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A
A
Constant heat
flux boundary
A - A
Adiabatic
H
W
Experiment Purpose Dh = 1mm simple plane channel
without plenum (Requirement)
• Velocity, v = 0.1 m/s (Re = 100) to 1 m/s (Re = 1000)
• Flow rate, 10^-7 (Re = 100) to 10^-6 (Re = 1000) (m^3/s)
• Heat flux at bottom alone Q/A = up to 100 kW/m^2
To find from experiment
• Pressure drop - pumping power
• Temperature fluid and wall (different
locations) – heat transfer coefficient
• Flow visualization
2. Other possibilities – After completion of simple plane channel (images for understanding)
Tapered microchannel wavy/serpentine microchannel
(increasing/ decreasing wavelength & amplitude)
Convergent/divergent (changing the throat area)
Fixing constant surface-to- volume ratio (changing cross-section of
microchannel square, rectangular, trapezoidal, rombus etc,.)
If possible providing microstructures in the channel
(fins, ribs, protrusions etc,.)
Parallel / counter flow arrangements
(single inlet & outlet / multiple inlets &outlets)

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Microchannel.pptx

  • 1. A A Constant heat flux boundary A - A Adiabatic H W Experiment Purpose Dh = 1mm simple plane channel without plenum (Requirement) • Velocity, v = 0.1 m/s (Re = 100) to 1 m/s (Re = 1000) • Flow rate, 10^-7 (Re = 100) to 10^-6 (Re = 1000) (m^3/s) • Heat flux at bottom alone Q/A = up to 100 kW/m^2 To find from experiment • Pressure drop - pumping power • Temperature fluid and wall (different locations) – heat transfer coefficient • Flow visualization
  • 2. 2. Other possibilities – After completion of simple plane channel (images for understanding) Tapered microchannel wavy/serpentine microchannel (increasing/ decreasing wavelength & amplitude) Convergent/divergent (changing the throat area) Fixing constant surface-to- volume ratio (changing cross-section of microchannel square, rectangular, trapezoidal, rombus etc,.)
  • 3. If possible providing microstructures in the channel (fins, ribs, protrusions etc,.) Parallel / counter flow arrangements (single inlet & outlet / multiple inlets &outlets)