Quick Recap

The instructor outlined the upcoming class topics on convection heat transfer, including both without and with phase change, and announced practice questions would be released for the test. The discussion covered technical calculations related to Nusselt numbers, velocity determination, and heat transfer coefficients, with emphasis on practical applications and experimental conditions. The session concluded with discussions on boiling types and characteristics, along with administrative announcements about upcoming classes and course feedback.

Next Steps

  • Students to spend at least 1 hour daily studying the course material.
  • MSubbu to release questions for conduction, condensation, convection, and heat exchangers by tomorrow.
  • MSubbu to cover radiation and evaporation in the next class.
  • MSubbu to cover conceptual questions in the last class.
  • Students to review related theory before and after each class.
  • MSubbu to finish heat transfer topics and start mass transfer next week.
  • Students to provide feedback on the course-materials and classes.

SUMMARY

Convection Heat Transfer Class Overview

MSubbu outlines the topics for the upcoming class on convection heat transfer. He explains that the focus will be on convection without phase change and with phase change (condensation and boiling). MSubbu mentions that he will release practice questions for the test by the next day, covering conduction, condensation, convection, and heat exchangers. He also announces that the next class will cover radiation and evaporation, followed by a final class on conceptual questions. MSubbu encourages participation in the peer discussion on Saturday.

Nusselt Number Calculation Techniques

The discussion focuses on calculating the Nusselt number from a given temperature profile near a solid boundary. MSubbu explains that the Nusselt number can be derived by equating convection and conduction equations near the wall. He demonstrates how to use the temperature gradient near the wall to calculate the heat transfer coefficient and subsequently the Nusselt number. MSubbu also mentions two common experimental conditions: uniform wall heat flux and uniform wall temperature, providing the corresponding Nusselt numbers for laminar flow in pipes (4.36 and 3.66 respectively). He then discusses how to determine when flow becomes fully thermally developed based on temperature data along a pipe's length.

Heat and Momentum Transfer Analogy

The instructor explains how to calculate velocity using pressure drop data and the Darcy friction factor. He then discusses the Chilton-Colburn analogy and its application in heat and mass transfer calculations. 

The instructor expresses concern about students' lack of engagement and urges them to spend at least an hour daily studying the course material. He emphasizes the importance of regular, consistent study habits rather than accumulating work.

Heat Transfer Principles and Convection

MSubbu explains the principles of heat transfer through conduction and convection in different setups. He describes how the arrangement of hot and cold plates affects the heat flux, with setups promoting natural convection having higher heat transfer rates than those with only conduction. MSubbu clarifies that when the hot plate is at the bottom, it creates favorable conditions for convection, while a hot plate at the top suppresses it. He also notes that the heat flux is higher at higher average temperatures due to greater density differences in the fluid.

Prandtl Number and Boundary Layers

The instructor discusses the Prandtl number and its relationship to boundary layer thickness for different types of fluids. For liquid metals, the Prandtl number is less than one, resulting in a thicker thermal boundary layer compared to the momentum boundary layer. Gases have a Prandtl number of approximately one, while liquids generally have a Prandtl number greater than one. The instructor also briefly mentions condensation, comparing dropwise and filmwise condensation, with dropwise condensation offering higher heat transfer coefficients.

Condensation Heat Transfer Relationships

The discussion focuses on heat transfer coefficients in condensation processes. MSubbu explains that the local heat transfer coefficient is inversely proportional to the distance from the leading edge, and the average heat transfer coefficient is 4/3 of the local value at a given location. He also discusses the relationship between mass flow rate, condensate thickness, and distance, noting that the condensate thickness grows proportionally to the distance raised to the power of 1/4. MSubbu advises memorizing these key relationships to solve condensation problems efficiently.

Boiling Mechanisms and Heat Transfer

MSubbu discusses the types and characteristics of boiling, focusing on pool boiling and flow boiling. He explains the different regions of the boiling curve, including natural convection, nucleate boiling, transition boiling, and film boiling. MSubbu emphasizes that the optimal operating region for boiling devices is near the critical heat flux point, within the nucleate boiling region. He also mentions the importance of surface roughness in creating nucleation sites for boiling and briefly touches on analogies used in heat transfer, such as Reynolds Analogy and Chilton-Colburn Analogy.

Course Updates

MSubbu encourages students to watch available videos before class and to provide feedback on the course. He announces upcoming classes, including a finishing class for Heat Transfer and the start of Mass Transfer next week. MSubbu also reminds students to attend discussion sessions and thanks those who are participating.

Last modified: Wednesday, 25 June 2025, 10:51 AM