Part of JME-09 — Fluid Mechanics: Pascal, Bernoulli & Viscosity

Bernoulli's Theorem and Applications

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Bernoulli's theorem is conservation of energy for ideal fluid flow: P+12ρv2+ρgh=constantP + \frac{1}{2}\rho v^2 + \rho gh = \text{constant} along a streamline. The three terms represent pressure energy, kinetic energy, and potential energy per unit volume. Assumptions: ideal fluid (incompressible, non-viscous), steady flow, along a streamline.

Combined with the equation of continuity (A1v1=A2v2A_1 v_1 = A_2 v_2), Bernoulli explains many phenomena. The Venturi effect: at a constriction, velocity increases and pressure decreases. This is the principle behind Venturi meters (flow measurement), atomizers (sprayers), and carburetors.

Torricelli's theorem (v=2ghv = \sqrt{2gh}) gives the speed of efflux from a hole at depth hh. The exiting stream follows projectile motion with horizontal range R=2h(Hh)R = 2\sqrt{h(H-h)}, maximized when the hole is at mid-height (h=H/2h = H/2, Rmax=HR_{\max} = H). Time to empty a tank requires integration: t=(A/a)2H/gt = (A/a)\sqrt{2H/g}.

Aerodynamic lift on wings arises from faster airflow over the curved top surface (lower pressure) versus the flatter bottom (higher pressure). The Magnus effect explains why spinning balls curve — asymmetric airflow creates a lateral pressure difference.

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