Fluidic and Microfluidic Pumps, Micropumps, Compressors, Fans and Blowers an Overview

1. Fluidic and Microfluidic Pumps, Micropumps, Compressors, Fans and Blowers an Overview

2. Pumps, Fans, Compressors and Blowers Increase Fluid Energy • Velocity – Kinetic Energy a) Fans b) Propulsion Propellers • Pressure – Internal Energy – Enthalpy - Heat a) Pumps b) Compressors • Velocity and Pressure – Some of Both a) Pumps • Blowers

3. Types of Pumps, Fans, Compressors and Blowers

4. Types of Pumps, Fans, Compressors and Blowers

5. Types of Pumps, Fans, Compressors and Blowers

6. Pump Performance Trade offs

7. Fluidic System Pressure vs. Flow Curve Determines the type of Pump Needed

8. Typical Pump Operating Curves

9. Typical Pump Operating Curves

10. Fan and Blower Geometries

11. Pump Type Efficiencies

12. Some General Pump Theory

13. BERNOULLI’S THEOREM • The Bernoulli equation is a special statement of the general energy equation • Work added to the system is referred to as pump head (hP) • Losses from the system are referred to as head loss (hL) • Pressure (lbf/in2) is a form of work • Strictly Mechanical Energy so we get the equation: P1 + PE1 + KE1 + WK = PE2 + KE2 + WKFRIC + P2

14. BERNOULLI’S Equation Z1 + (P1/) + (V12/2g) = Z2 + (P2/) + (V22/2g) + hP - hL Z : Elevation (ft) P : Pressure (lb/ft2)  : Density (lb/ft3) V : Velocity (ft/sec) g : acceleration (32.2 ft/sec2) Hp: pump head (ft) HL: Head Loss (ft) = f(L/D)(V2/2Zg) where f : friction factor L: Length D: Diameter

15. Fluidic Design Equations – Bernoulli Again

16. THE CONCEPT OF “HEAD” • The vertical difference between 2 levels of liquid • Use FT to measure the pressure exerted by a body of liquid in term of weight • Head α Pressure α Energy • Velocity Head • The distance a liquid would have to fall for a given V • Hv = V12/2g • Friction Head • Hl= f(L/D)(V2/2Zg) where • f : friction factor • L: Length • D: Diameter

17. Pressure Head STATIC DISCHARGE HEAD NET STATIC HEAD STATIC SUCTION PRESSURE PUMP

18. Velocity Head • Head required to impart velocity to a liquid • Equivalent to the vertical distance through which the liquid would have to fall to acquire the same velocity • Equal to V2 / 2g

19. Friction Head • The force or pressure required to overcome friction is obtained at the expense of the static pressure head • Unlike velocity head, friction head cannot be “recovered” or reconverted to static pressure head • Thermal energy is usually wasted, therefore resulting in a head loss from the system

20. Centrifugal Pump Scaling “Laws”

21. More Pump “Laws” Apply to centrifugal (non-positive displacement) pumps only V  N Hp N2 W  N3 V = volumetric flow rate N = speed of rotation Hp = pump head W = power required (prime mover) . . .

22. Pump Design Equation – Bernoulli Again

23. Anatomy of Several Pump Types

24. Centrifugal and Fan Pump Elements DRIVE TYPE (electric motor, steam drive, gear driven, etc…) IMPELLER PUMP SHAFT & Seal DISCHARGE CASING SUCTION

25. Centrifugal Pump Elements

26. Centrifugal and Fan Pump Elements

27. Centrifugal and Fan Pump Elements

28. Centrifugal Pump Elements

29. “Roots” Blower

30. Gerotor Pump

31. Vane Pump

32. Small Silicon Micro-Compressor Design Concept

33. MEMS Magnetically Actuated Micropump

34. Single and double Acting Piston Pumps

35. Archimedes Screw Pump

36. Multiple Screw Pump

37. Conical Drag Pump

38. Tesla “Drag” Pump

39. Drag or Pos. Displacement “Screw” Pump

40. Small Spiral “Viscous Drag” Pump

41. Examples of Small Commercially Available and “Academic Research” Pumps Fans and Blowers

42. Typical “Micro-Blower”

43. Typical Double Fan Blower

44. Typical Fan based “Micro-Blower”

45. Small Sunon Blower

46. Small Sunon Blower - Continued

47. High Volume - Low Pressure - Centrifugal Blower

48. Micro-Vacuum Products

49. Small Blower – Mesoscopics, Inc.

50. Small Blower – Mesoscopics, Inc.