Fluid Mechanics & Hydraulics

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Presentation transcript:

Fluid Mechanics & Hydraulics Mr. Shiva Assistant Professor Department of Aeronautical Engineering By Shiva U

UNIT 4 Boundary Layer Theory & Pipe Flow Boundary layer - introductory concepts of boundary layer, large Reynolds number flows and Prandtl’s boundary layer hypothesis Pressure drag and skin friction drag; Pipe flow - Reynolds experiment, Darcy’s equation, major and minor losses in pipes and numerical problems. Flow between parallel plates, flow through long tubes –fully developed flow, Turbulent flow, variation of friction factor with Reynolds’s Number, Moody's chart.

The Boundary-Layer Concept Details of Viscous flow Around an Airfoil.

The Boundary-Layer Concept Boundary Layer on a flat Plate(Vertical thickness exaggerated greatly)

Boundary Layer Thicknesses Boundary-Layer thickness Definitions

Boundary Layer Characteristics Momentum boundary Layer over a flat plate: Laminar-to-Turbulent Transition

Boundary Layer Thicknesses Disturbance Thickness, d Displacement Thickness, d* Momentum Thickness, q

Displacement thickness y u There is a reduction in the flow rate due to the presence of the boundary layer U y u This is equivalent to having a theoretical boundary layer with zero flow d U

Pressure Gradients in Boundary-Layer Flow Boundary Layer flow with pressure gradient (Boundary layer thickness)

By Shiva U

By Shiva U

Methods of Preventing the Separation of Boundary Layer Suction of the slow moving fluid by a suction slot Supplying additional energy from the blower Providing a bypass in the slotted wing Rotating boundary in the direction of flow Providing small divergence in a diffuser Providing guide-blades in a bend Providing a trip-wire ring in the laminar region for the flow a sphere. By Shiva U

Lift force FL = ½ CLρAPv2 FL is lift force, CL is the coefficient of lift, ρ is fluid density, AP is the projected area of the body or surface area orientated perpendicular to the fluid flow, and v is relative velocity of the body with respect to the fluid. Note: The size, shape and orientation of the body (angle of attack) in the fluid are essential for generating lift force. The lift force increases with the square of the flow of velocity similar to drag force, but lift force increases are an advantage in sporting activities.

The lift/drag ratio The aim in sport is to maximize lift force while reducing drag force. The angle of attack of projected objects (a swimmer’s hand) is constantly changing throughout the flight path, and therefore, the lift/drag ratio changes as well.

Drag Drag Coefficient with or

Drag types Pure Friction Drag: Flat Plate Parallel to the Flow Pure Pressure Drag: Flat Plate Perpendicular to the Flow Friction and Pressure Drag: Flow over a Sphere and Cylinder Streamlining

Drag Flow over a Flat Plate Parallel to the Flow: Friction Drag Boundary Layer can be 100% laminar, partly laminar and partly turbulent, or essentially 100% turbulent; hence several different drag coefficients are available

Drag Flow over a Flat Plate Parallel to the Flow: Friction Drag (Continued) Laminar BL: Turbulent BL: … plus others for transitional flow

Drag Flow over a Flat Plate Perpendicular to the Flow: Pressure Drag Drag coefficients are usually obtained empirically

Drag Flow over a Flat Plate Perpendicular to the Flow: Pressure Drag (Continued)

Drag Flow over a Sphere and Cylinder: Friction and Pressure Drag

Drag Flow over a Sphere and Cylinder: Friction and Pressure Drag (Continued)

Streamlining(control of boundary layer separation) Used to Reduce Wake and hence Pressure Drag

Lift Mostly applies to Airfoils Note: Based on planform area Ap

Lift Examples: NACA 23015; NACA 662-215

Lift Induced Drag

Lift Induced Drag (Continued) Reduction in Effective Angle of Attack: Finite Wing Drag Coefficient:

Lift Induced Drag (Continued)

Robbins – Magnus effect When a spherical body (such as a ball) rotates as it moves through the air, it carries with it a boundary layer of air. The object will seek the path of least resistance, (the side of the ball that is rotating the same direction as the oncoming air). The effect is to cause the ball to curve in the direction of this low pressure air. Examples are tennis, golf, soccer, volleyball and football. These are top spin or backward spin (around horizontal axis). Spin right or left known as a hook or slice is around the vertical axis. Spin about the axis of the line of flight is called gyroscopic action and acts to stabilize the object as it moves through the air.

Robbins – Magnus effect

Case Study Case 1 Case 2

A flat plate 1.5m x 1.5m moves at 50 km/hr in stationary air of density 1.15kg/m3. If the coefficients of drag and lift are 0.15 and 0.75 respectively, determine i. Lift force ii. Drag force iii. The resultant force and iv. The power required to keep the plate in motion.

2. An aircraft model is mounted in a wind tunnel for drag determination. To decrease the drag contribution of the mounting system, the 1m long column is streamlined into an airfoil shape with a chord length of 10cm. At flow speed of 80m/s in the wind tunnel, estimate the error due to the drag on the mounting column, if the variation of CD of the streamlined column with Re given in table.

CD Vs Re for Mounting Column 3 x 10 5 0.0045 6 x 10 5 0.0055 1 x 10 6 0.0060 3 x 10 6 0.0065 CD = 0.072 ReL-1/5 – 1670/ReL

2. Find the displacement thickness, the momentum thickness and energy thickness for the velocity distribution in the boundary layer given by 𝑢 𝑈 = 𝑦 𝛿 , where u is the velocity at a distance y from the plate and u = U at y = 𝛿, where 𝛿 = boundary layer thickness. Also calculate the value of 𝛿∗/Ɵ.

Part II Pipe flow - Reynolds experiment, Darcy’s equation, major and minor losses in pipes and numerical problems. Flow between parallel plates, flow through long tubes –fully developed flow, Turbulent flow, variation of friction factor with Reynolds’s Number, Moody's chart. Note: For the above mentioned Topics Refer Notes

Thank You