Young-Laplace Equation Calculator

Calculate pressure difference across curved interfaces using the Young-Laplace equation. Supports bubbles, droplets, capillary rise, meniscus curvature, and contact angle calculations.

Laplace Pressure (ΔP)
145.600 Pa
2γ/r
ΔP (hPa / mbar)
1.456
1.092 mmHg
Surface Tension
72.80 mN/m
Water (20 °C)
Capillary Length
2.73 mm
κ⁻¹ = √(γ/ρg)
ΔP / P_atm
0.1437%
Fraction of atmospheric pressure

Laplace Pressure vs Radius

15M
10nm
3M
50nm
1M
100nm
146k
1μm
15k
10μm
1k
100μm
146
1mm
15
10mm
Pressure (Pa) vs radius — note logarithmic scale

Surface Tension Reference

Liquidγ (mN/m)ρ (kg/m³)Contact Angle (glass)Cap. Length (mm)
Water (20 °C)72.899820°2.73
Water (37 °C)7099320°2.68
Ethanol22.17890°1.69
Methanol22.67910°1.71
Acetone25.27840°1.81
Mercury48513534140°1.91
Blood55106030°2.30
Benzene28.98760°1.83
Toluene28.48670°1.83
Glycerol63.4126150°2.26
Olive Oil3291130°1.89
Hexane18.46550°1.69
Lung Surfactant (min)2599820°1.60
Lung Surfactant (max)7099820°2.67
Soap Solution25101010°1.59
Isopropanol237860°1.73
DMSO43.5110030°2.01
Diethyl Ether177130°1.56
Planning notes, formulas, and examples

About the Young-Laplace Equation Calculator

The Young-Laplace equation describes the pressure difference (Laplace pressure) across a curved interface between two fluids due to surface tension. For a general surface with two principal radii of curvature R₁ and R₂: ΔP = γ(1/R₁ + 1/R₂), where γ is the surface tension.

This fundamental equation of capillarity governs soap bubbles (ΔP = 4γ/r for two interfaces), liquid droplets (ΔP = 2γ/r), capillary rise in narrow tubes, meniscus shape in containers, and the stability of foams and emulsions. It connects macroscopic surface tension to the microscopic curvature of interfaces.

This calculator computes Laplace pressure for spheres, cylinders, general ellipsoids, and capillary tubes. It includes surface tension data for common liquids, predicts capillary rise heights, and provides context for applications in microfluidics, lung surfactant physics, inkjet printing, and nanoparticle stability.

When This Page Helps

Understanding Laplace pressure is vital in microfluidics design, pharmaceutical emulsion stability, pulmonary medicine (alveolar mechanics), inkjet and 3D printing, enhanced oil recovery, and nanotechnology — wherever curved fluid interfaces determine system behavior. It also improves communication between theory and experiments by letting teams translate radius and surface-tension measurements into pressure impacts that can be validated in practical setups.

How to Use the Inputs

  1. Select the geometry: sphere (bubble/droplet), cylinder, general curvature, or capillary tube.
  2. Enter the surface tension of your liquid or select from presets.
  3. Enter the radius of curvature in the appropriate unit.
  4. For soap bubbles, the calculator automatically applies the 4γ/r formula (two surfaces).
  5. For capillary rise, enter the tube diameter and contact angle.
  6. Review the Laplace pressure and related quantities.
  7. Use the reference table for surface tension values of 20+ common liquids.
Formula used
General: ΔP = γ(1/R₁ + 1/R₂). Sphere: ΔP = 2γ/r. Soap bubble: ΔP = 4γ/r. Capillary rise: h = 2γ cos θ / (ρgr), where θ is contact angle, ρ is liquid density, g = 9.81 m/s², and r is tube radius.

Example Calculation

Result: ΔP = 145.6 Pa (1.09 mmHg)

A water droplet of radius 1 mm has ΔP = 2 × 0.0728 / 0.001 = 145.6 Pa. This is small relative to atmospheric pressure, but becomes significant for micrometer-sized droplets.

Tips & Best Practices

  • Remember that Laplace pressure increases as droplet radius decreases — this makes nanoparticles much harder to stabilize.
  • Surfactants reduce γ and hence reduce Laplace pressure, stabilizing emulsions and foams.
  • In the lungs, surfactant prevents small alveoli from collapsing into large ones (the Laplace instability).
  • For capillary rise calculations, use the inner radius of the tube, not the outer.
  • Temperature increases generally decrease surface tension (roughly −0.15 mN/(m·K) for water).
  • Critical capillary pressure for porous media scales as γ/r_pore — important in soil science and oil recovery.

Young-Laplace Equation in Different Geometries

For a **sphere** (droplet or gas bubble), R₁ = R₂ = r, giving ΔP = 2γ/r. For a **soap bubble**, the factor doubles to 4γ/r because of two air-liquid interfaces. For a **cylinder** (e.g., a liquid jet), one principal radius is r and the other is infinite, giving ΔP = γ/r. For a **saddle-shaped surface**, the two radii have opposite signs, potentially giving ΔP = 0.

Alveolar Mechanics

The lungs contain approximately 300 million alveoli with radii around 0.1-0.15 mm. Without pulmonary surfactant, the Laplace pressure in the smallest alveoli would be ~3 kPa, causing them to collapse. Surfactant reduces surface tension from ~70 mN/m to ~25 mN/m at end-expiration, preventing atelectasis. In premature infants, surfactant deficiency causes Respiratory Distress Syndrome (RDS).

Capillary Length

The capillary length κ⁻¹ = √(γ/(ρg)) defines the scale below which surface tension dominates gravity. For water, κ⁻¹ ≈ 2.7 mm. Droplets smaller than this are approximately spherical; larger ones flatten. This is why raindrops flatten but fog droplets are spherical.

Sources & Methodology

Last updated:

Frequently Asked Questions

  • Surface tension acts to minimize surface area, compressing the gas inside. The smaller the bubble, the higher the internal pressure — this is why small bubbles dissolve faster than large ones (Ostwald ripening).