Partial Pressure Calculator
How it Works
01Pick the Method
Dalton (gas-mix), Ideal gas (n,T,V), Henry method 1 (K in L·atm/mol), or method 2 (K in atm).
02Dalton or Ideal Gas
P_i = x_i · P_total (Dalton) or P = nRT/V (ideal gas) — for known mixtures or pure conditions.
03Henry's Law (Dissolved Gases)
P = K_H · C (concentration form) or P = K_H · x (mole-fraction form) for gas-liquid equilibria.
04Get Partial Pressure
Output in your chosen unit (kPa / atm / bar / mmHg / psi / torr / Pa) with conversion to all 7.
What is a Partial Pressure Calculator?
The calculator includes built-in Henry's law constants for 8 common gases at 25 °C: Oxygen, Nitrogen, Carbon dioxide, Hydrogen, Helium, Methane, Argon, and Carbon monoxide — sourced from the CRC Handbook of Chemistry and Physics. Output gives the partial pressure in 7 different pressure units simultaneously (Pa, kPa, atm, bar, mmHg, psi, torr) so you can copy whichever unit your downstream calculation, instrument, or report requires.
Designed for chemistry students learning gas laws, atmospheric scientists modelling gas exchange (CO₂ flux at the ocean surface, water-vapour saturation), respiratory physiologists analysing alveolar O₂ / CO₂, divers calculating partial pressures at depth (oxygen toxicity at > 1.4 atm; nitrogen narcosis depth limits), HVAC engineers spec'ing humidity control, and any researcher needing to convert between concentration and equilibrium gas pressure, the tool runs entirely in your browser — no account, no data stored.
Pro Tip: Pair this with our Molarity Calculator for stock preparation, our Serial Dilution Calculator for concentration series, or our Rate Constant Calculator for kinetics analysis.
How to Use the Partial Pressure Calculator?
How is partial pressure calculated?
Four equations for partial pressure, each from a different chapter of physical chemistry. All assume ideal gas behaviour; Henry's law adds the dilute-solution assumption.
References: Atkins' Physical Chemistry, IUPAC Quantities Units and Symbols, CRC Handbook of Chemistry and Physics for Henry's law constants.
1. Dalton's Law of Partial Pressures (1801)
P_i = x_i · P_total
where P_i is the partial pressure of component i, x_i is its mole fraction (n_i / n_total), and P_total is the total pressure of the mixture. Equivalently P_total = Σ P_i — the total pressure equals the sum of partial pressures.
Standard example: dry atmospheric air has x_N₂ = 0.781, x_O₂ = 0.209, x_Ar = 0.0093, x_CO₂ ≈ 4.2×10⁻⁴. At sea level (P_total = 101.325 kPa): P_O₂ = 0.209 × 101.325 = 21.18 kPa.
2. Ideal Gas Law for a Single Component
P = n · R · T / V
where n is moles, R = 8.31446 J/(mol·K) is the universal gas constant, T is absolute temperature in K, V is volume in m³. Result: P in Pa.
Useful when you know amount of substance and container conditions — common in vacuum-line gas handling, cylinder pressure calculations, balloon experiments. For a gas mixture, apply this to each component individually with its own n_i to get P_i.
3. Henry's Law — Method 1 (Concentration Form)
P_gas = K_H · C_dissolved
where C is the concentration of dissolved gas in mol/L (= M), and K_H has units of L·atm/mol. P_gas comes out in atm. The Henry's law constant K_H is gas-specific and temperature-dependent.
For O₂ in water at 25 °C: K_H = 769.2 L·atm/mol. So 1 mM dissolved O₂ corresponds to gas-phase pressure 769.2 × 0.001 = 0.7692 atm = 78 kPa above the solution at equilibrium.
4. Henry's Law — Method 2 (Mole-Fraction Form)
P_gas = K_H · x_dissolved
where x is the mole fraction of dissolved gas, and K_H has units of atm (the mole-fraction form of Henry's constant). Same physical situation as method 1, but uses dimensionless mole fraction instead of molar concentration.
For O₂ in water at 25 °C: K_H = 42,590 atm. So if x_O₂ in water = 4×10⁻⁶ (typical saturation at 1 atm O₂), P_O₂ = 42,590 × 4×10⁻⁶ = 0.17 atm. Method 2 is preferred in chemical engineering and physical chemistry texts; method 1 is preferred in environmental and biological chemistry.
Henry's Law Constants at 25 °C (CRC Handbook):
- Oxygen (O₂): K_H1 = 769.2 L·atm/mol; K_H2 = 42,590 atm.
- Nitrogen (N₂): K_H1 = 1639 L·atm/mol; K_H2 = 86,920 atm. (Less soluble than O₂.)
- Carbon dioxide (CO₂): K_H1 = 29.4 L·atm/mol; K_H2 = 1605 atm. (Far more soluble than O₂ — the chemistry of carbonated drinks.)
- Hydrogen (H₂): K_H1 = 1282 L·atm/mol; K_H2 = 71,420 atm.
- Helium (He): K_H1 = 2700 L·atm/mol; K_H2 = 144,300 atm. (Lowest solubility of common gases.)
- Methane (CH₄): K_H1 = 714 L·atm/mol; K_H2 = 41,470 atm.
- Argon (Ar): K_H1 = 715 L·atm/mol; K_H2 = 39,930 atm.
- Carbon monoxide (CO): K_H1 = 1052 L·atm/mol; K_H2 = 56,440 atm.
Pressure Unit Conversions
- 1 atm = 101,325 Pa = 101.325 kPa = 1.01325 bar = 760 mmHg = 760 torr = 14.696 psi.
- 1 bar = 100,000 Pa = 100 kPa = 0.987 atm = 750.06 mmHg = 14.504 psi.
- 1 mmHg = 1 torr = 133.322 Pa.
- 1 psi = 6,894.76 Pa.
SI standard pressure unit is the pascal (Pa), but practical chemistry uses atm or kPa most commonly. Vacuum work uses torr (= mmHg) at typical 10⁻³ to 10⁻⁹ ranges. Engineering and meteorology often use bar or kPa. Tire pressure and US plumbing use psi.
Partial Pressure – Worked Examples
- P_O₂ = 0.209 × 101.325 = 21.18 kPa = 0.209 atm = 159 mmHg.
- Equivalent to 21.18 kPa O₂ partial pressure entering alveoli — the basis of pulmonary gas-exchange physiology.
- At altitude (lower P_total), P_O₂ scales proportionally — at 5,000 m where P_total ≈ 54 kPa, P_O₂ drops to ~11 kPa, half of sea-level value (the basis of altitude sickness).
Example 2 — Helium Tank (Ideal Gas). 0.5 mol He in a 10 L tank at 25 °C.
- T = 25 + 273.15 = 298.15 K. V = 10 L = 0.01 m³.
- P = nRT/V = 0.5 × 8.314 × 298.15 / 0.01 = 123,924 Pa = 124 kPa = 1.22 atm.
- Compare to ideal-gas-law verification: at 1 atm, 25 °C, 0.5 mol fills 22.4 × 0.5 × (298/273) ≈ 12.2 L. Our 10 L gives slightly higher pressure (1.22 atm), consistent.
Example 3 — Dissolved O₂ in Water (Henry Method 1). Lake water analysis: dissolved O₂ measured at 0.27 mM (typical for cold well-aerated water).
- K_H1 (O₂ in water at 25 °C) = 769.2 L·atm/mol.
- P_O₂ = 769.2 × 0.27×10⁻³ = 0.208 atm = 21.0 kPa.
- Matches the atmospheric O₂ partial pressure (Example 1) — the lake is at equilibrium with the atmosphere, as expected for an open well-aerated water body.
- At the water surface, dissolved O₂ saturation drops with temperature (warmer water holds less O₂) — this is the basis of summer fish kills in eutrophic lakes.
Example 4 — Carbonated Beverage (Henry Method 1). Coca-Cola has dissolved CO₂ at ~0.1 M (sweet-spot for pleasant carbonation).
- K_H1 (CO₂ in water at 25 °C) = 29.4 L·atm/mol (CO₂ is far more soluble than O₂).
- P_CO₂ above the liquid at equilibrium = 29.4 × 0.1 = 2.94 atm = 297 kPa.
- This is the CO₂ pressure inside the sealed bottle. Open it: P_CO₂ above the liquid drops to atmospheric ~4×10⁻⁴ atm; the dissolved CO₂ supersaturated by ~7,000-fold rapidly bubbles out — the famous fizzing.
Example 5 — Same Equilibrium via Method 2 (Henry Mole-Fraction). O₂ saturation in water at 1 atm O₂.
- Inverse calculation: at equilibrium with P_O₂ = 1 atm, what's x_O₂ in water?
- x_O₂ = P / K_H2 = 1 / 42,590 = 2.35 × 10⁻⁵ mole fraction (extremely small — O₂ is sparingly soluble).
- In molar terms (using density of water 55.5 mol/L): C_O₂ = 2.35×10⁻⁵ × 55.5 = 1.30 × 10⁻³ M = 1.30 mM. Cross-check method 1: P = 769.2 × 1.30×10⁻³ = 1.00 atm ✓.
- The two Henry methods give identical results when the conversion factor (water density 55.5 mol/L for dilute aqueous solutions) is properly applied.
Who Should Use the Partial Pressure Calculator?
Technical Reference
Dalton's Law — Historical and Practical. John Dalton published the law of partial pressures in 1801 in his "New System of Chemical Philosophy". The law states that gases in a mixture behave independently — each component contributes a partial pressure equal to what it would exert alone in the container. Dalton's law is exact for ideal gases and very accurate (better than 1%) for real gases at low to moderate pressures. It breaks down at high pressures where intermolecular forces become significant — for high-pressure gas mixtures, use the Lewis-Randall fugacity rule or full equation-of-state mixing rules.
Ideal Gas Law and Real-Gas Corrections. The ideal gas law PV = nRT (and its rearrangement P = nRT/V for partial pressure) assumes: (1) gas molecules occupy negligible volume; (2) intermolecular forces are negligible; (3) collisions are perfectly elastic. These approximations are excellent at low pressures (P ≤ 10 atm), high temperatures (T ≥ 100 K), and for small / non-polar gases (He, Ne, Ar, H₂, N₂, O₂, CH₄). They break down for: high-pressure compressed gases, gases near critical points (CO₂ at > 73 bar, 304 K), polar molecules (NH₃, H₂O, HCl), and at low temperatures near liquefaction. Real-gas corrections via:
- Van der Waals (1873): (P + a·n²/V²)(V − n·b) = nRT, where a corrects for intermolecular attraction and b for molecular volume. Gives qualitatively correct PVT behaviour.
- Redlich-Kwong (1949): empirical improvement over Van der Waals; better accuracy for many gases.
- Peng-Robinson (1976): the modern industrial standard for petroleum / natural-gas / refinery process design; handles both gases and liquids.
- Compressibility factor Z = PV/(nRT): the empirical correction. For ideal gas Z = 1; real gases at high P typically have Z > 1 (repulsion-dominated); at moderate P near critical, Z < 1 (attraction-dominated).
Henry's Law — Origin and Conventions. William Henry published his law in 1803: at constant temperature, the amount of a gas dissolved in a liquid is proportional to the partial pressure of the gas above the liquid. The proportionality constant K_H comes in MULTIPLE conventions that are widely confused in literature:
- K_H,cp = C / P (concentration / pressure): solubility form; units mol/(L·atm) or M/atm. Larger K_H,cp = MORE soluble gas. Used in environmental chemistry.
- K_H,pc = P / C = 1 / K_H,cp: volatility form; units L·atm/mol. Larger K_H,pc = LESS soluble gas. This is the calculator's "method 1" form.
- K_H,px = P / x: mole-fraction form; units atm. Larger K_H,px = LESS soluble gas. This is the calculator's "method 2" form.
- K_H,xp = x / P = 1 / K_H,px: reciprocal of the above; units atm⁻¹. Common in engineering.
Critical caveat: when reading published Henry's law constants, ALWAYS check which convention is used. The same gas (e.g. O₂ in water) has K_H values of 769.2 (method 1) or 42,590 (method 2) — same physics, different units. The CRC Handbook explicitly tabulates which form it uses; many papers leave it ambiguous.
Temperature Dependence of K_H — van't Hoff Equation. Henry's law constants are strongly temperature-dependent — gas solubility DECREASES with increasing temperature for most gases (an unusual entropy-driven effect). The van't Hoff form: d(ln K_H) / d(1/T) = −ΔH_sol / R, where ΔH_sol is the enthalpy of solution (typically negative — gas dissolution is exothermic). For O₂ in water: ΔH_sol ≈ −12.5 kJ/mol; warming from 25 °C to 35 °C decreases O₂ solubility by ~15%. This is why warmer water holds less dissolved O₂ — a critical issue in thermal pollution and summer fish kills.
Reference: O₂ Saturation in Water vs Temperature (at 1 atm air = P_O₂ = 0.209 atm above the surface):
- 0 °C: 14.6 mg/L = 0.456 mM dissolved O₂.
- 10 °C: 11.3 mg/L = 0.353 mM.
- 20 °C: 9.1 mg/L = 0.284 mM.
- 25 °C: 8.3 mg/L = 0.260 mM.
- 30 °C: 7.6 mg/L = 0.236 mM.
- 40 °C: 6.4 mg/L = 0.200 mM.
Aquatic-life thresholds: salmonids need ≥ 6 mg/L O₂; most warm-water fish need ≥ 4 mg/L; below 2 mg/L hypoxic / "dead zone" conditions develop.
Atmospheric Composition Reference (Dry Air, Sea Level):
- N₂: 78.084% (mole fraction 0.78084) → P_N₂ = 79.1 kPa.
- O₂: 20.946% (0.20946) → P_O₂ = 21.2 kPa.
- Ar: 0.934% (9.34×10⁻³) → P_Ar = 0.946 kPa.
- CO₂: 0.042% (~420 ppm in 2024, rising ~2.5 ppm/yr) → P_CO₂ = 0.043 kPa.
- Trace: Ne, He, CH₄, Kr, H₂, N₂O, Xe — all sub-ppm.
- Total: 101.325 kPa = 1 atm = 760 mmHg.
Diving / Hyperbaric Partial Pressure Limits:
- P_O₂ ≥ 1.4 atm: CNS oxygen toxicity risk (the "Paul Bert effect") — convulsions, blackouts. Recreational diving max 1.4 atm; technical max 1.6 atm during decompression.
- P_O₂ ≤ 0.16 atm: hypoxic (insufficient O₂); equivalent to altitude > 5,500 m on land. Loss of consciousness within minutes.
- P_N₂ ≥ ~3 atm: nitrogen narcosis ("the rapture of the deep") — judgment impairment, similar to alcohol intoxication. Equivalent to depth ~30 m breathing air.
- P_He has no narcosis effect at recreational pressures — basis of helium-oxygen (heliox) and helium-nitrogen-oxygen (trimix) breathing gases for technical / commercial diving.
- P_CO₂ ≥ 0.05 atm: hypercapnia symptoms (headache, breathlessness); equivalent to ~5% CO₂ at 1 atm — the OSHA short-term exposure limit.
Respiratory Physiology Reference:
- Alveolar P_O₂ at sea level: ~100 mmHg (lower than inspired 159 mmHg due to humidification, dilution by alveolar CO₂).
- Alveolar P_CO₂ at sea level: ~40 mmHg (set by ventilation rate; the body's primary acid-base regulator).
- Arterial P_O₂ (PaO₂): normal 80-100 mmHg; mild hypoxemia < 80; moderate < 60; severe < 40 (medical emergency).
- Arterial P_CO₂ (PaCO₂): normal 35-45 mmHg; hypercapnia > 45 (respiratory acidosis); hypocapnia < 35 (respiratory alkalosis).
- Mixed venous P_O₂: ~40 mmHg after tissues extract O₂.
When Henry's Law Breaks Down. Henry's law is the limiting law for very dilute solutions. It breaks down when:
- Gas concentration is high (typically > 1 M for sparingly soluble gases, > 0.1 M for highly soluble gases) — non-ideal interactions between dissolved gas molecules.
- Solvent is non-aqueous with strongly different polarity than water — the gas-solvent interactions can be specific (e.g. O₂ in fluorocarbons is anomalously soluble; NH₃ in water has acid-base chemistry that breaks the simple Henry framework).
- Chemical reaction occurs: CO₂ in water partially converts to carbonic acid, bicarbonate, carbonate; the "effective" solubility differs from physical Henry's law solubility.
- Near phase transitions: close to liquefaction or solidification of the dissolved gas, simple proportionality between concentration and pressure breaks down.
For these cases, use empirical solubility tables (NIST, IUPAC Solubility Data Series, CRC Handbook), activity-coefficient corrections, or full thermodynamic modelling (NRTL, UNIQUAC, equation-of-state methods like SRK, PR for non-aqueous systems).
Key Takeaways
Frequently Asked Questions
What is the Partial Pressure Calculator?
Pro Tip: Pair this with our Molarity Calculator for stock preparation.
What's Dalton's law of partial pressures?
How does the ideal gas law give partial pressure?
What's Henry's law and why are there two methods?
What's the partial pressure of O₂ in air?
How does temperature affect Henry's law constants?
Why is CO₂ so much more soluble than O₂?
What's the partial pressure of CO₂ in a Coke bottle?
What partial pressure is dangerous to breathe?
What pressure unit should I use?
When does the ideal gas approximation break down?
Disclaimer
All four methods assume ideal gas behaviour. Approximation valid for low pressures (≤ 10 atm), high temperatures (≥ 100 K), and small / non-polar gases. Breaks down at high pressures, low temperatures, polar molecules, near phase transitions. Henry's law adds the dilute-solution assumption (typically valid below ~1 M). Henry's law constants are temperature-dependent; built-in values are at 25 °C. References: CRC Handbook of Chemistry and Physics, IUPAC Quantities Units and Symbols, Atkins' Physical Chemistry. For non-ideal conditions use Van der Waals or Peng-Robinson EOS; for high-loading solutions use activity-coefficient corrections.