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Fluid Dynamics

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Darcy-Weisbach Equation

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An empirical equation that describes the pressure losses due to friction along a given length of pipe with a constant diameter, represented as

ΔP=fLD12ρv2 \Delta P = f \frac{L}{D} \frac{1}{2} \rho v^2
where ΔP\Delta P is the pressure loss, ff the Darcy friction factor, LL the pipe length, DD the pipe diameter, vv the flow velocity, and ρ\rho the fluid density.

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Mach Number

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A dimensionless quantity representing the ratio of the speed of an object moving through a fluid to the speed of sound in that fluid, defined as

Ma=vc Ma = \frac{v}{c}
where vv is object's velocity and cc is the speed of sound in the fluid.

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Turbulent Flow

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Type of fluid motion characterized by chaotic changes in pressure and flow velocity. It is associated with high momentum convection and eddy formation.

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Stream Function

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A mathematical function used to simplify the description of a two-dimensional, incompressible flow, where the function's value remains constant along streamlines and its partial derivatives are related to the velocity components.

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Bernoulli's Equation

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Describes the conservation of energy in a flowing fluid, represented as

P+12ρv2+ρgh=constant P + \frac{1}{2}\rho v^2 + \rho gh = \text{constant}
where PP is the fluid pressure, ρ\rho the density, vv the flow velocity, and hh the elevation.

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Laminar Flow

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Type of fluid motion in which all the particles in the fluid move along smooth, regular paths in layers or lamina, with minimal mixing and disruption between the layers.

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Continuity Equation

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Expresses the conservation of mass in fluid dynamics, often simplified for incompressible flow as

ρt+(ρv)=0 \frac{\partial \rho}{\partial t} + \nabla \cdot (\rho \mathbf{v}) = 0
or for steady, incompressible flow as A1v1=A2v2 A_1v_1 = A_2v_2 where AA is the cross-sectional area and vv is the flow velocity.

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Navier-Stokes Equations

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A set of nonlinear partial differential equations that describe the motion of fluid substances, represented as

ρ(vt+vv)=P+μ2v+f\rho \left( \frac{\partial \mathbf{v}}{\partial t} + \mathbf{v} \cdot \nabla \mathbf{v} \right) = -\nabla P + \mu \nabla^2 \mathbf{v} + \mathbf{f}
where v\mathbf{v} is the fluid velocity, PP the pressure, μ\mu the dynamic viscosity, and f\mathbf{f} represents body forces.

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Boundary Layer

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The layer of fluid in the immediate vicinity of a bounding surface where effects of viscosity are significant, generating a velocity gradient perpendicular to the flow direction.

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Reynolds Number

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Dimensionless quantity used to predict flow patterns in different fluid flow situations, represented as

Re=ρvLμ Re = \frac{\rho v L}{\mu}
where vv is the flow velocity, LL a characteristic length, ρ\rho the density, and μ\mu the dynamic viscosity of the fluid.

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