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P. #3: An engineer conducted pool boiling experiments on a commonly used industrial copper substrate and obtained the followi

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Answer #1

P. #3:

Pool boiling curve:

In the pool boiling curve there are 4 phases with transition being excess temperature. They are,

  1. Natural/ Free convection boiling
  2. Nucleate boiling - (Unstable & Stable)
  3. Transition boiling
  4. Film boiling

1. Natural/ Free convection boiling:

  • In this case the liquid is being slightly overheated.
  • In this form of boiling the fluid motion is governed by natural currents of convection.
  • At around 7oC (at point 1 to A) excess temperature.

2. Nucleate boiling:

  • At an increasing number of nucleation sites, the bubbles shape at an rising pace as we pass along the boiling curve towards point C.
  • Unstable boiling is at beginning part of the nucleate boiling.
  • Then another component is available higher at steady boiling time.
  • The heat transfer coefficient varies from around 3000 to 30000 W/m2 K for the entire boiling range of the nucleates.
  • Region A-B: Isolated bubbles
  • Region B-C: Numerous continuous columns of vapour in the liquid.

3. Transition boiling:

  • The heat flux decreases as over temperature increases beyond point C.
  • That is because a vapor film covers a significant fraction of the heater surface, which serves as an insulation.
  • Nucleate and film boiling partly occur in the transition boiling regime.
  • In action activity in the boiling transition regime, also called the chaotic boiling film regime, is avoided.
  • The transition boiling occurs for copper substrate over the excess temperature from about 30oC to about 120oC.

4. Film boiling:

  • Beyond point D a continuous stable vapor film fully covers the heater flux sheet.
  • Point D, where the flux of heat reaches a peak, is called Leidenfrost.
  • The presence of vapor film between the surface of the heater and the liquid is responsible for the low levels of heat transfer in the boiling region.
  • The heat transfer rate increases due to radiation to the liquid, with an increase in excess temperature.
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