Torr to Standard atmospheres (Torr to atm)
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Torr-to-atmospheres conversions are the within-pressure scale roll-up that translates Torr-precision vacuum-technology, semiconductor-fabrication and physics-laboratory figures into the standard-atmosphere reference unit used in chemistry, physics and meteorology. A 760 Torr atmospheric reference rolls up to exactly 1 atm by the unit's definition; a 380 Torr partial-vacuum chamber rolls up to 0.5 atm; a 1520 Torr above-atmospheric pressurised chamber rolls up to 2 atm. The conversion is the canonical reference equivalence between the two pressure units that Torricelli's 1643 mercury-barometer experiment originally connected, with one Torr defined as exactly 1/760 of a standard atmosphere by BIPM convention adopted in 1958. The conversion runs at every Torr-precision-source to atm-reference-destination boundary across vacuum-technology, physics-laboratory and chemistry contexts.
How to convert Torr to Standard atmospheres
Formula
atm = Torr × 0.001316
To convert Torr to atmospheres, divide the Torr figure by 760 — equivalently, multiply by 0.00131579, the atm value of one Torr. The factor is exact by the BIPM 1958 definition that fixed one Torr as exactly 1/760 of a standard atmosphere. For mental math, "Torr ÷ 760" lands the atm figure cleanly: 760 Torr is 1 atm, 380 Torr is 0.5 atm, 760,000 Torr would be 1000 atm (hypothetical, well above any practical pressure). The conversion runs at every Torr-precision-source to atm-reference-destination boundary, particularly common in vacuum-technology equipment work, semiconductor-fabrication process documentation, physics-laboratory thermodynamic cross-references, and pressure-swing-adsorption cycle-analysis documentation. The factor is exact rather than approximate and is one of the cleanest within-pressure-unit conversions in modern measurement.
Worked examples
Example 1 — 760 Torr
Seven hundred and sixty Torr — by definition exactly one standard atmosphere — converts to 760 / 760 = exactly 1 atm. That is the canonical "1 atm = 760 Torr" reference equivalence anchored in Torricelli's 1643 mercury-barometer experiment and formalised at BIPM in 1958. The relationship is exact rather than approximate.
Example 2 — 380 Torr
Three hundred and eighty Torr — half the standard-atmosphere reference — converts to 380 / 760 = 0.5 atm. That is a typical partial-vacuum chamber pressure, the kind of figure used in physics-laboratory experiments studying gas behaviour at sub-atmospheric pressures, with the Torr-figure on the chamber gauge and the atm-figure on the thermodynamic-calculation documentation.
Example 3 — 0.001 Torr
One thousandth of a Torr — a typical high-vacuum laboratory pressure — converts to 0.001 / 760 = 1.32 × 10⁻⁶ atm. That is the figure on physics-laboratory thermodynamic calculations for high-vacuum chamber experiments, with the Torr-figure on the vacuum-gauge display and the atm-figure on the ideal-gas-law calculation. Ultra-high-vacuum work runs at even lower pressures (10⁻⁹ to 10⁻¹² Torr).
Torr to atm conversion table
| Torr | atm |
|---|---|
| 1 Torr | 0.0013 atm |
| 2 Torr | 0.0026 atm |
| 3 Torr | 0.0039 atm |
| 4 Torr | 0.0053 atm |
| 5 Torr | 0.0066 atm |
| 6 Torr | 0.0079 atm |
| 7 Torr | 0.0092 atm |
| 8 Torr | 0.0105 atm |
| 9 Torr | 0.0118 atm |
| 10 Torr | 0.0132 atm |
| 15 Torr | 0.0197 atm |
| 20 Torr | 0.0263 atm |
| 25 Torr | 0.0329 atm |
| 30 Torr | 0.0395 atm |
| 40 Torr | 0.0526 atm |
| 50 Torr | 0.0658 atm |
| 75 Torr | 0.0987 atm |
| 100 Torr | 0.1316 atm |
| 150 Torr | 0.1974 atm |
| 200 Torr | 0.2632 atm |
| 250 Torr | 0.3289 atm |
| 500 Torr | 0.6579 atm |
| 750 Torr | 0.9868 atm |
| 1000 Torr | 1.3158 atm |
| 2500 Torr | 3.2895 atm |
| 5000 Torr | 6.5789 atm |
Common Torr to atm conversions
- 0.001 Torr=0 atm
- 0.01 Torr=0 atm
- 1 Torr=0.0013 atm
- 10 Torr=0.0132 atm
- 76 Torr=0.1 atm
- 100 Torr=0.1316 atm
- 380 Torr=0.5 atm
- 500 Torr=0.6579 atm
- 760 Torr=1 atm
- 1520 Torr=2 atm
What is a Torr?
One Torr is defined as exactly 1/760 of a standard atmosphere, which equals exactly 101,325/760 = 133.322368... pascals. The relationship to the millimetre of mercury (mmHg) is very close but technically distinct: 1 mmHg = 133.322387415 Pa per the BIPM definition based on standard gravity acting on a column of mercury, while 1 Torr = 133.322368... Pa per the 1/760-atmosphere definition. The two values differ by about 0.000015% and are interchangeable for all practical purposes outside high-precision metrology. The recognised symbol is "Torr" (capitalised, in honour of Torricelli), occasionally seen as "torr" in casual writing but BIPM convention preserves the capital. Vacuum-technology pressure ranges span from ultra-high vacuum (10⁻⁹ Torr and below) through high vacuum (10⁻³ to 10⁻⁹ Torr), medium vacuum (10⁻³ to 1 Torr), low vacuum (1 to 760 Torr) up to atmospheric (760 Torr). Above atmospheric the unit is rarely used; pressure scales transition to bar or kPa.
The Torr is named after Evangelista Torricelli (1608-1647), the Italian physicist and mathematician who in 1643 demonstrated atmospheric pressure with the first mercury barometer — a sealed glass tube inverted in a dish of mercury, with the mercury column standing at the height proportional to atmospheric pressure. Torricelli's barometer experiment, originally proposed by Galileo and executed by Torricelli in his role as Galileo's secretary, established that air has weight and that a column of mercury about 760 mm tall at sea level is equal in weight to the column of air above it. The unit named in Torricelli's honour was formally adopted at the BIPM in 1958 as exactly 1/760 of a standard atmosphere, making it numerically very close to but legally distinct from the millimetre of mercury (mmHg). Both units are used in vacuum technology, with Torr being the dominant convention in physics laboratories and high-vacuum technology and mmHg dominating in clinical medicine and meteorology. The Torr is not part of the SI but is recognised by NIST and BIPM as a non-SI unit accepted for limited use; ISO 80000-4 deprecates it in favour of pascals for new technical writing.
Vacuum technology and high-vacuum laboratory work: physics-laboratory vacuum chambers, semiconductor-fabrication chambers, mass-spectrometry source pressures, electron-microscopy vacuum levels and surface-science laboratory work all denominate working pressures in Torr. Ultra-high-vacuum chambers operate at 10⁻⁹ to 10⁻¹² Torr; high-vacuum lithography systems at 10⁻⁶ to 10⁻⁸ Torr; mass-spectrometer source regions at 10⁻⁵ to 10⁻⁷ Torr; electron-microscope columns at 10⁻⁴ to 10⁻⁶ Torr. Edwards, Pfeiffer, Leybold and Agilent vacuum-equipment manufacturers all preserve Torr alongside Pa and mbar on their product specs and pressure-gauge displays. Semiconductor manufacturing: photolithography, plasma etching, chemical-vapour deposition (CVD) and physical-vapour deposition (PVD) chambers all run at sub-atmospheric pressures denominated in Torr in industry-standard tooling specifications. ASML, Lam Research, Applied Materials and Tokyo Electron all use Torr alongside Pa on their semiconductor process-tool spec sheets. Pressure-swing adsorption gas separation: industrial gas-purification systems (oxygen concentrators, hydrogen purifiers) cycle between low-Torr and atmospheric pressures with Torr as the conventional low-side pressure unit. Medical vacuum: chest-tube drainage and surgical-suction equipment operates at Torr-scale pressures (50-200 mmHg/Torr below atmospheric), with the Torr-vs-mmHg distinction immaterial at the precision required for clinical use.
What is a Standard atmosphere?
One standard atmosphere (atm) is defined as exactly 101,325 pascals (101.325 kPa) by the 10th CGPM resolution of 1954. This value is also equal to exactly 760 millimetres of mercury (mmHg, or torr) at 0 °C under standard gravity — the equivalence is by definition, not by measurement, and was specifically constructed so that the older mercury-column convention and the pascal-based SI convention give the same numerical reference. Conversions to other commonly-encountered pressure units: 1 atm = 1.01325 bar exactly, 1 atm = 14.6959488 psi, 1 atm = 29.9213 inches of mercury, and 1 atm = 1,013.25 millibar / hectopascal. The unit symbol "atm" is recognised by the BIPM but explicitly listed as a non-SI unit whose use is discouraged in favour of the pascal — yet it persists in chemistry, hyperbaric medicine and diving because the magnitude is human-scale and the gas-law formulas are taught in terms of it. A closely related notation, "ATA" (atmospheres absolute), is used in diving and hyperbaric work to make explicit that the pressure is referenced to a perfect vacuum rather than to local atmospheric pressure — so 1 ATA at the surface, 2 ATA at 10 metres of seawater, and so on.
The standard atmosphere descends from Evangelista Torricelli's 1644 barometric experiment in Florence, in which a glass tube sealed at one end and filled with mercury was inverted into a dish of mercury; the column settled at about 760 mm above the dish, balanced by atmospheric pressure on the dish surface. Pascal's 1648 Puy de Dôme expedition extended Torricelli's work to confirm altitude dependence, and the 760 mm value became the conventional reference for "one atmosphere" of pressure across the eighteenth and nineteenth centuries. Through that period the standard atmosphere consolidated as the reference pressure for gas-law work — Boyle's law (1662), Charles's law (1787), Avogadro's hypothesis (1811), and the unified ideal-gas equation pV = nRT all referenced atmospheric pressure as the natural baseline, and chemistry developed a deep practical reliance on the atm as the working pressure unit for laboratory calculations. The modern numerical definition was fixed by the 10th General Conference on Weights and Measures (CGPM) in 1954 — the same conference that defined the kelvin against the triple point of water — at 1 atm = 101,325 Pa exactly. The CGPM framed the value as the mean atmospheric pressure at sea level, 45° latitude, 0 °C: an idealised reference rather than a directly measured quantity, closing nearly two centuries of small national variations in the assumed value. In 1982, IUPAC redefined "standard temperature and pressure" (STP) from 0 °C + 1 atm to 0 °C + 1 bar (100,000 Pa) for SI alignment. The older 1 atm definition remains in the educational literature and many engineering reference works, and the resulting "old STP" / "new STP" split is the most persistent legacy issue in introductory chemistry pedagogy.
Chemistry and gas-law calculations are the centerpiece of atm's active educational and laboratory use. Every introductory and physical-chemistry textbook in the English-speaking world (Atkins, McQuarrie-Simon, Levine, Zumdahl) presents the ideal-gas equation pV = nRT with worked examples in which the pressure variable carries units of atm, and the universal gas constant R is most commonly memorised in its convenient form 0.08206 L·atm·mol⁻¹·K⁻¹ rather than its SI form 8.314 J·mol⁻¹·K⁻¹. Dalton's law of partial pressures, Henry's law for gas solubility, Raoult's law for vapour pressure of solutions, and the equilibrium constant Kp (defined in terms of partial pressures) all conventionally use atm as the reference pressure. The molar volume of an ideal gas at the older STP convention (0 °C, 1 atm) is the famous 22.414 litres per mole, a value memorised by chemistry students for almost a century — superseded numerically but not pedagogically by the 22.711 L/mol of the post-1982 STP convention. Diving and decompression theory: recreational and technical diving teaches depth-pressure as multiples of one atmosphere absolute (ATA), with one additional atmosphere added for every ten metres of seawater depth. A diver at 10 m experiences 2 ATA, at 20 m experiences 3 ATA, at 30 m (the recreational limit on air without decompression-stop training) experiences 4 ATA, and a technical diver at 60 m experiences 7 ATA. The US Navy Diving Manual decompression tables, the PADI and SSI recreational dive tables, and the algorithm-driven dive computers (Bühlmann ZH-L16, VPM-B, RGBM) all denominate ambient pressure in ATA for the decompression-modelling calculations even when the cylinder gauge on the same dive reads in bar. Henry's law gas-loading and off-loading from body tissues — the foundation of decompression theory — is computed in terms of ambient ATA partial pressures of nitrogen and helium. Hyperbaric medicine: clinical hyperbaric oxygen therapy (HBOT) prescribes treatment pressures explicitly in ATA. The Undersea and Hyperbaric Medical Society (UHMS) approved indications for HBOT specify treatment regimes typically at 2.0–2.4 ATA for chronic wound healing, diabetic foot ulcers, radiation tissue injury, and carbon monoxide poisoning, with severe decompression sickness and arterial gas embolism treated under US Navy Treatment Table 6 at 2.8 ATA. Hospital monoplace and multiplace hyperbaric chambers display chamber pressure in ATA on the operator console as the primary clinical variable. Autoclave sterilisation: hospital and laboratory steam autoclaves operate at approximately 1 atm gauge pressure (about 2 ATA absolute) at 121 °C for 15–30 minutes per the CDC's Guideline for Disinfection and Sterilisation in Healthcare Facilities and the ANSI/AAMI ST79 comprehensive sterilisation guide; the higher 134 °C "flash" cycle uses about 2 atm gauge (3 ATA absolute) for shorter exposure. ASME Boiler and Pressure Vessel Code Section VIII pressure-vessel calculations for autoclave design carry the ratings in psi for the US market and bar for European, but clinical and microbiological literature consistently report cycle parameters in atm. Planetary science uses atm as a convenient ratio reference for comparing other planetary atmospheres to Earth's: the surface pressure of Venus is about 92 atm (a crushing nine-kilometre-deep ocean equivalent in pressure terms), Mars surface is about 0.006 atm (well below the Armstrong limit of 0.0618 atm at which water boils at body temperature), Titan's surface is about 1.45 atm, and the gas-giant atmospheres are conventionally measured against the 1 atm "surface" level of their pressure profiles since they have no solid surface.
Real-world uses for Torr to Standard atmospheres
Vacuum-technology Torr operating pressures translated to atm-reference physics calculations
Vacuum-technology equipment (Edwards, Pfeiffer, Leybold, Agilent vacuum pumps and chambers) operates at Torr-precision pressures across the ultra-high-vacuum to atmospheric range, with chamber-pressure readings translated to atm for the physics-laboratory thermodynamic calculation. A 760 Torr atmospheric chamber pressure rolls up to 1 atm for the ideal-gas-law calculation; a 0.001 Torr ultra-high-vacuum rolls up to 1.32 × 10⁻⁶ atm. The conversion runs at every chamber-pressure to thermodynamic-calculation step in vacuum-technology laboratory work.
Semiconductor-fabrication Torr process pressures translated to atm-equivalent process documentation
Semiconductor-fabrication equipment (ASML photolithography tools, Lam Research etch systems, Applied Materials CVD/PVD systems, Tokyo Electron deposition systems) runs process chambers at Torr-precision pressures but the process-engineering documentation references atm-equivalents for cross-disciplinary engineering review. A 1 Torr CVD process pressure rolls up to 0.001316 atm; a 100 Torr atmospheric-pressure CVD process rolls up to 0.1316 atm. The conversion runs at every process-spec documentation step.
Physics-laboratory Torr vacuum readings cross-referenced to atm thermodynamic calculations
Physics-laboratory work (mass-spectrometry, electron-microscopy, surface-science research, laser-cooling experiments) operates at Torr-precision vacuum levels with frequent cross-reference to atm for thermodynamic calculations and gas-law applications. A 10⁻⁶ Torr electron-microscope column pressure rolls up to 1.32 × 10⁻⁹ atm for the ideal-gas-law mean-free-path calculation; a 10⁻³ Torr mass-spectrometer source rolls up to 1.32 × 10⁻⁶ atm. The conversion runs at every vacuum-physics laboratory thermodynamic-cross-reference step.
Pressure-swing-adsorption Torr cycle pressures translated to atm-reference cycle analysis
Industrial pressure-swing-adsorption (PSA) gas-purification systems (oxygen concentrators for medical-grade O2 production, hydrogen-purification systems, nitrogen-generation systems) cycle between low-Torr and atmospheric pressures with Torr-precision cycle-pressure readings rolled up to atm for the thermodynamic-cycle-analysis documentation. A 76 Torr low-cycle pressure rolls up to 0.1 atm; a 760 Torr atmospheric cycle endpoint rolls up to 1 atm. The conversion runs at every PSA-cycle thermodynamic-analysis step.
When to use Standard atmospheres instead of Torr
Use atmospheres whenever the destination is a chemistry, physics or meteorology reference, an ideal-gas-law thermodynamic-calculation input, an international scientific publication, or any context where the standard-atmosphere reference is the natural unit. Atm is the universal scientific reference pressure unit. Stay in Torr when the destination is a vacuum-technology equipment gauge, semiconductor-fabrication process-pressure spec, physics-laboratory chamber-pressure reading, or any high-precision sub-atmospheric vacuum work where Torr granularity is the natural unit. The conversion is at the vacuum-technology-source to scientific-reference-destination boundary, with the Torr figure on the vacuum-gauge side and the atm figure on the thermodynamic-calculation side. Most everyday vacuum-technology work preserves Torr throughout; the atm-equivalent appears only on cross-disciplinary thermodynamic-calculation documentation.
Common mistakes converting Torr to atm
- Treating Torr and mmHg as exactly equivalent in high-precision metrology. The two definitions differ by about 0.000015% (1 Torr = 133.322 Pa exactly, 1 mmHg = 133.322 Pa per a separate gravity-and-mercury-column definition). For everyday vacuum-technology, semiconductor-fabrication, and physics-laboratory work the two are interchangeable; for primary-standards calibration laboratories the distinction matters.
- Reporting vacuum-pressure figures as decimal-Torr without specifying the gauge type. Bayard-Alpert ionisation gauges (the standard high-vacuum gauge) are gas-species dependent (calibrated typically against nitrogen), and a "10⁻⁶ Torr" reading on argon may differ from the equivalent nitrogen-equivalent pressure by a factor of two or more. Cross-spec vacuum documentation should specify gauge type and gas calibration.
Frequently asked questions
How many atm in 760 Torr?
Seven hundred and sixty Torr equals exactly 1 atm by the unit's definition. That is the canonical "1 atm = 760 Torr" reference equivalence, formalised at BIPM in 1958 with one Torr defined as exactly 1/760 of a standard atmosphere. The relationship is exact rather than approximate, and the same 760 Torr equals 101,325 Pa or 14.696 psi as the standard sea-level atmospheric pressure reference.
How many atm in 380 Torr?
Three hundred and eighty Torr equals exactly 0.5 atm — half the standard atmospheric pressure. That is a typical partial-vacuum chamber pressure used in physics-laboratory experiments studying gas behaviour at sub-atmospheric pressures, with the Torr-figure on the vacuum-gauge display and the atm-figure on the thermodynamic-calculation documentation. Half-atmosphere pressures are common in physiology research and pressure-cycling studies.
Why is 1 atm exactly 760 Torr?
One atmosphere was historically defined as the pressure exerted by a 760 mm column of mercury at sea level (the height Torricelli observed in his 1643 mercury-barometer experiment). When BIPM formalised the Torr unit in 1958, they fixed one Torr as exactly 1/760 of a standard atmosphere, making the "1 atm = 760 Torr" relationship exact by definition rather than approximate. The 760 figure is therefore historical-experimental rather than calculated.
Quick way to convert Torr to atm in my head?
Divide the Torr figure by 760 — for round-numbered Torr figures the conversion is straightforward: 760 Torr is 1 atm, 380 Torr is 0.5 atm, 76 Torr is 0.1 atm, 7.6 Torr is 0.01 atm. For non-round-numbered Torr figures the conversion benefits from a calculator, since 760 is not a power of 10 and the mental division is non-trivial.
Is Torr the same as mmHg?
For all practical purposes, yes — one Torr equals one millimetre of mercury (mmHg) to within about 0.000015%. The two units have slightly different definitions (Torr is 1/760 of a standard atmosphere; mmHg is the pressure of a 1 mm column of mercury at standard gravity), but the numerical difference is immaterial outside primary-standards metrology laboratories. Vacuum-technology and physics-laboratory work treats them as interchangeable.
When does Torr-to-atm conversion appear in real work?
Torr-to-atm appears in vacuum-technology operating pressures translated to atm-reference physics calculations, semiconductor-fabrication process pressures translated to atm-equivalent process documentation, physics-laboratory vacuum readings cross-referenced to atm thermodynamic calculations, and pressure-swing-adsorption cycle pressures translated to atm-reference cycle analysis. The conversion is uncommon in everyday consumer work but routine in vacuum-technology, semiconductor and physics-laboratory contexts. Each case rolls up Torr-precision vacuum-equipment readings into atm-reference thermodynamic-calculation documentation.
How precise should Torr-to-atm be for vacuum-technology work?
For vacuum-technology equipment work the Torr-to-atm conversion is exact at the BIPM definition (1 Torr = 1/760 atm), and the typical vacuum-gauge precision (±5% for ionisation gauges, ±2% for capacitance manometers) limits the practical precision of the conversion result. The exact 1/760 factor preserves precision through the conversion; gauge-precision and gas-calibration corrections are the relevant precision allowances. Primary-standards calibration laboratories preserve full BIPM-defined precision through the conversion step itself.