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FLUID MECHANICS - Review

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1 FLUID MECHANICS - Review
Summary of (some) Fluids Concepts Learned in 3015C Properties of Interest: Density, ; Temperature, T; Pressure, p (All properties can be a function of space and time (x,y,z,t) VELOCITY - V (x,y,z,t) Probably the most important one from a fluid mechanics perspective. Viscosity – Dynamic Viscosity,  (N.sec/m2); Kinematic Viscosity,  (m2/sec) Pressure Behavior (for static conditions) Pascal’s law: for a fluid at rest, I.e. under static conditions pressure acts uniformly in all directions. It also always perpendicular to the surface. Pressure variation: For a continuous fluid at rest the pressure varies according to: dp/dz = - g where z is the vertical direction, opposite to gravity Rigid Body Motion The ratio of linear (or angular) acceleration to the gravitational acceleration, determines the shape of the free surface. Buoyancy: The buoyancy force on a submerged object is equal to the weight of the fluid displaced by the object. (Applies for fully or partially submerged objects of all shapes)

2 Summary of (some) Fluids Concepts Learned in 3015C (cont’d)
Boundary Layers: A region very close to solid surfaces where viscous effects are important A region very close to solid surfaces where velocity gradients are significant. Boundary layers can be Laminar or Turbulent Determined by the Reynolds Number Fundamental Equations of Motion: Conservation of Mass (continuity): Conservation of Momentum - If viscosity is neglected: Euler’s Equation OR

3 Summary of (some) Fluids Concepts Learned in 3015C (cont’d)
Conservation of Momentum - If viscosity is neglected: Euler’s Equation Integrate Euler’s equation along a streamline to obtain Bernoulli’s Equation It is only valid for : incompressible fluids, steady flow along a streamline, no energy loss due to friction, no heat transfer Conservation of Energy - If energy is added, removed or lost via pumps turbines, friction, etc.then we use the energy equation or Extended Bernoulli’s Equation: Flow work + kinetic energy + potential energy = constant Where hA , hE is work done by or on the systems, e.g turbines, pumps, etc. and hL is Frictional Head Loss where


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