Heat transfer

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Transcript Heat transfer

Heat Transfer: Overview of Heat Transfer Analysis

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Objectives

Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 2  Understand the basics of heat transfer analysis.

 Study Conduction, Convection and Radiation modes of heat transfer.

 Identify the considerations required for solving heat transfer problems.

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Overview of Heat Transfer Analysis

Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 3

Heat – energy produced as a result of combustion, chemical reaction,

electrical resistance, friction, fission, fusion, incident solar radiation, microwaves, etc .

Heat transfer – the exchange of heat from one body to another, the

study of which is applicable across a broad range of applications.

Common heat transfer problems include the calculation of heat loss/gain :      Through windows In electronic chips Through pipes carrying steam Through fins on a radiator And many more… The Sun is by far the largest natural source of heat for our planet.

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Modes of Heat Transfer

Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 4 Transfer of heat takes place from a body at a higher temperature to a body at a lower temperature via one or more of the following mechanisms:  Conduction  Convection  Radiation  Heat transfer can occur through a body via all three modes simultaneously.

 Cases with occurrence of more than one mode are termed as conjugate heat transfer problems.

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Conduction

Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 5  Fourier Equation:

Q

 

kA

T

x

 Q = heat transferred  K = thermal conductivity  A = area 

T

x

= Gradient of temperature Q  The negative sign in the Fourier equation serves to counter the negative gradient of temperature.

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Convection

Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 6

Q

UhA

(

T b

T a

) Where:

T a

U = Velocity of moving fluid h = Convection coefficient A = area of the plate

T b

T b = Temperature of the solid body T a = Ambient fluid temperature Heat loss to air moving across fins on a radiator is a common engineering problem that involves convection.

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Conduction and Convection

 Diffusion  Advection Diffusion Advection Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 7 Conduction Convection © 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the original, and must attribute source content to Autodesk.

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Conduction and Convection

Ra

g

 

TL

3  Where:       Volumetric Thermal Expansivity Thermal Diffusivity Kinematic Viscosity Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 8 If the objective is to stop heat transfer, then convection can be curbed by placing obstacles in the direction of flow.

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Conduction and Convection

Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 9  Both conduction and convection can be solved by the energy equation.

 The energy equation in simplified form:  

q x

x

 

q y

y

 

q

z z

 

divq

Energy in Change in Energy Within the system Energy Out  The energy equation in full form: 

D

  1 2 (

u

2 

v

2 

w

2 )  

Dt

 

u

.

gradp

u

(   

x xx

  

yx

y

   

z zx

)   (   

x xy

  

yy

y

  

zy

z

) 

w

(   

x xz

   

y yz

   

z zz

) 

u

.

S M

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Radiation

Radiative exchange between two bodies is expressed by the equation:

Q

 

A

(

T b

4 

T a

4 )  Where: 

A

   Surface Emissivity Stephan Boltzman Constant Area of surface

T b

 Temperature in K of radiant body

T a

 Temperature in K of ambient sink Radiative loss to the ambient at absolute zero:

Q

 

A

(

T

4 ) Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 10

T a T b

Unlike convection and conduction, no medium is required. © 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the original, and must attribute source content to Autodesk.

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Solving Heat Transfer Problems

Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 11  Heat transfer problems, just like fluid flow problems, are now solved predominantly using computational techniques.

 Previously, heat transfer calculations involved calculating heat gain and loss via different modes using the formulae mentioned in the above slides.

 For convection, the majority of calculations are done using regressions evaluated by experimental techniques.

 Finite difference methods (FDM) are often taught at the graduate level for solving 2D conductive heat transfer.

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Summary

Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 12  Heat transfer affects us in profound ways.  Our very existence depends upon the transfer of heat.  The subject of heat transfer in engineering sciences is fundamental and its application is almost inescapable.  Conduction, convection and radiation are the three modes of heat transfer.

 Conduction requires a stationary medium, while convection requires a moving medium.  Heat transfer problems can be solved though numerical analysis. © 2011 Autodesk Freely licensed for use by educational institutions. Reuse and changes require a note indicating that content has been modified from the original, and must attribute source content to Autodesk.

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Summary

Section 6 – Thermal Analysis Module 1: Overview of Heat Transfer Page 13  The fundamental equation for conduction is the Fourier equation.

 For convection cases, dimensionless parameters measured through experiments are used.  In the case of radiation, the Stephen Boltzmann law applies and surface properties influence this mode of heat transfer.  Today, heat transfer problems are solved with the help of 3D computer software.

 This has greatly reduced the need for experiments, thus cutting costs and product turnaround times.

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