Boyle's, Charles's, and Gay-Lussac's Laws
~9 min read · Tier toggle changes depth (T1 plain · T2 standard · T3 rigour)
You should be comfortable with the definitions of pressure, volume, and absolute temperature (Kelvin), and understand how to convert between common units such as atmospheres, litres, and Pascals.
Why this matters
These three empirical laws form the foundational building blocks of the ideal gas equation.
Before we can derive the universal gas law, we must understand how gases behave under specific constraints. Boyle, Charles, and Gay-Lussac independently discovered that gas properties are not independent variables but are tightly coupled. By isolating one variable at a time, we can predict how a gas will respond to changes in its environment. This lecture dissects these individual relationships, showing how they emerge from the kinetic molecular theory and how they combine to describe the macroscopic behaviour of gases in chemical and physical processes.
The Kinetic Picture of Gas Behaviour
Imagine a sealed container filled with gas molecules. These molecules are in constant, random motion, colliding with each other and with the walls of the container. The pressure exerted by the gas is simply the result of these collisions transferring momentum to the container walls. To understand the laws of gas behaviour, we must look at what happens when we change the conditions of this system. If we compress the gas by reducing its volume, the molecules have less space to move. Consequently, they collide with the walls more frequently. This increase in collision frequency leads to a higher pressure, assuming the temperature remains constant. This is the intuitive basis of Boyle’s law. Conversely, if we heat the gas, the molecules gain kinetic energy and move faster. Faster molecules collide with the walls more forcefully and more frequently, increasing the pressure. If the container is flexible, such as a balloon, this increased pressure causes the volume to expand until the pressure equalises with the surroundings. This is the essence of Charles’s law. These observations are not just abstract rules; they are direct consequences of the microscopic motion of particles. By understanding this kinetic picture, we can predict gas behaviour without memorising formulas. For instance, a syringe filled with air resists compression because the trapped molecules are being forced into a smaller space, increasing their collision rate with the plunger. Similarly, a balloon expands when placed in a warm room because the heated air molecules move faster and push the balloon walls outward. These everyday phenomena are governed by the same fundamental principles that we will now quantify mathematically.
Boyle’s Law: The Inverse Relationship
Boyle’s law describes the relationship between pressure and volume when the amount of gas and its temperature are held constant. Robert Boyle demonstrated in the 17th century that for a fixed mass of gas at a constant temperature, the volume is inversely proportional to the pressure. Mathematically, this is expressed as \( V \propto \frac{1}{P} \), or equivalently \( PV = \text{constant} \). This means that if you double the pressure, the volume halves, provided the temperature does not change. Consider a piston-cylinder system. If you push the piston down, reducing the volume, the gas molecules are confined to a smaller space. They hit the walls more often, increasing the pressure. If you pull the piston up, increasing the volume, the molecules have more space, they hit the walls less often, and the pressure drops. This inverse relationship is crucial in many applications, from the operation of syringes to the breathing mechanics of the lungs. When you inhale, your diaphragm contracts, increasing the volume of your thoracic cavity. This decrease in pressure relative to the atmosphere draws air into your lungs. When you exhale, the volume decreases, pressure increases, and air is forced out. Understanding Boyle’s law allows us to calculate the final volume or pressure of a gas after a change in conditions, provided we know the initial state and that temperature and amount of gas remain unchanged.
Here, \( P_1 \) and \( V_1 \) are the initial pressure and volume, while \( P_2 \) and \( V_2 \) are the final pressure and volume. This equation is derived directly from the proportionality \( PV = k \). It is important to note that this law assumes ideal gas behaviour, which is a good approximation for most gases at moderate pressures and temperatures. At very high pressures, intermolecular forces become significant, and the gas deviates from this simple inverse relationship.
Charles’s Law: The Direct Relationship
Charles’s law describes the relationship between volume and temperature when the pressure and amount of gas are held constant. Jacques Charles observed that for a fixed mass of gas at constant pressure, the volume is directly proportional to the absolute temperature. This is expressed as \( V \propto T \), or \( \frac{V}{T} = \text{constant} \). It is crucial to use the Kelvin scale for temperature in this law, as the relationship is linear only when zero is defined as absolute zero. With Celsius the relationship is still a straight line, but not a proportionality, because 0 °C is not where the volume would extrapolate to zero. Consider a balloon in a refrigerator. As the temperature drops, the gas molecules lose kinetic energy and move slower. They collide with the balloon walls less forcefully, causing the balloon to shrink. When you take the balloon out and let it warm up, the molecules speed up, collide more forcefully, and the balloon expands. This direct proportionality means that if you double the absolute temperature, the volume also doubles, provided the pressure remains constant. This law is fundamental in understanding the behaviour of gases in various industrial processes, such as the expansion of gases in engines and the operation of hot-air balloons. Hot-air balloons work by heating the air inside the envelope, causing it to expand and become less dense than the surrounding cooler air. This density difference creates buoyancy, allowing the balloon to rise. Charles’s law provides the quantitative basis for calculating the volume changes associated with temperature variations.
In this equation, \( T \) must be in Kelvin. This law highlights the importance of absolute temperature in gas calculations. It also shows that as temperature approaches absolute zero, the volume of an ideal gas would theoretically approach zero, although real gases liquefy or solidify before reaching this point.
Gay-Lussac’s Law: Pressure and Temperature
Gay-Lussac’s law, also known as Amontons’s law, describes the relationship between pressure and temperature when the volume and amount of gas are held constant. Joseph Louis Gay-Lussac found that for a fixed mass of gas at constant volume, the pressure is directly proportional to the absolute temperature. This is expressed as \( P \propto T \), or \( \frac{P}{T} = \text{constant} \). This law is particularly relevant in sealed containers, such as aerosol cans or pressure vessels. If you heat a sealed can of spray paint, the gas cannot expand, so its pressure increases (and the vapour pressure of the liquid propellant rises as well). This can be dangerous if the pressure exceeds the strength of the can, leading to an explosion. Conversely, if you cool a sealed container, the pressure drops. This is why aerosol cans often have a lower pressure when stored in a cold environment. The kinetic explanation is straightforward: as temperature increases, the molecules move faster and collide with the walls more forcefully, increasing the pressure. Since the volume is fixed, the frequency of collisions also increases, further contributing to the pressure rise. Gay-Lussac’s law is essential for understanding the safety limits of pressurised systems and for designing equipment that operates under varying temperature conditions. It also plays a role in the calibration of pressure gauges and in the study of thermodynamic cycles.
Again, temperature must be in Kelvin. This law complements Boyle’s and Charles’s laws by providing the relationship between the two variables that are not held constant in the other two laws. Together with Avogadro's law (\(V \propto n\) at fixed \(P\) and \(T\)), these three laws give a complete description of ideal-gas behaviour. They are not independent; rather, they are different facets of the same underlying physical reality. By combining them, we can derive the ideal gas law, which relates all four variables: pressure, volume, temperature, and amount of gas.
The result
The ideal gas law
Three separately discovered empirical proportionalities — Boyle's law (\(V\propto1/P\) at fixed \(n,T\)), Charles's law (\(V\propto T\) at fixed \(n,P\)), and Avogadro's law (\(V\propto n\) at fixed \(T,P\), gas-stoichiometry-avogadro) — combine into a single joint proportionality \(V\propto nT/P\), which becomes an equation once a proportionality constant \(R\) (the universal gas constant, empirically found to be the same for every gas in the ideal limit) is introduced: \(PV=nRT\).
A common misconception is that these laws apply to real gases under all conditions. In reality, real gases deviate from ideal behaviour at high pressures and low temperatures due to intermolecular forces and the finite size of molecules. For example, at very high pressures, the volume occupied by the molecules themselves becomes significant, and the simple inverse relationship of Boyle’s law breaks down. Similarly, at low temperatures, attractive forces between molecules can cause condensation, violating the assumptions of Charles’s and Gay-Lussac’s laws. Always check the conditions of your problem to ensure that the ideal gas approximation is valid. If the gas is near its condensation point or at extremely high pressures, you may need to use more complex equations of state, such as the van der Waals equation, to accurately describe its behaviour. C
Worked example
Problem. A sample of gas occupies a volume of 2.50 L at a pressure of 1.20 atm and a temperature of 300 K. If the gas is compressed to a volume of 1.00 L and heated to 350 K, what is the final pressure? Assume the amount of gas remains constant.
- Identify the given values: \( V_1 = 2.50\ \mathrm{L} \), \( P_1 = 1.20\ \mathrm{atm} \), \( T_1 = 300\ \mathrm{K} \), \( V_2 = 1.00\ \mathrm{L} \), \( T_2 = 350\ \mathrm{K} \).
- Recognise that this problem involves changes in pressure, volume, and temperature, so we need to combine Boyle’s, Charles’s, and Gay-Lussac’s laws into the combined gas law: \( \frac{P_1 V_1}{T_1} = \frac{P_2 V_2}{T_2} \).
- Rearrange the equation to solve for the unknown final pressure \( P_2 \): \( P_2 = P_1 \times \frac{V_1}{V_2} \times \frac{T_2}{T_1} \).
- Substitute the known values into the equation: \( P_2 = 1.20\ \mathrm{atm} \times \frac{2.50\ \mathrm{L}}{1.00\ \mathrm{L}} \times \frac{350\ \mathrm{K}}{300\ \mathrm{K}} \).
- Calculate the result: \( P_2 = 1.20 \times 2.50 \times 1.1667 = 3.50\ \mathrm{atm} \).
Units check. The units of volume and temperature cancel out, leaving the pressure in atmospheres, which is consistent with the initial pressure unit.
Three quick tests
- What happens to the volume of a gas if the pressure is doubled while the temperature remains constant?
Answer
The volume is halved, according to Boyle’s law. - Why must temperature be measured in Kelvin when applying Charles’s law?
Answer
Because volume is proportional to temperature only when temperature is measured from absolute zero; with Celsius the relationship is linear but not proportional. - If a sealed container of gas is heated, what happens to the pressure?
Answer
The pressure increases, according to Gay-Lussac’s law, because the molecules move faster and collide more forcefully with the walls.
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Every lecture and every result in this unit, with prerequisites and threads.
Lecture notes checked line by line by the editor; every number in the worked example was recomputed.