Boyle's law

Squeeze the plunger of a sealed syringe and the trapped air pushes back harder the smaller you make its space. Let the plunger out again and the push weakens. Nothing about the gas itself changes in this process — its temperature and the number of molecules inside stay fixed — yet pressure and volume swing in perfect lockstep, one up whenever the other goes down. Robert Boyle first pinned this behaviour down experimentally in 1662, using a J-shaped glass tube of trapped air and a column of mercury, and it remains the first quantitative gas law every ICSE Class 9 Chemistry student meets. This article rebuilds the law from the molecular picture of a gas, gives its exact mathematical form, works through the pressure-volume arithmetic in full, and flags the mistakes that cost the most marks.

The core insight

At constant temperature, the volume of a fixed mass of gas is inversely proportional to its pressure, so P1V1=P2V2P_1V_1 = P_2V_2 whenever pressure or volume changes and temperature does not.

The core idea

A gas is not a static substance sitting in its container — it is billions of molecules in constant, random motion, darting about and colliding with each other and with the container walls. Every one of those wall collisions delivers a tiny push, and the combined effect of countless pushes per second, spread over the wall's area, is what we measure as pressure. This molecular picture is the reasoning behind everything Boyle's Law predicts. Now compress that same fixed mass of gas into a smaller volume while holding its temperature steady. The molecules still move at the same average speed (temperature has not changed), but they now have less distance to travel before hitting a wall, so they strike more often in a given time. More collisions per second means higher pressure. Squeeze harder, and the pressure rises further; let the gas expand, and the molecules travel farther between collisions, so pressure falls. Boyle's Law states this precisely:

At constant temperature, the volume of a fixed mass of a gas is inversely proportional to its pressure.

V∝1P(fixed mass, constant T)V \propto \frac{1}{P} \quad \text{(fixed mass, constant } T\text{)}

where: VV is the volume occupied by the gas, PP is its pressure, and the proportionality holds only when the mass of gas and its temperature are both held fixed. Because V∝1/PV \propto 1/P, the product PVPV is a constant for that gas at that temperature — so if the state changes from an initial pressure and volume (P1,V1)(P_1, V_1) to a final pair (P2,V2)(P_2, V_2) without any change in temperature or mass:

P1V1=P2V2P_1V_1 = P_2V_2

where: P1,V1P_1, V_1 are the pressure and volume before the change, and P2,V2P_2, V_2 are the pressure and volume after — all four values referring to the same fixed mass of gas at the same fixed temperature.

Reading the graphs. Plotting PP against VV gives a smooth downward curve called a rectangular hyperbola: as VV rises, PP falls, but never in a straight line. Plotting PP against 1/V1/V instead straightens the same relationship into a line through the origin, because PP is directly proportional to 1/V1/V. ICSE questions often ask you to identify which of the two graphs is which, so it is worth being able to sketch both from memory.

Figure
Two graphs side by side showing pressure against volume as a downward curve and pressure against one over volume as a straight line through the origin
P vs V — a curve Volume V Pressure P P vs 1/V — a line 1 / Volume Pressure P

Boyle's law from the molecular picture

The result that lets you calculate unknown pressures and volumes is P1V1=P2V2P_1V_1 = P_2V_2 for a fixed mass of gas held at constant temperature, and it deserves a short reasoned build rather than being taken purely on Boyle's authority, because ICSE examiners routinely ask you to "explain" it rather than merely "state" it.

Step 1. Fix the physical picture. A container holds NN molecules of gas, each colliding with the walls and rebounding; pressure is the total force per unit area these collisions exert. Temperature is a measure of the average kinetic energy of the molecules — if temperature is unchanged, the molecules' average speed is unchanged too.

Step 2. Compress the container from a larger volume V1V_1 to a smaller volume V2V_2, keeping NN and the temperature fixed. The same number of molecules, moving at the same average speed, are now confined to a smaller space, so each molecule covers less distance between one wall collision and the next.

Step 3. Count collisions. Less distance between collisions, at the same speed, means more collisions per second on every unit of wall area. Since pressure is built from the rate and force of these collisions, pressure must rise as volume falls, and it must fall as volume rises — the two quantities move in strictly opposite directions.

Step 4. Turn the qualitative link into a proportion. Boyle's experiments (and the reasoning above) show the relationship is not just "opposite" but precisely inverse: V∝1/PV \propto 1/P, so PVPV stays constant for that fixed mass of gas at that fixed temperature. Writing the constant value at state 1 and state 2 and setting them equal gives P1V1=P2V2P_1V_1 = P_2V_2 — the working form of Boyle's Law used in every numerical problem.

Worked example

A gas occupies 600 cm³ at a pressure of 1 atmosphere. What will be its volume if the pressure is increased to 1.5 atmospheres, temperature remaining constant?

Step 1. List the known values: P1=1 atmP_1 = 1\,\text{atm}, V1=600 cm3V_1 = 600\,\text{cm}^3, P2=1.5 atmP_2 = 1.5\,\text{atm}, and V2V_2 is unknown. Temperature and mass of gas are both constant, so Boyle's Law applies directly.

Step 2. Apply Boyle's Law and substitute. P1V1=P2V2P_1V_1 = P_2V_2 gives 1×600=1.5×V21 \times 600 = 1.5 \times V_2.

Step 3. Solve for V2V_2. V2=6001.5=400 cm3V_2 = \dfrac{600}{1.5} = 400\,\text{cm}^3.

The volume decreases to 400 cm³. This is exactly what the molecular picture predicts: raising the pressure at constant temperature must squeeze the same gas into a smaller space.

Competitive stretch

A gas has a volume of 250 cm³ at STP (1 atmosphere). Find its volume if the pressure is reduced to half of its STP value, temperature kept constant.

Step 1. P1=1 atmP_1 = 1\,\text{atm}, V1=250 cm3V_1 = 250\,\text{cm}^3, P2=0.5 atmP_2 = 0.5\,\text{atm}.

Step 2. P1V1=P2V2⇒1×250=0.5×V2P_1V_1 = P_2V_2 \Rightarrow 1 \times 250 = 0.5 \times V_2.

Step 3. V2=2500.5=500 cm3V_2 = \dfrac{250}{0.5} = 500\,\text{cm}^3. Halving the pressure exactly doubles the volume — a clean check that P1V1=1×250=250P_1V_1 = 1 \times 250 = 250 equals P2V2=0.5×500=250P_2V_2 = 0.5 \times 500 = 250, confirming the product stays constant.

Common traps

  • Forgetting "constant temperature." Boyle's Law only holds if temperature does not change during the process; if it does, the combined gas equation is needed instead.
  • Treating PP and VV as directly proportional. They are inversely proportional — pressure up means volume down, and vice versa, for a fixed mass of gas.
  • Mixing units across the two sides. Both P1P_1 and P2P_2 must share one unit (e.g. both in atm), and both V1V_1 and V2V_2 must share one unit (e.g. both in cm³), or P1V1=P2V2P_1V_1 = P_2V_2 is meaningless.
  • Misreading the graphs. The PP–VV graph is a curve, not a straight line; only PP plotted against 1/V1/V gives a straight line through the origin.

Ask the tutor: Want another Boyle's Law problem with different starting units, or a quick refresher on sketching the P-V and P-1/V graphs? Ask your AI tutor for a guided walkthrough.

Why does the P-V graph curve instead of being a straight line?

Because PP and VV are inversely proportional, not directly proportional. A straight line through the origin only appears when one quantity is a constant multiple of another, as in y=kxy = kx. Here P=constant/VP = \text{constant}/V, which is the equation of a hyperbola — it falls steeply at small volumes and flattens out at large volumes, but never becomes a straight line or touches either axis.

Does Boyle's Law work for any gas, in any amount?

It works well for a fixed mass of a given gas behaving as an ideal gas, which most real gases approximate closely at ordinary pressures and temperatures. The mass must stay fixed because P1V1=P2V2P_1V_1 = P_2V_2 compares the same amount of gas before and after; if you add or remove gas, both PP and VV can change for reasons that have nothing to do with Boyle's Law. At very high pressure or very low temperature, real gases deviate from this ideal behaviour, but that lies beyond the ICSE syllabus.

How is Boyle's Law different from the other gas laws I will meet in this chapter?

Boyle's Law is specifically the pressure-volume relationship at constant temperature. Later in the same chapter you will meet Charles's Law, which relates volume and temperature at constant pressure, and the combined gas equation, which lets pressure, volume and temperature all change together for a fixed mass of gas. Boyle's Law is the special case of the combined equation where temperature is deliberately held fixed.

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