CHEM-7.4

The Combined & Ideal Gas Laws

Master the combined gas law and PV = nRT: pick the right R, convert to kelvin, match your units, and solve for pressure, volume, temperature, or moles.

What you'll do in this lesson

A voice-first session with the Crimsora tutor on The Combined & Ideal Gas Laws, then targeted practice and FRQs — with the tutor adapting to where you get stuck.

What this lesson covers

You already know Boyle's, Charles's, and Gay-Lussac's laws, each holding two variables fixed while two others trade off. Real gas samples rarely cooperate that neatly — a weather balloon rising through the atmosphere changes pressure, volume, and temperature all at once. The combined gas law bundles those three relationships into one equation, and the ideal gas law goes one step further by bringing in the amount of gas, in moles.

This lesson shows you how to decide which equation a problem calls for, how to choose the right value of the gas constant RR, and why every temperature must be in kelvin before it touches an equation. The math is short; the care is in the setup. Most mistakes in this topic are not algebra errors at all — they are unit errors, and they are completely preventable once you know where to look.

The Combined Gas Law: One Equation for Changing Conditions

The combined gas law merges Boyle's, Charles's, and Gay-Lussac's laws into a single relationship for a fixed amount of gas:P1V1T1=P2V2T2\frac{P_1V_1}{T_1} = \frac{P_2V_2}{T_2}Read it as a statement that the quantity PVT\frac{PV}{T} stays constant for a sealed sample. If the gas is compressed, its pressure must rise or its temperature must fall to keep the ratio balanced.

Each of the earlier laws is hiding inside this one. If temperature is held constant, T1=T2T_1 = T_2 cancels and you are left with P1V1=P2V2P_1V_1 = P_2V_2, which is Boyle's law. If pressure is constant, you get V1T1=V2T2\frac{V_1}{T_1} = \frac{V_2}{T_2}, Charles's law. If volume is constant — a rigid steel tank, for instance — you get P1T1=P2T2\frac{P_1}{T_1} = \frac{P_2}{T_2}, Gay-Lussac's law. That means you never have to memorize four equations. Memorize one and cancel whatever does not change.

Because the combined gas law compares two states of the same sample, units only have to be consistent between the two sides, not any particular set. If V1V_1 is in milliliters, V2V_2 comes out in milliliters. If P1P_1 is in kPa, use kPa for P2P_2. The one exception is temperature: TT appears in a denominator, so a Celsius value of zero or a negative Celsius value would break the math entirely. Temperature must always be absolute.

A useful habit is to solve for the unknown symbolically first. For V2V_2:V2=V1×P1P2×T2T1V_2 = V_1 \times \frac{P_1}{P_2} \times \frac{T_2}{T_1}Then check the two ratios against physical sense. If pressure dropped, P1P2\frac{P_1}{P_2} should be greater than 1 and the volume should grow.

Why Temperature Must Be in Kelvin

Gas laws describe proportionality, and proportionality only works from a true zero. The Celsius scale places its zero at the freezing point of water, an arbitrary reference. Absolute zero, 273.15 C-273.15\ ^\circ\text{C}, is where the kinetic-molecular model says particle motion stops, so it is the only zero that makes "twice the temperature means twice the average kinetic energy" a true statement.

Convert with T(K)=T(C)+273.15T(\text{K}) = T(^\circ\text{C}) + 273.15, or +273+273 when the data have three significant figures.

Here is the concrete damage Celsius does. Take a gas at 10.0 C10.0\ ^\circ\text{C} that is warmed to 20.0 C20.0\ ^\circ\text{C} at constant pressure. Using Celsius numbers you would predict the volume doubles. Using kelvin, 283.15 K293.15 K283.15\ \text{K} \to 293.15\ \text{K}, the volume grows by about 3.5 percent. The Celsius answer is not slightly off; it is wrong by a factor of nearly 30.
SituationCelsius valueKelvin valueWhat Celsius does to the math
Ice water0 C0\ ^\circ\text{C}273 K273\ \text{K}Division by zero
Dry ice78 C-78\ ^\circ\text{C}195 K195\ \text{K}Negative volume predicted
Room temp25 C25\ ^\circ\text{C}298 K298\ \text{K}Ratios badly distorted
The reverse error also shows up: students convert to kelvin, solve correctly, and then report a final temperature of 350350 without noting the unit, or subtract 273273 when the question wanted kelvin. Write the unit on every line, and if a problem gives Celsius data it usually expects a Celsius answer — convert back at the end, after the algebra is finished.

The Ideal Gas Law and Choosing R

The combined gas law compares two states, but it cannot tell you how much gas you have. The ideal gas law can:PV=nRTPV = nRTHere nn is moles and RR is the universal gas constant. Use PV=nRTPV = nRT whenever a problem involves one set of conditions and mentions moles, grams, or molar mass. Use the combined gas law when a sample changes from one set of conditions to another.

RR is one physical constant written in different units, and the units you pick must match the units in your data.
Value of RRUnitsUse when pressure is in
0.08210.0821LatmmolK\frac{\text{L}\cdot\text{atm}}{\text{mol}\cdot\text{K}}atmospheres
8.3148.314LkPamolK\frac{\text{L}\cdot\text{kPa}}{\text{mol}\cdot\text{K}}kilopascals
62.462.4LmmHgmolK\frac{\text{L}\cdot\text{mmHg}}{\text{mol}\cdot\text{K}}mmHg or torr
Every version demands volume in liters, temperature in kelvin, and amount in moles. Milliliters must become liters (÷1000\div 1000); grams must become moles (divide by molar mass).

A quick sanity check: at standard temperature and pressure, 273 K273\ \text{K} and 1 atm1\ \text{atm}, one mole of an ideal gas occupiesV=nRTP=(1)(0.0821)(273)122.4 LV = \frac{nRT}{P} = \frac{(1)(0.0821)(273)}{1} \approx 22.4\ \text{L}If your answer for roughly one mole near room conditions comes out near 0.02240.0224 or 22,40022{,}400, you dropped or added a factor of 1000 somewhere in a volume conversion.

The law is called ideal for a reason: it assumes particles have no volume and no attractions. Real gases follow it closely at ordinary temperatures and moderate pressures, and deviate at very high pressure or very low temperature, where particles are crowded and attractions matter.

Setting Up Problems Without Getting Lost

A reliable routine handles almost every problem in this topic.

First, list what you are given with units, and mark the unknown. Second, decide which equation fits: two states means the combined gas law, one state with an amount of gas means PV=nRTPV = nRT. Third, convert — kelvin always, liters for PV=nRTPV = nRT, and pressures matched to your chosen RR. Fourth, rearrange algebraically before substituting numbers. Fifth, check whether the answer moved in the direction physics says it should.

The most common places students go wrong:

Forgetting that a rigid or sealed container fixes volume. Words like "steel cylinder," "rigid tank," or "bulb" mean V1=V2V_1 = V_2, so those terms cancel.

Mixing pressure units within one problem — using 760 mmHg760\ \text{mmHg} for the initial pressure and 0.85 atm0.85\ \text{atm} for the final. Convert one to the other first. Remember 1 atm=760 mmHg=760 torr=101.3 kPa1\ \text{atm} = 760\ \text{mmHg} = 760\ \text{torr} = 101.3\ \text{kPa}.

Using PV=nRTPV = nRT for a problem where moles never appear. If the amount of gas is unchanged and unmentioned, the combined gas law is faster and needs no constant.

Inverting a ratio. If a gas is cooled at constant pressure, the volume must shrink; if your answer grew, you multiplied by T1T2\frac{T_1}{T_2} instead of T2T1\frac{T_2}{T_1}.

Leaving mass as grams. PV=nRTPV = nRT has no slot for grams. Convert with n=mMn = \frac{m}{M}, where MM is molar mass in grams per mole. Substituting that in gives PV=mMRTPV = \frac{m}{M}RT, which is how these problems connect to finding an unknown gas's molar mass.

Key terms

Combined gas law.
The relationship P1V1T1=P2V2T2\frac{P_1V_1}{T_1} = \frac{P_2V_2}{T_2}, valid for a fixed amount of gas moving between two sets of conditions.
Ideal gas law.
PV=nRTPV = nRT, relating pressure, volume, moles, and absolute temperature of a gas at a single set of conditions.
Universal gas constant (R).
The proportionality constant in PV=nRTPV = nRT; equal to 0.0821 LatmmolK0.0821\ \frac{\text{L}\cdot\text{atm}}{\text{mol}\cdot\text{K}}, 8.314 LkPamolK8.314\ \frac{\text{L}\cdot\text{kPa}}{\text{mol}\cdot\text{K}}, or 62.4 LmmHgmolK62.4\ \frac{\text{L}\cdot\text{mmHg}}{\text{mol}\cdot\text{K}}.
Absolute temperature.
Temperature measured on the Kelvin scale, whose zero is absolute zero; found from T(K)=T(C)+273.15T(\text{K}) = T(^\circ\text{C}) + 273.15.
Ideal gas.
A model gas whose particles occupy no volume and exert no attractive forces on one another; real gases approach this behavior at low pressure and high temperature.
STP.
Standard temperature and pressure, 273 K273\ \text{K} and 1 atm1\ \text{atm}, at which one mole of an ideal gas occupies 22.4 L22.4\ \text{L}.
Molar volume.
The volume occupied by one mole of a gas at stated conditions; 22.4 L/mol22.4\ \text{L/mol} at STP.
Rigid container.
A vessel whose volume cannot change, making V1=V2V_1 = V_2 so the volume terms cancel from the combined gas law.

Worked example

A weather balloon holds 4.50 L of helium at 1.05 atm and 22 °C. It rises until the surrounding pressure is 0.720 atm and the temperature is −8 °C. (a) What is the new volume of the balloon? (b) How many moles of helium are in the balloon?
Part (a) — two states, so use the combined gas law.

List and convert. P1=1.05 atmP_1 = 1.05\ \text{atm}, V1=4.50 LV_1 = 4.50\ \text{L}, T1=22+273=295 KT_1 = 22 + 273 = 295\ \text{K}. P2=0.720 atmP_2 = 0.720\ \text{atm}, V2=?V_2 = ?, T2=8+273=265 KT_2 = -8 + 273 = 265\ \text{K}. Both pressures are already in atm, so no pressure conversion is needed.

Rearrange before substituting:V2=V1×P1P2×T2T1V_2 = V_1 \times \frac{P_1}{P_2} \times \frac{T_2}{T_1}Substitute:V2=4.50 L×1.050.720×265295V_2 = 4.50\ \text{L} \times \frac{1.05}{0.720} \times \frac{265}{295}V2=4.50×1.458×0.8983=5.89 LV_2 = 4.50 \times 1.458 \times 0.8983 = 5.89\ \text{L}Sense check: the pressure dropped a lot (expansion) while the temperature dropped only a little (slight contraction). Expansion should win, and it did — 5.89 L is larger than 4.50 L.

Part (b) — one state with an amount of gas, so use PV=nRTPV = nRT.

Use the ground-level conditions and R=0.0821 LatmmolKR = 0.0821\ \frac{\text{L}\cdot\text{atm}}{\text{mol}\cdot\text{K}} because pressure is in atm.n=PVRT=(1.05 atm)(4.50 L)(0.0821)(295 K)=4.72524.22=0.195 moln = \frac{PV}{RT} = \frac{(1.05\ \text{atm})(4.50\ \text{L})}{(0.0821)(295\ \text{K})} = \frac{4.725}{24.22} = 0.195\ \text{mol}Verify with the high-altitude conditions, since the balloon is sealed and nn cannot change:n=(0.720)(5.89)(0.0821)(265)=4.2421.76=0.195 moln = \frac{(0.720)(5.89)}{(0.0821)(265)} = \frac{4.24}{21.76} = 0.195\ \text{mol}The two agree, which confirms part (a). That cross-check is worth doing whenever a problem gives you both states.

Practice questions

A sealed 10.0 L flask contains 2.00 mol of nitrogen gas at 27 °C. What is the pressure inside the flask?
  1. 0.164 atm
  2. 0.493 atm
  3. 4.93 atm
  4. 44.3 atm

Answer: 4.93 atm

Only one set of conditions is given and moles are named, so use PV=nRTPV = nRT. Convert the temperature first: 27+273=300 K27 + 273 = 300\ \text{K}. Using R=0.0821 LatmmolKR = 0.0821\ \frac{\text{L}\cdot\text{atm}}{\text{mol}\cdot\text{K}}, P=nRTV=(2.00)(0.0821)(300)10.0=49.2610.0=4.93 atmP = \frac{nRT}{V} = \frac{(2.00)(0.0821)(300)}{10.0} = \frac{49.26}{10.0} = 4.93\ \text{atm}. The value 44.3 atm comes from leaving the temperature in Celsius and multiplying incorrectly, and 0.493 atm comes from a misplaced decimal in the division. A quick reality check helps: 2 moles squeezed into 10 L is denser than the 22.4 L per mole at STP, so the pressure should be several atmospheres, not a fraction of one.
A rigid steel cylinder of oxygen reads 15.0 atm at 20.0 °C. It is left in a hot truck and warms to 65.0 °C. Calculate the new pressure, and explain why you do not need to know the cylinder's volume.

Answer: About 17.3 atm.

Start from the combined gas law, P1V1T1=P2V2T2\frac{P_1V_1}{T_1} = \frac{P_2V_2}{T_2}. The word rigid means the cylinder cannot expand, so V1=V2V_1 = V_2 and both volume terms cancel, leaving P1T1=P2T2\frac{P_1}{T_1} = \frac{P_2}{T_2} — Gay-Lussac's law emerging from the general equation. Because volume cancels algebraically, its actual value never matters. Convert temperatures: T1=293 KT_1 = 293\ \text{K} and T2=338 KT_2 = 338\ \text{K}. Then P2=P1×T2T1=15.0×338293=17.3 atmP_2 = P_1 \times \frac{T_2}{T_1} = 15.0 \times \frac{338}{293} = 17.3\ \text{atm}. Heating raised the pressure, which matches the kinetic-molecular picture: faster particles strike the walls harder and more often in the same space.
A student solving a gas problem writes PV=nRTPV = nRT with P=745 mmHgP = 745\ \text{mmHg}, V=250. mLV = 250.\ \text{mL}, T=25 CT = 25\ ^\circ\text{C}, and R=0.0821 LatmmolKR = 0.0821\ \frac{\text{L}\cdot\text{atm}}{\text{mol}\cdot\text{K}}. Identify every unit problem and give the corrected values.

Answer: Three problems: pressure must be converted to atm (0.980 atm), volume to liters (0.250 L), and temperature to kelvin (298 K).

The chosen RR carries units of LatmmolK\frac{\text{L}\cdot\text{atm}}{\text{mol}\cdot\text{K}}, so every quantity substituted into the equation must use those same units. Pressure: 745 mmHg×1 atm760 mmHg=0.980 atm745\ \text{mmHg} \times \frac{1\ \text{atm}}{760\ \text{mmHg}} = 0.980\ \text{atm}. Volume: 250. mL×1 L1000 mL=0.250 L250.\ \text{mL} \times \frac{1\ \text{L}}{1000\ \text{mL}} = 0.250\ \text{L}. Temperature: 25+273=298 K25 + 273 = 298\ \text{K}. An equally valid alternative is to keep the pressure in mmHg and switch to R=62.4 LmmHgmolKR = 62.4\ \frac{\text{L}\cdot\text{mmHg}}{\text{mol}\cdot\text{K}}, but volume and temperature still need converting. With the corrections, n=(0.980)(0.250)(0.0821)(298)=0.0100 moln = \frac{(0.980)(0.250)}{(0.0821)(298)} = 0.0100\ \text{mol}.

FAQ

How do I know whether to use the combined gas law or PV = nRT?
Count the sets of conditions. If the problem describes a gas changing — before and after, initial and final, at the surface and at altitude — you have two states and the combined gas law applies. If it describes a single situation and mentions moles, grams, or molar mass, use PV=nRTPV = nRT. A tell-tale sign for the combined gas law is that the amount of gas is never given and never changes, so it cancels out of the comparison.
Which value of R should I use?
Match RR to the pressure unit in your data. Use 0.08210.0821 with atmospheres, 8.3148.314 with kilopascals, and 62.462.4 with mmHg or torr. All three require liters, kelvin, and moles no matter which one you pick. If your data mix pressure units, convert everything to one unit first, then choose the matching RR.
Why can't I just use Celsius if I use it consistently on both sides?
Because the gas laws are proportionalities that require a scale starting at true zero. Celsius zero is the freezing point of water, not the absence of molecular motion, so ratios of Celsius temperatures are meaningless. Worse, TT sits in a denominator in the combined gas law, so 0 C0\ ^\circ\text{C} would mean dividing by zero and any temperature below freezing would predict a negative volume.
Where does the 22.4 L per mole at STP number come from?
It is just PV=nRTPV = nRT evaluated at standard conditions. Substituting n=1 moln = 1\ \text{mol}, P=1 atmP = 1\ \text{atm}, T=273 KT = 273\ \text{K}, and R=0.0821R = 0.0821 gives V=22.4 LV = 22.4\ \text{L}. Because it is a consequence of the ideal gas law rather than a separate rule, it applies only at STP — at any other temperature or pressure you must recalculate. It is still a handy benchmark for checking whether an answer is physically reasonable.

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