Understandings |
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Pressure |
Equation of state for an ideal gas |
Kinetic model of an ideal gas |
Mole, molar mass and the Avogadro constant |
Differences between real and ideal gases |
Applications and Skills |
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Solving problems using the equation of state for an ideal gas and gas laws |
Sketching and interpreting changes of state of an ideal gas on pressure–volume, pressure–temperature and volume–temperature diagrams |
Investigating at least one gas law experimentally |
$$ P = \frac{F}{A}\\ n = \frac NN_a\\ PV = nRT\\ \tilde{E_K}= \frac{3}{2}k_BT = \frac{3}{2}\frac{R}{N_A}T $$
Let’s consider a gas molecule confined in a closed box.
The molecule’s direction is always changing and is it is feeling a force from the walls of the box. By Newton’s third law, the molecule is exerting an equal and opposite force on the walls of the box. We say that the walls of the box feel a pressure P.
More specifically, pressure is defined as the normal force applied per unit area
$$ P = \frac FA $$
Example 1
Two hollow cubes of side 25 cm with one face missing are placed together at the missing face, as shown on the right. The air inside the solid formed is pumped out.
Determine the force that is necessary to separate the cubes.
Example 2
By definition, one mole of any substance contains as many particles as there are atoms in $12 g$ of carbon-12.