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In physics, the Young–Laplace equation (/ləˈplɑːs/) is an equation that describes the capillary pressure difference sustained across the interface between

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steady current density Young–Laplace equation, in physics, describing pressure difference over an interface in fluid mechanics Laplace expansion, in linear

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Pierre-Simon, Marquis de Laplace (/ləˈplɑːs/; French: [pjɛʁ simɔ̃ laplas]; 23 March 1749 – 5 March 1827) was a French polymath, a scholar whose work has

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and gas, or between two immiscible liquids. The Laplace pressure is determined from the Young–Laplace equation given as Δ P ≡ P inside − P outside = γ

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mathematician, unified the work of these two scientists to derive the Young–Laplace equation, the formula that describes the capillary pressure difference

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developed within a liquid droplet/film can be calculated using the Young–Laplace equation (e.g.): Δ p = − γ ∇ ⋅ n ^ = γ ( 1 R 1 + 1 R 2 ) {\displaystyle

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Young's equation may refer to: Young–Laplace equation, describes the capillary pressure difference sustained across the interface between two static fluids

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all the forces are balanced, the resulting equation is known as the Young–Laplace equation: Δ p = γ ( 1 R x + 1 R y ) {\displaystyle \Delta p=\gamma \left({\frac

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movement. In contrast, the equilibrium contact angle described by the Young-Laplace equation is measured from a static state. Static measurements yield

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force up and force down relationship of two fluids in equilibrium. The Young–Laplace equation is the force up description of capillary pressure, and the

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