Membrane Tension and Laplace Pressure Calculator

Convert membrane tension into the pressure difference it can sustain across a curved surface, and check the resulting areal strain against the bilayer lysis limit.

🫧 Membrane Tension and Laplace Pressure Calculator
Membrane tension (σ)
mN/m
0.01 mN/m50 mN/m
Radius of curvature (R)10 µm
µm
Geometry
Area compressibility modulus (KA)
mN/m
Laplace pressure (ΔP)
—
ΔP in mmHg
—
Areal strain (σ / KA)
—
Step-by-step working

🫧 What is Membrane Tension and Laplace Pressure?

Membrane tension is the in-plane force per unit length carried by a membrane, and Laplace pressure is the pressure difference that tension can sustain across a curved surface. The two are linked by the Young-Laplace equation, which for a sphere reads ΔP = 2σ/R. This calculator applies that relation for the three geometries that matter in cell biology and soft matter, a sphere with one interface, a soap bubble with two, and a cylinder such as a membrane tether, and it also converts the tension into the areal strain the membrane must be carrying.

The relation shows up constantly in practice. Respiratory physiology uses it to explain why pulmonary surfactant is essential, since without it the tension of the alveolar air-liquid interface would generate hundreds of pascals of collapse pressure in the smallest alveoli. Vesicle and liposome researchers use it to predict how much internal pressure a giant unilamellar vesicle can hold before lysing during micropipette aspiration. Cell mechanics groups use it to interpret tether-pulling experiments, and microfluidics engineers use the same equation to compute the capillary pressure needed to push a droplet through a narrow channel.

The most common error is applying the soap-bubble factor of 4 to a cell or a lipid vesicle. A soap film has two air-liquid interfaces, so both contribute, while a bilayer has a single mechanical surface and takes the factor 2. A second frequent mistake is treating membrane tension as a fixed material constant like the surface tension of water. It is not. Membrane tension is an elastic response, roughly KA times the fractional area change, so it rises steeply from near zero as the membrane is stretched and collapses back when area is added.

This calculator is useful because the unit chain from millinewtons per meter and micrometres to pascals is easy to get wrong by three or six orders of magnitude, and because it immediately reports the areal strain implied by the tension you entered. That strain check is the fastest way to see whether the scenario you are modelling is physically survivable for a lipid bilayer, which typically ruptures somewhere around 3% to 5% areal strain.

📐 Formula

ΔP  =  n × σ ÷ R
ΔP = pressure difference across the surface, in pascals
σ = membrane tension, in N/m (this calculator accepts mN/m and converts internally)
R = radius of curvature, in meters (this calculator accepts micrometres and converts internally)
n = geometry factor: 2 for a sphere, vesicle or cell, 4 for a soap bubble with two interfaces, 1 for a cylinder, tether or tube
Areal strain: α = σ ÷ KA, where KA is the area compressibility modulus, about 240 mN/m for a fluid bilayer
Unit conversions: 1 mmHg = 133.322 Pa and 1 atm = 101325 Pa
Example: σ=0.5 mN/m on a sphere of R=10 µm gives ΔP = 100.00 Pa, which is 0.750 mmHg.

📖 How to Use This Calculator

Steps

1
Enter the membrane tension. Set the membrane tension in millinewtons per meter using the slider or the number box, typically well under 1 mN/m for a resting cell.
2
Enter the radius of curvature. Type the radius of the vesicle, cell, bubble, or tube in micrometres.
3
Choose the geometry. Select sphere (factor 2), soap bubble (factor 4), or cylinder (factor 1) to match the surface you are modelling.
4
Read the pressure and strain. See the pressure difference in pascals and mmHg, the areal strain with a lysis warning, the radius table, and the pressure versus radius chart.

💡 Example Calculations

Example 1 — Giant Unilamellar Vesicle under Micropipette Aspiration

σ=0.5 mN/m, R=10 µm, sphere geometry, KA=240 mN/m

1
Convert units: σ = 0.5 mN/m = 5×10⁻⁴ N/m and R = 10 µm = 1×10⁻⁵ m
2
ΔP = 2σ/R = 2 × 5×10⁻⁴ ÷ 1×10⁻⁵ = 100.00 Pa, which is 0.750 mmHg
3
Areal strain α = 0.5 ÷ 240 = 0.208%, far below the 3% to 5% lysis strain, so the vesicle is safely inside its elastic range
ΔP = 100.00 Pa (0.750 mmHg), areal strain 0.208%
Try this example →

Example 2 — Alveolus with No Pulmonary Surfactant

σ=25 mN/m (bare air-liquid interface), R=100 µm, sphere geometry, KA=240 mN/m

1
σ = 25 mN/m = 0.025 N/m and R = 100 µm = 1×10⁻⁴ m
2
ΔP = 2 × 0.025 ÷ 1×10⁻⁴ = 500.00 Pa = 3.750 mmHg, a collapse pressure the lung would have to fight on every breath
3
The implied areal strain of 10.417% is far beyond bilayer lysis, which is exactly why the alveolar surface needs surfactant to drop its tension as the radius shrinks
ΔP = 500.00 Pa (3.750 mmHg), areal strain 10.417%
Try this example →

Example 3 — Soap Bubble with Two Interfaces

σ=25 mN/m, R=5000 µm (a 5 mm bubble), soap bubble geometry, KA=240 mN/m

1
A soap film has an outer and an inner interface, so the geometry factor is 4 rather than 2
2
ΔP = 4σ/R = 4 × 0.025 ÷ 5×10⁻³ = 20.00 Pa = 0.150 mmHg
3
The pressure is far smaller than Example 2 despite the identical tension, because the bubble radius is 50 times larger
ΔP = 20.00 Pa (0.150 mmHg), areal strain 10.417%
Try this example →

Example 4 — Membrane Tether Pulled from a Cell

σ=1 mN/m, R=0.05 µm (a 50 nm radius tube), cylinder geometry, KA=240 mN/m

1
A cylinder is curved in one direction only, so the geometry factor drops to 1 and ΔP = σ/R
2
ΔP = 1×10⁻³ ÷ 5×10⁻⁸ = 20000.00 Pa = 150.012 mmHg = 20 kPa
3
The tiny radius makes this a very large pressure even at a modest tension, and the areal strain of 0.417% remains perfectly safe for the bilayer itself
ΔP = 20000.00 Pa (150.012 mmHg), areal strain 0.417%
Try this example →

❓ Frequently Asked Questions

What is the Young-Laplace equation for a membrane?+
For a spherical membrane the Young-Laplace equation is dP = 2 sigma / R, where dP is the pressure difference across the membrane, sigma is the membrane tension, and R is the radius of curvature. A soap bubble with two interfaces uses dP = 4 sigma / R, and a cylinder uses dP = sigma / R.
Why is the factor 4 used for a soap bubble but 2 for a cell?+
A soap bubble has two air-liquid interfaces, an outer and an inner surface, and each contributes its own 2 sigma / R, giving 4 sigma / R in total. A lipid vesicle or a cell has a single mechanical membrane, so the correct factor is 2. Using 4 for a cell doubles the computed pressure.
What is a typical membrane tension in a living cell?+
Resting plasma-membrane tension in animal cells is usually measured between about 0.003 and 0.04 mN/m by tether pulling, rising several-fold during spreading, migration, or osmotic swelling. Giant unilamellar vesicles under micropipette aspiration are commonly studied between 0.01 and 5 mN/m.
At what tension does a lipid bilayer rupture?+
Fluid phospholipid bilayers lyse at roughly 3 to 10 mN/m, corresponding to an areal strain of about 3% to 5% because the area compressibility modulus is around 240 mN/m. This calculator reports the areal strain and flags values in that danger band.
How do I convert Laplace pressure from pascals to mmHg?+
Divide the pressure in pascals by 133.322 to get millimetres of mercury. For example, a 500 Pa pressure difference is 3.75 mmHg. The calculator reports both units, plus kilopascals in the reference table.
How does radius affect Laplace pressure?+
Pressure scales inversely with radius, so halving the radius doubles the pressure difference at constant tension. That is why small vesicles and capillaries sustain far higher pressure differences than large ones, and why the pressure curve on this page is a hyperbola rather than a straight line.
What is areal strain and how is it related to tension?+
Areal strain is the fractional increase in membrane area, alpha = sigma / K_A, where K_A is the area compressibility modulus (about 240 mN/m for a fluid bilayer). A tension of 5 mN/m therefore stretches the membrane area by about 2%, which is already close to the rupture limit.
Why does the alveolus need surfactant according to Laplace's law?+
Without surfactant the air-liquid interface of an alveolus would have a tension near 25 mN/m, producing about 500 Pa of collapse pressure at a 100 micrometre radius. Pulmonary surfactant drops the tension several-fold at small radii, which lowers the pressure and stops small alveoli from emptying into large ones.
Does Laplace pressure apply to membrane tethers and tubes?+
Yes, but with the cylindrical form dP = sigma / R, because a cylinder is curved in one direction only. A 50 nm radius tether at 1 mN/m therefore sustains about 20 kPa, which is very large compared with the pressure a giant vesicle sustains at the same tension.
What is the difference between membrane tension and surface tension?+
Both have units of force per length, but surface tension arises from cohesive forces at a liquid interface and is a fixed material property, while membrane tension is an elastic response to stretching, given by K_A times the areal strain. A bilayer therefore has no single fixed tension, its tension depends on how much its area has been stretched.
How is membrane tension measured in the laboratory?+
The main techniques are micropipette aspiration of giant unilamellar vesicles, optical-tweezers tether pulling, atomic force microscopy indentation, and fluorescent membrane-tension probes such as Flipper-TR. Micropipette aspiration is the reference method because it sets tension directly through the suction pressure.
Can Laplace pressure explain why cells resist osmotic swelling?+
Partly. As a cell swells, membrane area strain rises and tension climbs steeply because K_A is large, and the resulting Laplace pressure opposes further inflow. However the membrane can only stretch a few percent before lysing, so cells mainly rely on regulatory volume decrease and mechanosensitive channels rather than membrane elasticity alone.

What is the Young-Laplace equation for a membrane?

For a spherical membrane the Young-Laplace equation is dP = 2 sigma / R, where dP is the pressure difference across the membrane, sigma is the membrane tension, and R is the radius of curvature. A soap bubble with two interfaces uses dP = 4 sigma / R, and a cylinder uses dP = sigma / R.

Why is the factor 4 used for a soap bubble but 2 for a cell?

A soap bubble has two air-liquid interfaces, an outer and an inner surface, and each contributes its own 2 sigma / R, giving 4 sigma / R in total. A lipid vesicle or a cell has a single mechanical membrane, so the correct factor is 2. Using 4 for a cell doubles the computed pressure.

What is a typical membrane tension in a living cell?

Resting plasma-membrane tension in animal cells is usually measured between about 0.003 and 0.04 mN/m by tether pulling, rising several-fold during spreading, migration, or osmotic swelling. Giant unilamellar vesicles under micropipette aspiration are commonly studied between 0.01 and 5 mN/m.

At what tension does a lipid bilayer rupture?

Fluid phospholipid bilayers lyse at roughly 3 to 10 mN/m, corresponding to an areal strain of about 3% to 5% because the area compressibility modulus is around 240 mN/m. This calculator reports the areal strain and flags values in that danger band.

How do I convert Laplace pressure from pascals to mmHg?

Divide the pressure in pascals by 133.322 to get millimetres of mercury. For example, a 500 Pa pressure difference is 3.75 mmHg. The calculator reports both units, plus kilopascals in the reference table.

How does radius affect Laplace pressure?

Pressure scales inversely with radius, so halving the radius doubles the pressure difference at constant tension. That is why small vesicles and capillaries sustain far higher pressure differences than large ones, and why the pressure curve on this page is a hyperbola rather than a straight line.

What is areal strain and how is it related to tension?

Areal strain is the fractional increase in membrane area, alpha = sigma / K_A, where K_A is the area compressibility modulus (about 240 mN/m for a fluid bilayer). A tension of 5 mN/m therefore stretches the membrane area by about 2%, which is already close to the rupture limit.

Why does the alveolus need surfactant according to Laplace's law?

Without surfactant the air-liquid interface of an alveolus would have a tension near 25 mN/m, producing about 500 Pa of collapse pressure at a 100 micrometre radius. Pulmonary surfactant drops the tension several-fold at small radii, which lowers the pressure and stops small alveoli from emptying into large ones.

Does Laplace pressure apply to membrane tethers and tubes?

Yes, but with the cylindrical form dP = sigma / R, because a cylinder is curved in one direction only. A 50 nm radius tether at 1 mN/m therefore sustains about 20 kPa, which is very large compared with the pressure a giant vesicle sustains at the same tension.

What is the difference between membrane tension and surface tension?

Both have units of force per length, but surface tension arises from cohesive forces at a liquid interface and is a fixed material property, while membrane tension is an elastic response to stretching, given by K_A times the areal strain. A bilayer therefore has no single fixed tension, its tension depends on how much its area has been stretched.

How is membrane tension measured in the laboratory?

The main techniques are micropipette aspiration of giant unilamellar vesicles, optical-tweezers tether pulling, atomic force microscopy indentation, and fluorescent membrane-tension probes such as Flipper-TR. Micropipette aspiration is the reference method because it sets tension directly through the suction pressure.

Can Laplace pressure explain why cells resist osmotic swelling?

Partly. As a cell swells, membrane area strain rises and tension climbs steeply because K_A is large, and the resulting Laplace pressure opposes further inflow. However the membrane can only stretch a few percent before lysing, so cells mainly rely on regulatory volume decrease and mechanosensitive channels rather than membrane elasticity alone.