank<br />

in pascals and in atm. We begin by converting the volume and temperature<br />

to more convenient units, V =0.01 m 3 and T = 288.15 K. Next, the ideal<br />

gas law provides the pressure in Pa.<br />

P = NRT<br />

V = 5 mol · 8.314 J<br />

mol·K · 288.15 K<br />

=1.20 · 10 6 Pa (8.18)<br />

0.01 m 3<br />

Finally, we convert the pressure to the desired units.<br />

P =1.20 · 10 6 Pa ·<br />

1 atm<br />

101325 Pa<br />

=11.8 atm (8.19)<br />

As another example, consider a container that holds neon atoms at a<br />

temperature of T =25 ◦ C. Assume that the pressure in the container is 10

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