Presentation is loading. Please wait.

Presentation is loading. Please wait.

Internal Incompressible

Similar presentations


Presentation on theme: "Internal Incompressible"— Presentation transcript:

1 Internal Incompressible
Introduction to Fluid Mechanics Chapter 8 Internal Incompressible Viscous Flow © Pritchard

2 Main Topics Entrance Region Fully Developed Laminar Flow 
Between Infinite Parallel Plates Fully Developed Laminar Flow in a Pipe Turbulent Velocity Profiles in Fully Developed Pipe Flow Energy Considerations in Pipe Flow Calculation of Head Loss Solution of Pipe Flow Problems Flow Measurement © Pritchard

3 Entrance Region © Pritchard

4 Daerah berkembangnya profil kecepatan dari linier di hulu menjadi parabolik disebut entrance region, sedangkan daerah dengan profik kecepatan berbentuk parabolik disebut fully developed region.

5 Fully Developed Laminar Flow Between Infinite Parallel Plates
Both Plates Stationary © Pritchard

6 Problems 8.1 Standar air enters a 150 mm diameter duct. Find the volume flow rate at which the flow becomes turbulent. At this flow rate, estimate the entrance length required to establish fully developed flow

7 Fully Developed Laminar Flow Between Infinite Parallel Plates
 Both Plates Stationary Plates Transformation of Coordinates © Pritchard

8 Fully Developed Laminar Flow Between Infinite Parallel Plates
 Both Plates Stationary Plates Shear Stress Distribution Volume Flow Rate © Pritchard

9 Fully Developed Laminar Flow Between Infinite Parallel Plates
 Both Plates Stationary Flow Rate as a Function of Pressure Drop Average and Maximum Velocities © Pritchard

10 Fully Developed Laminar Flow
Between Infinite Parallel Plates  Upper Plate Moving with Constant Speed, U © Pritchard

11 Problems 8.9 Viscous oil flow steadily between parallel plates. The flow is fully developed and laminar. The pressure gradient is 1,25 kPa/m and the channel half-width is h = 1,5 mm. Calculate the magnitude and direction of the wall shear stress at the upper plate surface. Find the volume flow rate through the channel (μ = 0,50 Ns/m²)

12 Problems 8.23 Two immiscible fluids are contained between infinite parallel plates. The plates are separated by distance 2h, and the two fluid layers are of equal thickness h; the dynamic viscosity of the upper fluid is three times that of the lower fluid. If the lower plate is stationary and the upper plate moves at constant speed U = 6,1 m/s, what is the velocity at the interface? Assume laminar flows, and that the pressure gradient in the direction of flow is zero.

13 Fully Developed Laminar in a Pipe Flow
Velocity Distribution Flow Shear Stress Distribution Pritchard

14 Fully Developed Laminar Flow in a Pipe Rate Volume Flow Flow Rate as
Function of Pressure Drop © Pritchard

15 Fully Developed Laminar in a Pipe Flow
Average Velocity Flow Maximum Velocity Pritchard

16 Turbulent Velocity Profiles in Fully Developed Pipe Flow
© Pritchard

17 Turbulent Velocity Profiles in Fully Developed Pipe Flow
© Pritchard

18 Problems 8.47 A hypodermic needle, with inside diameter d = 0,127 mm and length L = 25 mm, is used to inject saline solution with viscosity five times that of water. The plunger diameter is D = 10 mm; the maximum force that can be exerted by a thumb on the plunger is F = 33,4 N. Estimate the volume flow rate of saline that can be produced.

19 Calculation of Head Loss Major Losses: Friction Factor © Pritchard

20 Calculation of Head Loss Factor Laminar Friction Turbulent Friction
© Pritchard

21 Calculation of Head Loss © Pritchard

22 Calculation of Head Loss
 Minor Losses Examples: Inlets and Exits; Enlargements and Contractions; Pipe Bends; Valves and Fittings © Pritchard

23 Le Calculation of Head Loss Minor Loss: Loss Coefficient, K Minor
Equivalent Length, Le © Pritchard

24 Calculation of Head Loss Pumps, Fans, and Blowers © Pritchard

25 Calculation of Head Loss Noncircular Ducts Example: Rectangular Duct
© Pritchard

26 Solution of Pipe Flow Problems Energy Equation © Pritchard

27 Solution of Pipe Flow Problems Major Losses © Pritchard

28 Solution of Pipe Flow Problems Minor Losses © Pritchard

29 Problems 8.73 Water flows from a horizontal tube into a large tank. The tube is located 2.5 m below the free surface of water in the tank. The head loss is 2 J/kg. Compute the average flow speed in the tube.

30 Problems 8.84 Water flows through a 25 mm diameter tube that suddenly enlarges to a diameter of 50 mm. the flow rate through the enlargement is 1,25 Liter/s. Calculate the pressure rise across the enlargement. Compare with the value for frictionless flow.

31 Flow Measurement  Direct Methods
Examples: Accumulation in a Container; Positive Displacement Flow meter  Restriction Flow Meters for Internal Flows Examples: Orifice Plate; Flow Nozzle; Venturi; Laminar Flow Element Pritchard

32 Flow Measurement  Linear Flow Meters •
Examples: Float Meter (Rotameter); Turbine; Ultrasonic Vortex; Electromagnetic; Magnetic; Pritchard

33 Flow Measurement  Traversing Methods • Examples: Pitot (or Pitot
Static) Tube; Laser Doppler Anemometer © Pritchard

34 Problems 8.173 A venture meter with a 762 mm diameter throat is place in a 152 mm diameter line carrying water at 24˚C. The pressure drop between the upstream tap and the venture throat is 305 mm of mercury. Compute the rate of flow.


Download ppt "Internal Incompressible"

Similar presentations


Ads by Google