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MEMS-BASED
MEMS BASED FLUID
  FLOW SENSOR



         by Jean P. Cortes
                 P
MEMS?
MEMS: Micro Electro Mechanical Systems


 MEGR                         Mathematics


               MEMS            Biology
 ECGR


Physics
  y                           Chemistry



               Micro motor.
MEMS?
   A)




  B)                                      C)




A) Micro gears, B) Micro pump, C) micro
wind blades.
Objectives
Design and evaluate a MEMS sensor with
capabilities in measuring parameters,
such as:


  • Fluid Flow rates
  • Velocity/direction
  • Pressure


based on thermal convection
                 convection.
Heat transfer
    Conduction
    within the same material
    Convection
    Through a medium (depends on the
    interaction with the medium)
    Radiation
    Every material radiates energy.
  On the device:
    less conduction
    dependence on convection
    high thermal conductivity fast response
Flow measurement
Thermal fl
Th      l flow sensors b
                       based on H t i
                           d    Hotwire
principles:
1) heat is produced (Joule’s effect)
2) heat is transferred by convection
3) ΔT is α to the flow rate.


             I2 Rw = h Aw (Tw – Tf)
Hotwire principle


 A)                                       B)

      Flow




              HEATER




A) Hotwire: flow rate depends on the loss of heat at the heater
B) Hotwire anemometry: flow rates and direction can be
   measured.
          d
             For flow measurement one or three elements can be used.
Example of MAF in a car




  Schematic representation of the Hotwire anemometry.
Analytical analysis
  Thin film
  Thi fil resistor powered by a constant
              it           db           tt
 current source is introduced in fluid medium.
  In thermal equilibrium with it ambient, th
  I th     l    ilib i    ith its  bi t then
                   I2 Rw = h Aw (Tw – Tf)
  The film resistance is:
               Rw= Rref [1 + TCR (Tw-Tref)]

 * for optimal operations TCR must be high.

       Rate: the heat transfer coefficient h is a function of
       fluid velocity vf according to King’s law
Analytical analysis




     * a, b, and c are calibration constants to be found empirically…


     Direction: the heat is removed form the heater and
     transfer to the detectors This calculations are
                     detectors.
     going to be obtained empirically.
Pressure measurement
Pressure sensors based on Hotwires
1) heat is produced ( p = Iw2 Rw )
2) heat is kept constant
3) h
 ) heat transfer due to I
             fd         Impingement rate:
                           i




4) The Tw increases as P goes down
Pressure measurement


                               Vacuum 
                               Chamber




                                                      Heater
                              Gas 
                              Molecules                        Pumping



  Schematic representation of the application to measure pressure.
        For pressure measurement one element is needed.
Design
                  100 μm
                                         Top view                        100 μm

                                                                                  100 μm
                                                                                      μ




 Heater (W)
 2 detectors (Ni/Pt)
        TCR = 3900 ppm/oC
                                                                          500 μm
 SiC support
       Metal
                           0.5 μm
                           10 μm
SiC

       500 μm              300 μm
                                                        500 μm
                                    Design of the three resistor for flow measurement.
      Side view       Si
Design
                                            Top view                 100 μm
                150 μm

                                                                              100 μm
                                                                                  μ
                         50 μm



 Heater (W)
 2 detectors (Ni/Pt)
        TCR = 3900 ppm/oC
                                                                              500 μm
 SiC support

       Metal
       Mtl
                              0.5 μm
                              10 μm
SiC

       500 μm                 300 μm
                                                          500 μm
                                       Design of the one resistor for vacuum measurement.
      Side view          Si
Why SiC?
  Can withstand harsh environments (chemical
inert, very high temperatures T > 1500 oC)

 High thermal conductivity (3.2- 4.9 W/cm K)
 Hardness and wear resistance high Young’s
                     resistance,      Young s
modulus, very low thermal coefficient of
expansion
 High resistance (102 to104 Ω-cm).
  The Challenge:
• SiC is expensive
• Develop a way to fabricate SiC at low cost
Fabrication of SiC
Equipment:
  Power source
  Solution
  Teflon cell (2 beakers)                     cathode

  Container                                          V

  Two electrodes (Pt)
                                             anode
                            • Si is inexpensive
                            • Can be used for electronic
                            circuits
                            • Porous Si can
                            accommodate the large
                            strain between Si and SiC
Fabrication of SiC
Low pressure chemical vapor deposition chamber.




                                                  Inside




                                                  Top view
Project Plan – Fall 08
Project Plan – Spring 09
Cost
                      Total Cost for making HOT-MEMS

                   Total Tooling Total Labor                    Manufacturing
   Operation                                           Cost
                       cost                                      Cost/Wafer
                                    cost
Cleaning                    $21.00             $2.50   $23.50             $0.94
Oxidation                   $23.00             $2.50   $25.50             $0.51
Metal Deposition          $260.00              $2.50 $262.50            $17.50

Mask creation               $25.00            $50.00   $75.00             $3.74
Photolithography            $25.80             $5.00   $30.80           $30.80

Metal Etch                   $4.20             $2.50    $6.70             $6.70
Dicing                      $10.50             $5.00   $15.60           $15.50
Total                     $369.50             $70.00 $439.60           *$75.69


                 18000 devices…….so the final price is ~ $      0.00456
   •6 in wafer
Applications - flow
Aerospace, velocity measurements at various
A              l it           tt       i
ranges of interest
Medical, respirators for pre-matured born, and
diagnostics of asthmatic attacks

Automotive industry,
Education, educational training of students on
fluid related experiments,
Semiconductor industry, for almost every
process where vacuum is involved
Summary
o W have designed a sensor suitable f
  We h     di      d         it bl for
  both: flow and vacuum measurement.
o We have started the process of
  fabricating SiC using porous silicon as
  template.
o Low cost process promises mass
   ow ost pro ess
  production of the device.
o High thermal conductivity of silicon
  carbide improves the detector’s
  response.
  response
Acknowledgments
Dr. Mohamed-Ali H
D Mh      d Ali Hasan ( d i
                      (advisor)
                              )
Dr. Asghar Hashmi
Dr. R. Gary Wilson
Dr. Stuart Smith
Payam Shoghi
Namit Singh
Ayman Zhobi
Tanya Dias
Dr. Horacio Estrada
Sr#1 Jp Cortes

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Sr#1 Jp Cortes

  • 1. MEMS-BASED MEMS BASED FLUID FLOW SENSOR by Jean P. Cortes P
  • 2. MEMS? MEMS: Micro Electro Mechanical Systems MEGR Mathematics MEMS Biology ECGR Physics y Chemistry Micro motor.
  • 3. MEMS? A) B) C) A) Micro gears, B) Micro pump, C) micro wind blades.
  • 4. Objectives Design and evaluate a MEMS sensor with capabilities in measuring parameters, such as: • Fluid Flow rates • Velocity/direction • Pressure based on thermal convection convection.
  • 5. Heat transfer Conduction within the same material Convection Through a medium (depends on the interaction with the medium) Radiation Every material radiates energy. On the device: less conduction dependence on convection high thermal conductivity fast response
  • 6. Flow measurement Thermal fl Th l flow sensors b based on H t i d Hotwire principles: 1) heat is produced (Joule’s effect) 2) heat is transferred by convection 3) ΔT is α to the flow rate. I2 Rw = h Aw (Tw – Tf)
  • 7. Hotwire principle A) B) Flow HEATER A) Hotwire: flow rate depends on the loss of heat at the heater B) Hotwire anemometry: flow rates and direction can be measured. d For flow measurement one or three elements can be used.
  • 8. Example of MAF in a car Schematic representation of the Hotwire anemometry.
  • 9. Analytical analysis Thin film Thi fil resistor powered by a constant it db tt current source is introduced in fluid medium. In thermal equilibrium with it ambient, th I th l ilib i ith its bi t then I2 Rw = h Aw (Tw – Tf) The film resistance is: Rw= Rref [1 + TCR (Tw-Tref)] * for optimal operations TCR must be high. Rate: the heat transfer coefficient h is a function of fluid velocity vf according to King’s law
  • 10. Analytical analysis * a, b, and c are calibration constants to be found empirically… Direction: the heat is removed form the heater and transfer to the detectors This calculations are detectors. going to be obtained empirically.
  • 11. Pressure measurement Pressure sensors based on Hotwires 1) heat is produced ( p = Iw2 Rw ) 2) heat is kept constant 3) h ) heat transfer due to I fd Impingement rate: i 4) The Tw increases as P goes down
  • 12. Pressure measurement Vacuum  Chamber Heater Gas  Molecules Pumping Schematic representation of the application to measure pressure. For pressure measurement one element is needed.
  • 13. Design 100 μm Top view 100 μm 100 μm μ Heater (W) 2 detectors (Ni/Pt) TCR = 3900 ppm/oC 500 μm SiC support Metal 0.5 μm 10 μm SiC 500 μm 300 μm 500 μm Design of the three resistor for flow measurement. Side view Si
  • 14. Design Top view 100 μm 150 μm 100 μm μ 50 μm Heater (W) 2 detectors (Ni/Pt) TCR = 3900 ppm/oC 500 μm SiC support Metal Mtl 0.5 μm 10 μm SiC 500 μm 300 μm 500 μm Design of the one resistor for vacuum measurement. Side view Si
  • 15. Why SiC? Can withstand harsh environments (chemical inert, very high temperatures T > 1500 oC) High thermal conductivity (3.2- 4.9 W/cm K) Hardness and wear resistance high Young’s resistance, Young s modulus, very low thermal coefficient of expansion High resistance (102 to104 Ω-cm). The Challenge: • SiC is expensive • Develop a way to fabricate SiC at low cost
  • 16. Fabrication of SiC Equipment: Power source Solution Teflon cell (2 beakers) cathode Container V Two electrodes (Pt) anode • Si is inexpensive • Can be used for electronic circuits • Porous Si can accommodate the large strain between Si and SiC
  • 17. Fabrication of SiC Low pressure chemical vapor deposition chamber. Inside Top view
  • 18. Project Plan – Fall 08
  • 19. Project Plan – Spring 09
  • 20. Cost Total Cost for making HOT-MEMS Total Tooling Total Labor Manufacturing Operation Cost cost Cost/Wafer cost Cleaning $21.00 $2.50 $23.50 $0.94 Oxidation $23.00 $2.50 $25.50 $0.51 Metal Deposition $260.00 $2.50 $262.50 $17.50 Mask creation $25.00 $50.00 $75.00 $3.74 Photolithography $25.80 $5.00 $30.80 $30.80 Metal Etch $4.20 $2.50 $6.70 $6.70 Dicing $10.50 $5.00 $15.60 $15.50 Total $369.50 $70.00 $439.60 *$75.69 18000 devices…….so the final price is ~ $ 0.00456 •6 in wafer
  • 21. Applications - flow Aerospace, velocity measurements at various A l it tt i ranges of interest Medical, respirators for pre-matured born, and diagnostics of asthmatic attacks Automotive industry, Education, educational training of students on fluid related experiments, Semiconductor industry, for almost every process where vacuum is involved
  • 22. Summary o W have designed a sensor suitable f We h di d it bl for both: flow and vacuum measurement. o We have started the process of fabricating SiC using porous silicon as template. o Low cost process promises mass ow ost pro ess production of the device. o High thermal conductivity of silicon carbide improves the detector’s response. response
  • 23. Acknowledgments Dr. Mohamed-Ali H D Mh d Ali Hasan ( d i (advisor) ) Dr. Asghar Hashmi Dr. R. Gary Wilson Dr. Stuart Smith Payam Shoghi Namit Singh Ayman Zhobi Tanya Dias Dr. Horacio Estrada