Electronics Cooling MPE 635

22
Electronics Cooling MPE 635 Mechanical Power Engineering Dept.

description

Electronics Cooling MPE 635. Mechanical Power Engineering Dept. Course Goals. 1. To establish fundamental understanding of heat transfer in electronic equipment. 2. To select a suitable cooling processes for electronic components and systems. - PowerPoint PPT Presentation

Transcript of Electronics Cooling MPE 635

Page 1: Electronics Cooling          MPE 635

Electronics Cooling MPE 635

Mechanical Power Engineering Dept.

Page 2: Electronics Cooling          MPE 635

1. To establish fundamental understanding of heat transfer in electronic equipment.

2. To select a suitable cooling processes for electronic components and systems.

3. To increase the capabilities of post-graduate students in design and analysis of cooling of electronic packages.

4. To analysis the thermal failure for electronic components and define the solution.

Course Goals

Page 3: Electronics Cooling          MPE 635

• Part-A• Main topics • Introduction to electronics cooling and thermal

packaging• Introduction to basic modes of heat transfer • Conduction heat transfer and extended surfaces in

electronic devices• Transient conduction• Natural convection heat transfer (i.e. PCB cooling) • Forced convection heat transfer (Internal and External

flow )• Fan performance• Radiation heat transfer and its applications in electronic

devices• Solving the electronics cooling problems with EES

software• Electronics cooling problems• Solution of selected electronics cooling problems

Page 4: Electronics Cooling          MPE 635

3. Basics of Heat Transfer

Page 5: Electronics Cooling          MPE 635

Modes of heat transfer

Page 6: Electronics Cooling          MPE 635

Conduction

• Conduction heat transfer as diffusion of energy due to molecular activity.

• Conduction in liquids and solids ascribed to molecules vibration (solids), translational and rotational (liquids)

Page 7: Electronics Cooling          MPE 635

Conduction

• Fourier’s law

dx

dTkqx

L

TTkqx

12

Page 8: Electronics Cooling          MPE 635

Thermal convection

• The heat transfer by convection is described by the Newton's law of cooling:

)( TThAq WA ir m o v e m e n t d u e t o t e m p e ra t u re d iffe re n c e

(a )F re e c o n v e c t io n o n e le c t ric c o m p o n e n t s c h ip s

A ir

(b )F o rc e d c o n v e c t io n o n e le c t ric c o m p o n e n t s c h ip s

F o rc e d fa n

Page 9: Electronics Cooling          MPE 635

Thermal convection

• convection heat transfer ranges Process h(w/m2.k)

Free convection - gases 2-25 - liquids 50-1000Forced convection - gases 25-250 - liquids 50-20,000Convection with two phase - boiling or condensation 2500-100,000

Page 10: Electronics Cooling          MPE 635

Thermal convection

• Example 3.1: An electric current is passed through a wire 1mm diameter and 10 cm long. This wire is submerged in liquid water at atmospheric pressure, and the current is increased until the water boils. For this situation h = 5000 W/m2.oC. And the water will be 100 oC. How much electric power must be supplied to the wire to maintain the wire surface at 114 oC?

Schematic:

Electric wire

Water

Page 11: Electronics Cooling          MPE 635

Thermal convection

• Solution:• The total convection loss from the wire is

given by.

• For this problem the surface area of the wire is A= π d L = π (1 x 10-3) (10 x 10-2) = 3.142 x10-4 m2

• The heat transfer is therefore

• And this is equal to the electric power which must be applied.

)( TThAq W

Wq 99.21)100114(10142.35000 4

Page 12: Electronics Cooling          MPE 635

Thermal radiation• The mechanism of heat transfer by radiation

depends on the transfer of energy between surfaces by electromagnetic waves in the wave length interval between 0.1 to 100 μm.

• Radiation heat transfer can travel in vacuum such as solar energy.

• Radiation heat transfer depends on the surface properties such as colors, surface orientation and fourth power of the absolute temperature (T4) of the surface.

• The basic equation for radiation heat transfer between two gray surfaces is given by

)( 42

41 TTfAq

Page 13: Electronics Cooling          MPE 635

Thermal radiation

• Example 3.2. A horizontal steel pipe having a diameter of 10 cm is maintained at a temperature of 60 oC in a large room where the air and wall temperature are at 20 oC with average heat transfer coefficient 6.5 W/m2K. The emissivity of the steel is 0.6 calculate the total heat lost from the pipe per unit length.

Page 14: Electronics Cooling          MPE 635

Thermal radiation

• Solution:• The total heat lost from the pipe due

to convection and radiation

• Because the pipe in a large enclosure then the geometrical factor ƒ = 1

)()( 44

TTfATTAh

qqq

SS

radiationconvectiontotal

mW

xxxqtotal/33.134

)293333)(1.0)(1)(6.0(1067.5)2060)(1.0(5.6 448

Page 15: Electronics Cooling          MPE 635

• There exists an analogy between the diffusion of heat and electrical charge. Just as an electrical resistance is associated with the conduc tion of electricity, a thermal resistance may be associated with the conduction of heat.

Analogy between Heat Transfer and Electric Circuits

Page 16: Electronics Cooling          MPE 635

Analogy between Heat Transfer and Electric Circuits

haR

TRqThAqkA

LR

TRqL

TkAq

convt

convtconvconv

condt

condtcondcond

1,

,

,

,

A

L

I

EERe

12

Page 17: Electronics Cooling          MPE 635

Series Circuits:

• By analogy

AhkAL

Ah

TTq

RRR

TTq

R

Tq

convtcondtconvt

t

overall

21

21

,,,

21

11

3,2,1,

21

eeee RRR

EE

R

Ei

Page 18: Electronics Cooling          MPE 635

Parallel Circuit: L1, k1, A1

L7, k7, A7

L6, k6, A6

L5, k5, A5

L4, k4, A4

L3, k3, A3

L2, k2, A2

qtotqtot

T1

T2

ittott

totttot

ttttttttot

itot

itiiii

RR

R

Tq

RRRRRRRTq

qq

R

T

L

TAkq

,,

,

7,6,5,4,3,2,1,

,

11

1111111

q1

qtot qtot

q7

q6

q7

q5

q6

q4

q5

q3 q3

q2 q2

R7

R6

R5

R3

R2

R4q4

Page 19: Electronics Cooling          MPE 635

Combined Modes of Heat Transfer

• Combined Convection and Radiationradconvnet qqq

)( fsrrad TTAhq

)(

)(

)(

44

fs

esse

fs

radr TT

TTF

TTA

qh

)(

)()()(

)(

)(

22

44

fs

fsfsfsser

fs

fsser

TT

TTTTTTFh

TT

TTFh

Page 20: Electronics Cooling          MPE 635

• Combined Convection and Radiation

Now if we define the arithmetic mean temperature as:

If further Ts-Te<<Ts then

So we may define the radiation heat transfer coefficient as:

And finally;

Where

)()2)((

)()(2

22

fsfsfsser

fsfsser

TTTTTTFh

TTTTFh

2fs

m

TTT

fsm TTT

34 mser TFh

)( fstotnet TTAhq radconvtot hhh

Combined Modes of Heat Transfer

Page 21: Electronics Cooling          MPE 635

Combined Modes of Heat Transfer

• Combined Convection and Conduction

• This combination is likely to occur with the use of extended surfaces where the primary surface exchanges heat by convection to the adjacent fluid flow and by conduction through the extended surfaces. This case may be considered in a similar manner as the above, but here the problem doesn't need extra work as the conduction thermal resistance is predefined.

condconvnet qqq

AL

TextTskTfTshconvqnet

)(

)(

Page 22: Electronics Cooling          MPE 635

Overall Heat Transfer Coefficient

)(1

)()()(1

1

,,,,,,

",

,,,

",

,,, shhfphhshhfph

hf

msccfpc

cf

sccfpcc

cchh

AAhAA

R

kAx

AA

R

AAh

AUAU

Fluid combination U, W/m2.ºK.

Water to water 850-1700

Water to oil 110-350

Steam condenser, water in tube 1000-6000

Ammonia condenser, water in tube 800-1400

Finned tube heat exchanger, water in tubes air in cross flow

25-50