15
Subject : Heat & Mass Transfer Topic: Conduction Lecture No: 3 Date: 8 – Feb - 2013 Presented By: Pritesh K Jaradi

Subject : Heat & Mass Transfer Topic: Conduction Lecture No: 3 Date: 8 – Feb - 2013 Presented By: Pritesh K Jaradi

Embed Size (px)

Citation preview

Subject : Heat & Mass TransferTopic: ConductionLecture No: 3Date: 8 – Feb - 2013

Presented By:Pritesh K Jaradi

Some Expectations

Respect others Respect the college Humility

Work Ethic

DO participate and ask questions. For order in class, raise your hand when asking a question.

BRING all specified books. HAND IN all homework ON TIME! SHOW CARE and concern for each other.

Help one another in homework. BUT NO COPYING OF ENTIRE ASSIGNMENTS!

Topics Covered

Fourier’s Law of heat conduction Effect of temperature

On thermal conductivity of metal On refractories & building material On gas Liquid General heat conduction equation

Lecture 3 by Pritesh Jaradi 48 February 2013

Fundamentals of Heat TransferConduction, Convection, and Radiation Heat Transfer ModeHeat transfer (or heat) is thermal energy in transit due to a temperature difference

Lecture 3 by Pritesh Jaradi 58 February 2013

Fourier’s Law of heat conduction

Lecture 3 by Pritesh Jaradi 6

• Rate of heat flow is directly proportional to area of section at normal to heat flow.

• Rate of heat flow is directly proportional to temperature gradient.

8 February 2013

Fourier’s Law of heat conduction (Contd.)Assumptionssteady state condition.No internal heat generationHomogeneous and isotropic materialUnidirectional heat flow (1-D)

Lecture 3 by Pritesh Jaradi 78 February 2013

Conduction Heat Transfer

TkAq

dxdTk

Axq ;

•First mechanism - molecular interaction (e.g. gas)

•Greater motion of molecule at higher energy level (temperature) imparts energy to adjacent molecules at lower energy levels

•Second mechanism – by free electrons (e.g. solid)

Lecture 3 by Pritesh Jaradi 88 February 2013

Thermal Conductivity of Gas

Smaller than solid. Intermolecular space is much

large. Continuous random motion. K increases as increase of

temp. At high temp collision

increase.

Lecture 3 by Pritesh Jaradi 98 February 2013

Thermal Conductivity of Metal

Due to migration of free electrons and molecular vibration.

At high temp vibration becomes violent and obstruct free flow of electrons.

Thus reduces HT by movement of free electrons.

For alloys TC is less than pure metals.

Lecture 3 by Pritesh Jaradi 108 February 2013

Thermal Conductivity of Liquid

Close spacing molecules + strong molecular attraction force.

Heat exchange via collision process.

Lies between gases and solid.

As temp increases reduction in molecular attraction….. Leads to decrease in K

Lecture 3 by Pritesh Jaradi 118 February 2013

Conductivity of refractories and building materials

Very low thermal conductivity. Known Insulating materials Porous structure with trapped air / liquid. At increased temp, conductivity of gases increases

………….leads to increase in thermal conductivity of building materials.

Lecture 3 by Pritesh Jaradi 128 February 2013

General heat conduction equation:

Lecture 3 by Pritesh Jaradi 138 February 2013

General heat conduction equation (Contd.):

Lecture 3 by Pritesh Jaradi 148 February 2013

THE END