In a mixture of gases, each constituent gas has a partial pressure which is the notional pressure of that constituent gas as if it alone occupied the entire volume of the original mixture at the same temperature.^[1] The total pressure of an ideal gas mixture is the sum of the partial pressures of the gases in the mixture (Dalton's Law).

The partial pressure of a gas is a measure of thermodynamic activity of the gas's molecules. Gases dissolve, diffuse, and react according to their partial pressures but not according to their concentrations in gas mixtures or liquids. This general property of gases is also true in chemical reactions of gases in biology. For example, the necessary amount of oxygen for human respiration, and the amount that is toxic, is set by the partial pressure of oxygen alone. This is true across a very wide range of different concentrations of oxygen present in various inhaled breathing gases or dissolved in blood;^[2] consequently, mixture ratios, like that of breathable 20% oxygen and 80% Nitrogen, are determined by volume instead of by weight or mass.^[3] Furthermore, the partial pressures of oxygen and carbon dioxide are important parameters in tests of arterial blood gases. That said, these pressures can also be measured in, for example, cerebrospinal fluid.

Symbol

The symbol for pressure is usually P or p which may use a subscript to identify the pressure, and gas species are also referred to by subscript. When combined, these subscripts are applied recursively.^[4][5]

Examples:

• ${\displaystyle P_{1))$ or ${\displaystyle p_{1))$ = pressure at time 1
• ${\displaystyle P_((\ce {H2))))$ or ${\displaystyle p_((\ce {H2))))$ = partial pressure of hydrogen
• ${\displaystyle P_{a_((\ce {O2))))}$ or ${\displaystyle p_{a_((\ce {O2))))}$ or P_aO₂ = arterial partial pressure of oxygen
• ${\displaystyle P_{v_((\ce {O2))))}$ or ${\displaystyle p_{v_((\ce {O2))))}$ or P_vO₂ = venous partial pressure of oxygen

Dalton's law of partial pressures

Dalton's law expresses the fact that the total pressure of a mixture of ideal gases is equal to the sum of the partial pressures of the individual gases in the mixture.^[6] This equality arises from the fact that in an ideal gas, the molecules are so far apart that they do not interact with each other. Most actual real-world gases come very close to this ideal. For example, given an ideal gas mixture of nitrogen (N₂), hydrogen (H₂) and ammonia (NH₃):

$${\displaystyle p=p_((\ce {N2))}+p_((\ce {H2))}+p_((\ce {NH3))))$$

• ${\displaystyle p}$ = total pressure of the gas mixture
• ${\displaystyle p_((\ce {N2))))$ = partial pressure of nitrogen (N₂)
• ${\displaystyle p_((\ce {H2))))$ = partial pressure of hydrogen (H₂)
• ${\displaystyle p_((\ce {NH3))))$ = partial pressure of ammonia (NH₃)

Ideal gas mixtures

Ideally the ratio of partial pressures equals the ratio of the number of molecules. That is, the mole fraction ${\displaystyle x_{\mathrm {i} ))$ of an individual gas component in an ideal gas mixture can be expressed in terms of the component's partial pressure or the moles of the component:

$${\displaystyle x_{\mathrm {i} }={\frac {p_{\mathrm {i} )){p))={\frac {n_{\mathrm {i} )){n))}$$

and the partial pressure of an individual gas component in an ideal gas can be obtained using this expression:

$${\displaystyle p_{\mathrm {i} }=x_{\mathrm {i} }\cdot p}$$

where:
${\displaystyle x_{\mathrm {i} ))$	= mole fraction of any individual gas component in a gas mixture
${\displaystyle p_{\mathrm {i} ))$	= partial pressure of any individual gas component in a gas mixture
${\displaystyle n_{\mathrm {i} ))$	= moles of any individual gas component in a gas mixture
${\displaystyle n}$	= total moles of the gas mixture
${\displaystyle p}$	= total pressure of the gas mixture

The mole fraction of a gas component in a gas mixture is equal to the volumetric fraction of that component in a gas mixture.^[7]

The ratio of partial pressures relies on the following isotherm relation:

$${\displaystyle {\frac {V_{\rm {X))}{V_{\rm {tot))))={\frac {p_{\rm {X))}{p_{\rm {tot))))={\frac {n_{\rm {X))}{n_{\rm {tot))))}$$

• V_X is the partial volume of any individual gas component (X)
• V_tot is the total volume of the gas mixture
• p_X is the partial pressure of gas X
• p_tot is the total pressure of the gas mixture
• n_X is the amount of substance of gas (X)
• n_tot is the total amount of substance in gas mixture

Partial volume (Amagat's law of additive volume)

The partial volume of a particular gas in a mixture is the volume of one component of the gas mixture. It is useful in gas mixtures, e.g. air, to focus on one particular gas component, e.g. oxygen.

It can be approximated both from partial pressure and molar fraction:^[8]

$${\displaystyle V_{\rm {X))=V_{\rm {tot))\times {\frac {p_{\rm {X))}{p_{\rm {tot))))=V_{\rm {tot))\times {\frac {n_{\rm {X))}{n_{\rm {tot))))}$$

• V_X is the partial volume of an individual gas component X in the mixture
• V_tot is the total volume of the gas mixture
• p_X is the partial pressure of gas X
• p_tot is the total pressure of the gas mixture
• n_X is the amount of substance of gas X
• n_tot is the total amount of substance in the gas mixture

Vapor pressure

Vapor pressure is the pressure of a vapor in equilibrium with its non-vapor phases (i.e., liquid or solid). Most often the term is used to describe a liquid's tendency to evaporate. It is a measure of the tendency of molecules and atoms to escape from a liquid or a solid. A liquid's atmospheric pressure boiling point corresponds to the temperature at which its vapor pressure is equal to the surrounding atmospheric pressure and it is often called the normal boiling point.

The higher the vapor pressure of a liquid at a given temperature, the lower the normal boiling point of the liquid.

The vapor pressure chart displayed has graphs of the vapor pressures versus temperatures for a variety of liquids.^[9] As can be seen in the chart, the liquids with the highest vapor pressures have the lowest normal boiling points.

For example, at any given temperature, methyl chloride has the highest vapor pressure of any of the liquids in the chart. It also has the lowest normal boiling point (−24.2 °C), which is where the vapor pressure curve of methyl chloride (the blue line) intersects the horizontal pressure line of one atmosphere (atm) of absolute vapor pressure. At higher altitudes, the atmospheric pressure is less than that at sea level, so boiling points of liquids are reduced. At the top of Mount Everest, the atmospheric pressure is approximately 0.333 atm, so by using the graph, the boiling point of diethyl ether would be approximately 7.5 °C versus 34.6 °C at sea level (1 atm).

Equilibrium constants of reactions involving gas mixtures

It is possible to work out the equilibrium constant for a chemical reaction involving a mixture of gases given the partial pressure of each gas and the overall reaction formula. For a reversible reaction involving gas reactants and gas products, such as:

$${\displaystyle {\ce (({\mathit {a))A}+((\mathit {b))B}<=>((\mathit {c))C}+((\mathit {d))D))))$$

the equilibrium constant of the reaction would be:

$${\displaystyle K_{\mathrm {p} }={\frac {p_{C}^{c}\,p_{D}^{d)){p_{A}^{a}\,p_{B}^{b))))$$

where:
${\displaystyle K_{p))$	=  the equilibrium constant of the reaction
${\displaystyle a}$	=  coefficient of reactant ${\displaystyle A}$
${\displaystyle b}$	=  coefficient of reactant ${\displaystyle B}$
${\displaystyle c}$	=  coefficient of product ${\displaystyle C}$
${\displaystyle d}$	=  coefficient of product ${\displaystyle D}$
${\displaystyle p_{C}^{c))$	=  the partial pressure of ${\displaystyle C}$ raised to the power of ${\displaystyle c}$
${\displaystyle p_{D}^{d))$	=  the partial pressure of ${\displaystyle D}$ raised to the power of ${\displaystyle d}$
${\displaystyle p_{A}^{a))$	=  the partial pressure of ${\displaystyle A}$ raised to the power of ${\displaystyle a}$
${\displaystyle p_{B}^{b))$	=  the partial pressure of ${\displaystyle B}$ raised to the power of ${\displaystyle b}$

For reversible reactions, changes in the total pressure, temperature or reactant concentrations will shift the equilibrium so as to favor either the right or left side of the reaction in accordance with Le Chatelier's Principle. However, the reaction kinetics may either oppose or enhance the equilibrium shift. In some cases, the reaction kinetics may be the overriding factor to consider.

Henry's law and the solubility of gases

Gases will dissolve in liquids to an extent that is determined by the equilibrium between the undissolved gas and the gas that has dissolved in the liquid (called the solvent).^[10] The equilibrium constant for that equilibrium is:

$${\displaystyle k={\frac {p_{x)){C_{x))))$$

(1)

where:

• ${\displaystyle k}$ =  the equilibrium constant for the solvation process
• ${\displaystyle p_{x))$ =  partial pressure of gas ${\displaystyle x}$ in equilibrium with a solution containing some of the gas
• ${\displaystyle C_{x))$ =  the concentration of gas ${\displaystyle x}$ in the liquid solution

The form of the equilibrium constant shows that the concentration of a solute gas in a solution is directly proportional to the partial pressure of that gas above the solution. This statement is known as Henry's law and the equilibrium constant ${\displaystyle k}$ is quite often referred to as the Henry's law constant.^[10][11][12]

Henry's law is sometimes written as:^[13]

$${\displaystyle k'={\frac {C_{x)){p_{x))))$$

(2)

where ${\displaystyle k'}$ is also referred to as the Henry's law constant.^[13] As can be seen by comparing equations (1) and (2) above, ${\displaystyle k'}$ is the reciprocal of ${\displaystyle k}$. Since both may be referred to as the Henry's law constant, readers of the technical literature must be quite careful to note which version of the Henry's law equation is being used.

Henry's law is an approximation that only applies for dilute, ideal solutions and for solutions where the liquid solvent does not react chemically with the gas being dissolved.

In diving breathing gases

In underwater diving the physiological effects of individual component gases of breathing gases are a function of partial pressure.^[14]

Using diving terms, partial pressure is calculated as:

partial pressure = (total absolute pressure) × (volume fraction of gas component)^[14]

For the component gas "i":

p_i = P × F_i^[14]

For example, at 50 metres (164 ft) underwater, the total absolute pressure is 6 bar (600 kPa) (i.e., 1 bar of atmospheric pressure + 5 bar of water pressure) and the partial pressures of the main components of air, oxygen 21% by volume and nitrogen approximately 79% by volume are:

pN₂ = 6 bar × 0.79 = 4.7 bar absolute

pO₂ = 6 bar × 0.21 = 1.3 bar absolute

where:
pi	= partial pressure of gas component i  = ${\displaystyle P_{\mathrm {i} ))$ in the terms used in this article
P	= total pressure = ${\displaystyle P}$ in the terms used in this article
Fi	= volume fraction of gas component i  =  mole fraction, ${\displaystyle x_{\mathrm {i} ))$, in the terms used in this article
pN2	= partial pressure of nitrogen  = ${\displaystyle P_{\mathrm {N_{2)) ))$ in the terms used in this article
pO2	= partial pressure of oxygen  = ${\displaystyle P_{\mathrm {O_{2)) ))$ in the terms used in this article

The minimum safe lower limit for the partial pressures of oxygen in a breathing gas mixture for diving is 0.16 bars (16 kPa) absolute. Hypoxia and sudden unconsciousness can become a problem with an oxygen partial pressure of less than 0.16 bar absolute.^[15] Oxygen toxicity, involving convulsions, becomes a problem when oxygen partial pressure is too high. The NOAA Diving Manual recommends a maximum single exposure of 45 minutes at 1.6 bar absolute, of 120 minutes at 1.5 bar absolute, of 150 minutes at 1.4 bar absolute, of 180 minutes at 1.3 bar absolute and of 210 minutes at 1.2 bar absolute. Oxygen toxicity becomes a risk when these oxygen partial pressures and exposures are exceeded. The partial pressure of oxygen also determines the maximum operating depth of a gas mixture.^[14]

Narcosis is a problem when breathing gases at high pressure. Typically, the maximum total partial pressure of narcotic gases used when planning for technical diving may be around 4.5 bar absolute, based on an equivalent narcotic depth of 35 metres (115 ft).

The effect of a toxic contaminant such as carbon monoxide in breathing gas is also related to the partial pressure when breathed. A mixture which may be relatively safe at the surface could be dangerously toxic at the maximum depth of a dive, or a tolerable level of carbon dioxide in the breathing loop of a diving rebreather may become intolerable within seconds during descent when the partial pressure rapidly increases, and could lead to panic or incapacitation of the diver.^[14]

In medicine

The partial pressures of particularly oxygen (${\displaystyle p_{\mathrm {O_{2)) ))$) and carbon dioxide (${\displaystyle p_{\mathrm {CO_{2)) ))$) are important parameters in tests of arterial blood gases, but can also be measured in, for example, cerebrospinal fluid.^[why?]

Reference ranges for ${\displaystyle p_{\mathrm {O_{2)) ))$ and ${\displaystyle p_{\mathrm {CO_{2)) ))$

	Unit	Arterial blood gas	Venous blood gas	Cerebrospinal fluid	Alveolar pulmonary gas pressures
${\displaystyle p_{\mathrm {O_{2)) ))$	kPa	11–13[16]	4.0–5.3[16]	5.3–5.9[16]	14.2
	mmHg	75–100[17]	30–40[18]	40–44[19]	107
${\displaystyle p_{\mathrm {CO_{2)) ))$	kPa	4.7–6.0[16]	5.5–6.8[16]	5.9–6.7[16]	4.8
	mmHg	35–45[17]	41–51[18]	44–50[19]	36