Published by Patrick Mutisya · 14 days ago
Describe the pressure and the changes in pressure of a gas in terms of the forces exerted by particles colliding with surfaces, creating a force per unit area.
The particle model assumes that all matter is made up of tiny particles (atoms or molecules) that are in constant motion. In a gas the particles:
When a gas particle strikes a surface it exerts a force on that surface. The cumulative effect of many such collisions over an area \$A\$ gives the pressure \$P\$:
\$P = \frac{F}{A}\$
where \$F\$ is the total force exerted by the particles on the surface and \$A\$ is the area of that surface.
Each collision changes the particle’s momentum. By Newton’s second law, a change in momentum over a time interval \$\Delta t\$ produces a force:
\$F = \frac{\Delta p}{\Delta t}\$
Summing the forces from all particles that strike the surface each second gives the total force, and dividing by the area yields the pressure.
The pressure of a gas changes when any of the following variables are altered:
| Relationship | Mathematical form | What changes? |
|---|---|---|
| Pressure–Force–Area | \$P = \dfrac{F}{A}\$ | Increase \$F\$ or decrease \$A\$ → pressure rises. |
| Boyle’s Law (constant \$T\$, \$n\$) | \$P1V1 = P2V2\$ | Decrease \$V\$ → pressure increases proportionally. |
| Charles’s Law (constant \$P\$, \$n\$) | \$\displaystyle \frac{V1}{T1} = \frac{V2}{T2}\$ | Increase \$T\$ → volume expands if pressure is fixed. |
| Gay‑Lussac’s Law (constant \$V\$, \$n\$) | \$\displaystyle \frac{P1}{T1} = \frac{P2}{T2}\$ | Increase \$T\$ → pressure rises proportionally. |
| Ideal Gas Equation | \$pV = nRT\$ | Shows combined effect of \$p\$, \$V\$, \$n\$, and \$T\$. |
Consider a sealed container:
Pressure is the result of countless microscopic collisions of gas particles with a surface. It can be expressed as a force per unit area, \$P = F/A\$. Changes in temperature, volume, or amount of gas alter the speed, frequency, or number of these collisions, leading to predictable changes in pressure as described by Boyle’s, Charles’s, Gay‑Lussac’s, and the ideal‑gas equations.