5. Consider the following diagram from one of the lecture slides: 111 Hot fluid Ta Cold fuid T F I Heat tanster trough a plane wall (4) Temperate distribution. () Equivalent themal circut Focus on temperature distribution from T,1 to Ts,1- which represents convective heat transfer from hot fluid to solid surface at x=0. Clearly, this distribution is nonlinear in nature (and it corresponds to boundary layer of the fluid). (a) Even though this is a nonlinear function, why we could use electrical circuit analogy for this situation i.e. heat convection from hot fluid to solid surface at x=0? (b) Heat conduction on the other hand, explicitly requires linear temperature distribution (see distribution from x-0 to x=L in solid) for electrical analogy to be used in the problem, why is that?

Introduction to Chemical Engineering Thermodynamics
8th Edition
ISBN:9781259696527
Author:J.M. Smith Termodinamica en ingenieria quimica, Hendrick C Van Ness, Michael Abbott, Mark Swihart
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Chapter1: Introduction
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# Understanding Heat Transfer: Analyzing Temperature Distribution

## Diagram Explanation

The diagram illustrates heat transfer through a plane wall and consists of two main parts:

1. **Temperature Distribution:**
   - Represents the flow of heat from a hot fluid with temperature \( T_{\infty,1} \) on one side to a cold fluid with temperature \( T_{\infty,2} \) on the other side.
   - Heat transfer occurs convectively from the hot fluid to the solid surface at \( x = 0 \), then through the solid, and finally to the cold fluid.
   - The red curve shows a nonlinear temperature profile within the solid, indicating the boundary layer effects on the fluid side.

2. **Equivalent Thermal Circuit:**
   - A thermal resistance circuit diagram is shown below the temperature profile.
   - Consists of resistances representing convective and conductive heat transfer: 
     - \( R_{conv,1} \) for convective resistance at the hot fluid side.
     - \( R_{cond} \) for conductive resistance through the solid medium.
     - \( R_{conv,2} \) for convective resistance at the cold fluid side.

## Focus Areas

- **Temperature Distribution from \( T_{\infty,1} \) to \( T_{s,1} \):**
  - Highlights convection from hot fluid to the solid surface at \( x = 0 \).
  - The distribution is nonlinear, reflecting the boundary layer influence of the fluid.

- **Discussion Points:**
  - **(a)** While the function is nonlinear, we can still use electrical circuit analogies to model heat convection at \( x = 0 \) because the principles governing flow (Ohm’s Law and Fourier’s Law of Heat Conduction) are analogous.
  - **(b)** On the other hand, heat conduction in the solid requires a linear temperature distribution (from \( x = 0 \) to \( x = L \)), which aligns with steady-state assumptions and allows reliable use of electrical circuit analogies. The reasons for this relate to the direct proportionality between temperature difference and heat flow within the solid, typical of linear systems.
Transcribed Image Text:# Understanding Heat Transfer: Analyzing Temperature Distribution ## Diagram Explanation The diagram illustrates heat transfer through a plane wall and consists of two main parts: 1. **Temperature Distribution:** - Represents the flow of heat from a hot fluid with temperature \( T_{\infty,1} \) on one side to a cold fluid with temperature \( T_{\infty,2} \) on the other side. - Heat transfer occurs convectively from the hot fluid to the solid surface at \( x = 0 \), then through the solid, and finally to the cold fluid. - The red curve shows a nonlinear temperature profile within the solid, indicating the boundary layer effects on the fluid side. 2. **Equivalent Thermal Circuit:** - A thermal resistance circuit diagram is shown below the temperature profile. - Consists of resistances representing convective and conductive heat transfer: - \( R_{conv,1} \) for convective resistance at the hot fluid side. - \( R_{cond} \) for conductive resistance through the solid medium. - \( R_{conv,2} \) for convective resistance at the cold fluid side. ## Focus Areas - **Temperature Distribution from \( T_{\infty,1} \) to \( T_{s,1} \):** - Highlights convection from hot fluid to the solid surface at \( x = 0 \). - The distribution is nonlinear, reflecting the boundary layer influence of the fluid. - **Discussion Points:** - **(a)** While the function is nonlinear, we can still use electrical circuit analogies to model heat convection at \( x = 0 \) because the principles governing flow (Ohm’s Law and Fourier’s Law of Heat Conduction) are analogous. - **(b)** On the other hand, heat conduction in the solid requires a linear temperature distribution (from \( x = 0 \) to \( x = L \)), which aligns with steady-state assumptions and allows reliable use of electrical circuit analogies. The reasons for this relate to the direct proportionality between temperature difference and heat flow within the solid, typical of linear systems.
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