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DETERMINATION OF FRACTURE TOUGHNESS IN PBGA PACKAGES USING FINITE ELEMENT AND

EXPERIMENTAL METHODS

by

TAN CHEW PHENG

Thesis submitted in fulfillment of the

requirements

for the

degree

of

Master of Science

U.S.M, Penang

November 2006

14,976 Words

(2)

,\'�t1"wkd!;CI1lCI1I'

ACKNOWLEDGEMENTS

I would like to express my

appreciation

and thanks to my supervisor Assoc. Prof. Dr. Ishak

Hj.

Abdul Azid and my

co-supervisor,

Assoc. Prof Dr

Mani Maran for their

grateful support, encouragement

and invaluable

guidance

in

helping

me to cope in every

stage

of the

project

I also wish to thank my friends from the School of Mechanical

Engineering,

Universiti Sains

Malaysia especially

Mr.

Ong Kang

Eu and Mr

Lee Boon

Leong

for their

help

in this

project.

I also wish to thank Prof. K. N Seetharamu and Prof. M. V. V.

Murthy

for their

guidance during

the

early

stage of this

project.

I would like to thank every lab staff of the School of Mechanical

Engineering especially

Mr. Baharom B.

Awang

and Mr. Md. Ashamuddin Hasim for their technical

support during

my

experiments

for this project I also would like to thank Mr. Md. Zandar Md. Saman from the School of Materials & Minerai

Resources

Engineering

in

providing

materials.

Finally,

I wish to thank my

family

members for their moral support

especially

my

parents.

Thanks also to those who

helped

me either

directly

or

indirectly

in

completing

my

project.

1,\1\ ('lIEWr/lENG McchFI1�.US1\(()(" 11 -

(3)

Tableofcontents

TABLE ,,)F CONTENTS

Page

Acknowledgements

II

Table of Contents III

List of Tables VIII

List of

Figures

X

List of Plates xv

List of Abbreviations XVI

List of

Symbols

XIX

List of

Equations

xxv

Abstrak XXXI

Abstract XXXIII

CHAPTER 1 - INTRODUCTION 1-6

1.1

Background

of research 1

1.2 Problem statement 3

1.3

Objectives

4

1.4

Scope

of research 5

CHAPTER 2 - LITERATURE REVIEW 7-21

2.1 Introduction 7

2.2 Review of related research on vapor pressure effect 7

2.3 Review of fracture

toughness analysis techniques

10

2.4 Review of related research on fracture

toughness

method 15

2.5 Review on

holographic interferometry techniques

18

TAN cutw PHENGMcchEng,USM 0(,' - III -

(4)

Table ofcontents

2.6 Review of

holographic technique applied

for fracture

toughness

19

2.7

Summary

20

CHAPTER 3 - ANALYSIS OF STRESS INTENSITY FACTOR IN 22-50 PLASTIC BALL GRID ARRAY

(PBGA)

3.1 Introduction 22

3.2 Theoretical

applications

of MCCI method 24

3.3 Methods of measurement 26

3.4

Methodology

29

3.5 Verification on Meei method 32-36

3.5.1 Thin

quad

flat

package

finite element

modeling

32

3.5.2

Sample

calculation on strain energy release rate 35

3.5.3 Results and discussions 36

3.6 Simulations and calculations 37-43

3.6.1

Temperature

distribution 37

3.6.2 Moisture distribution 39

3.6.3

Vapor

pressure determination 43

3.7 Results and discussions 44-49

3.7.1

Sample

calculation on strain energy release rate 45 3.7.2

Sample

calculation on stress

intensity

factor 45

3.7.3 Results and discussions 47

3.8

Summary

49

CHAPTER 4- DETERMINATION OF FRACTURE TOUGHNESS 51-76 USING SIMULATION AND CONVENTIONAL TENSILE TEST

4.1 Introduction 51

4.2

Underlying

theories offracture

toughness

test 53-59

TAN CIIEWPlIENG McchEng.USM 06' - IV -

(5)

Table()fcontents

4.2.1

Theory

of fracture

toughness

53

4.2.2 Fracture

toughness for single edge

notched tension 55

4.3

Sample specifications

60

4.4 Simulation evaluation 61-69

4.4.1

Ansys

simulation on thin

plate

deformation 6'1

4.4.2 Parameter

study

62

4.4.3 Discussions 68

4.4.4

Epoxy

based

polymer

thin

plate

evaluation 69

4.5 Conventional tensile test evaluation 70-74

4.5.1 Procedures oftest 70

4.5.2 Results and discussions 70

4.6

Summary

75

CHAPTER 5 - DETERMINATION OF FRACTURE TOUGHNESS 77 -118 USING HOLOGRAPHIC INTERFEROMETRY METHOD

5.1 Introduction 77

5.2

Underlying

theories of real-time

holographic interferometry

79

5.3

Methodology

82-89

5.3.1

Optical system

for

holographic

measurement 82

5.3.2

Layout specifications

84

5.3.3

Expanding

beam with

spatial

filter 85

5.3.4 Beam

intensity

ratio 86

5.3.5

Optical stability

test 87

5.3.6

Exposure

time

during image recording

88

5.3.7

Hologram image processing

88

5.4

Holographic interferometry

calibration 89-102

IAN CHEWPIlENGMcchEng.USM06' - V-

(6)

Tableoi"contents

5.4.1 Cantilever evaluation 89

5.4.2 Strain energy for linear deflection 94

5.4.3

Measuring fringe

order number 95

5.4.4

Perspective

distortion 97

5.4.S

Sample

calculations 98

5.4.6 Results and discussions 101

5.5 Uniform axial load evaluation

using holographic interferometry

103-114

5.5.1 Mathematical

application

103

S.S.2

Correcting

errors in

holographic

fracture

toughness

test 104

5.S.3

Holographic

fracture

toughness

test for aluminum 106 5.5.4

Holographic

fracture

toughness

test for epoxy 110

5.6 Results and discussions 114

S.7

Types

of error

during holographic interferometry

115

S.8

Summary

118

CHAPTER 6 - CONCLUSIONS AND RECOMMENDATIONS 119-121

6.1 Conclusions 119

6.2 Recommendations and futurework 121

References 122-127

1 .

2.

Ansys

simulation program code for TQFP

plastic

deformation

Ansys

simulation program code for PBGA

temperature

distribution

Ansys

simulation program COC9 for PBGA wetness distribution

Ansys

simulation program code for PBGA

plastic

deformation

128-213

128

135

Appendices

3.

4.

145

155

T /\NCIIEWPHENG MechEng.USM 06' - VI -

(7)

Tableofcontents

5.

Ansys

simulation program code for thin

plate

deformation 164 6.

Ansys

simulation on aluminum

plate

in different crack ratio 168

7. Simulation

analyses

on thin

plate

fracture

toughness

172

8. Cantilever deflection

using holographic interferometry

method 176

9. Aluminum

plate

extension

using holographic interferometry

192

method

10.

Epoxy plate

extension

using holographic interferometry

method 204

Publication List

I.A.

Azid,

C.P. Tan. B.L.

Lee,

K.N. Seetharamu

(2005).

Fracture Mechanic

Analysis

for

Package

Delamination.

Key Engineering Materials,

Vols.297-300.

p.844-850.

TANCHEWPHENGMechEng.USM 06' - VU -

(8)

Listoftables

LIST OF TABLES

Page

Table 3.1 Dimensions of PBGA 23

Table 3.2 Material

properties

forthe main constituents of PBGA 23 Table 3.3 Shear modulus for interfacial delamination stress 24

intensity

factor

Table 3.4 Mathematical

applications

of

experimental

methods 29 Table 3.5

Analogy

between thermal and moisture 29

Table 3.6 Dimensions ofTQFP 33

Table 3.7 Material

properties

for the main constituents ofTQFP 33 Table 3.8

Comparison

MCGI method with

Park,

Y.B. et als 36

results for 1 MPa vapor pressure

Table 3.9 Thermal

properties

for PBGA 37

Table 3.10 Moisture

properties

for PBGA

(85°C/85%RH)

39

Table 4.1 Material

properties

for

AI, Cu,

MS and epoxy resins 51 Table 4.2 The

specifications

and its

plane

condition 60

Table 4.3 Critical load and

compliance

rate for

AI,

Cu and MS 73

Table 4.4 Fracture

toughness

used total extension for

AI,

eu and 74

MS

Table

5.1(a) Compositions

of chemical for solution A 88 Table

5.1(b) Compositions

of chemical for solution B 88 Table

5.1(c) Compositions

of chemical for bleach solution 88 Table 5.2 Values of deflection for

6�m deflection, 6:r

delivered 99

theoretically

Table 5.3 Coordinates of

point

a, b and c 100

TAN CHEWPHENG McchEng.USM 06' - Vl11 -

(9)

l.istoftables

Table 5.4 Deflections obtained

experimentally

in case

study

1 100 Table 5.5 Deflections obtained

experimentally

in case

study

2 101 Table 5.6 Extension

along

AI

plate,

2.45mm crack

length

loaded 107

with 4N

using

HI method

Table 5.7 Material

properties

for D.E.R. 331 cured with Ancamide 110 260A

Table 5.8 Extension

along

epoxy

plate,

1mm crack

length

loaded 112

with 1 N

using

HI method

TANCIIEWPHENG McchEng,USM 06' - IX-

(10)

l.rstoffigures

LIST OF FIGURES

Page

Figure

1.1 I R reflow

soldering profile

2

Figure

1.2 Plastic

collapse

of popcorn failure 4

Figure

2.1

Cracking

mechanism

during

reflow

soldering

8

Figure

2.2 Cracked

body subjected

to load F 10

Figure

2.3 Load-extension

diagram

11

Figure

2.4 SENB for K determination 13

Figure

2.5 CT for K determination 14

Figure

2.6 Interiacial fracture

toug

hness test 14

Figure

2.7 Schematic

diagram

of adhesion test 16

Figure

2.8 Generic

interferometry

model 18

Figure

3.1 Schematic of X PBGA 22

Figure

3.2 The

principle

of

superposition

28

Figure

3.3 The

spectrum

of

experimental

methods

applied

on 28

fracture

problems

Figure

3.4 Crack

tip

elements 31

Figure

3.5 Cross sectional view ofTQFP 33

Figure

3.6

Typical plastic

deformation in TOFP 34

Figure

3.7 Plastic deformation in TQFP

(x1 00)

35

Figure

3.8 Variation of SERR with delamination ratio for TQFP 36

using

MCCI method at different vapor pressure

loadings

Figure

3.9

Temperature

distribution on PBGA

during

reflow 38

Figure

3.10 Case

study

on

temperature

distribution for LEO 39

TANCHEWPHENG McchEng.USM 06' - X -

(11)

LI�lofligures

Figure

3.11 Transientwetness distribution in PBGA for 34 hours 40

Figure

3.12 Transient wetness distribution in PBGA for 168 41 hours

Figure 3.13(a)

Transient wetness distribution in LED for 34 hours 42

Figure 3.13(b)

Transient wetness distribution in LED for 168 hours 42

Figure

3.14

Typical plastic

deformation in PBGA 44

Figure

3.15 Plastic deformation in PBGA

(x1 000)

45

Figure 3.16(a)

Variation of SERR with delamination ratio for PBGA 47

Figure 3.16(b)

Variation of SIF with delamination ratio for PBGA 47

Figure 3.17(a)

Variation of SERR with vapor pressure for PBGA 48

Figure 3.17(b)

Variation of SIF with vapor pressure for PBGA 48

Figure

4.1 3-D

drawing

of thin

plate specimen

52

Figure

4.2 Conventional tensile test 52

Figure

4.3 Fracture

toughness

with thickness for steel 54

(rr, =2068.43MPa)

Figure

4.4 Linear elastic thin

plate

55

Figure

4.5 Plate su

bjected

with a load 55

Figure

4.6 Free

body diagram

of thin

plate

in left

portion

57

Figure

4.7 AI

plate

deformation with crack ratio 0.1

(x100)

61

Figure 4.8(a)

Variation of fracture

toughness

with crack

length

62

ratio on total extension and crack

edge

extension for

AI

Figure 4.8(b)

Variation of fracture

toughness

with total

plate length

63

for AI

Figure 4.8(c)

Variation of fracture

toughness

with

plate

thickness 63

for AI

Figure 4.8(d)

Variation of fracture

toughness

with

applied

load for 64

AI

T ANCHEW PHENG MechEng.USM06' - Xl -

(12)

l.ist oi"figures

Figure 4.9(a)

Variation offracture

toughness

with crack

length

64

ratio on total extension and crack

edge

extension for eu

Figure 4.9(b)

Variation offracture

toughness

with total

plate length

65 for Cu

Figure 4.9(c)

Variation of fracture

toughness

with

plate

thickness 65

for Cu

Figure 4.9(d)

Variation of fracture

toughness

with

applied

load for 66

eu

Figure

4.1

O(a)

Variation of fracture

toughness

with crack

length

66

ratio on total extension and crack

edge

extension for MS

Figure 4.10(b)

Variation of fracture

toughness

with total

plate length

67

for MS

Figure

4.1

O(c)

Variation of fracture

toughness

with

plate

thickness 67

for MS

Figure

4.1

O(d)

Variation offracture

toughness

with

applied

load for 68

MS

Figure

4.11 Variation of fracture

toughness

with crack

length

69

ratio for epoxy

Figure 4.12(a)

Total extension-load curve for AI 71

Figure 4.12(b)

Variation of

compliance

with crack

length

ratio for AI 71

Figure 4.13(a)

Total extension-load curve for eu 72

Figure 4.13(b)

Variation of

compliance

with crack

length

ratio for eu 72

Figure 4.14(a)

Total extension-load curve for MS 73

Figure 4.14(b)

Variation of

compliance

with crack

length

ratio for 73

MS

Figure

5.1 Load-extension mechanism 78

Figure

5.2 Path of incident and reflected rays at

point

b 80

Figure

5.3 3-D reflected ray at

point

o 80

Figure

5.4

Optical system

for HI measurement 83

TANClIEWI'll[NG McchEng.USM06' - XII

-

(13)

List offigures

Figure

5.5

Optical layout

with its

specifications

84

Figure

5.6

Optical system

for

stability

test 87

Figure

5.7 Cantilever deflected in an

angle, ¢

90

Figure

5.8 Illumination and observation

angle

in x- z

plane

91

Figure

5.9 Cantilever rotate into an

angle, /3

93

Figure

5.10 Free

body diagram

of cantilever with

applied load,

F 94

Figure

5.11 Line

profile

of

fringes pattern

for cantilever deflection 96

Figure

5.12

Comparison

of unit

pixel

and unit dimension in the 97

analysis

of

perspective

distortion

Figure

5.13

Ansys

simulation on cantilever deflection

(x200)

for 99

Bum deflection, oZF

Figure 5.14(a) Comparison

of

holographic

result with deflection 101

theory

for cantilever in

0ZF =6�m

Figure 5.14(b) Comparison

of

holographic

result with deflection 102

.

theory

for cantilever in

au

=1

Ourn

Figure 5.14(c) Comparison

of

holographic

result with deflection 102

theory

for cantilever in

au

=

14J.lm

Figure 5.15(a)

Extension distribution

along plate using

HI method 105

Figure 5.15(b)

Extension distribution

along plate using Ansys

105

simulation

Figure

5.16

Correcting

errors in

holographic analysis

106

Figure

5.17 Load-extension curve for AI

plate

with crack

length,

106

as=

4mm

Figure

5.18 Line

profile

of

fringes pattern

for AI

plate,

2.45mm 107

crack

length

loaded with 4N

Figure

5.19 Extension distribution

along

AI

plate

108

Figure

5.20 Strain at center crack in different

loading

for AI

plate

108

Figure

5.21 Variation of

compliance

with crack

length

ratio for AI 109

plate

IANcur.w1'1I[,NG MeehEng.USM 06' - Xlll -

(14)

l.istoffigures

Figure

5.22 Load-extension curve for D.E.R. 331 with crack 111

length,

as= 4.5mm

Figure

5.23 Line

profile

of

fringes pattern

for epoxy

plate,

1mm 112

crack

length

loaded with 1N

Figure

5.24 Extension distribution

along

epoxy

plate

112

Figure

5.25 Strain at center crack in different

loading

for epoxy 113

plate

Figure

5.26 Variation of

compliance

with crack

length

ratio for 113

epoxy

plate

Figure

5.27

Safety

conditions for EMC

(O.E.R. 331)

on PBGA 114

TANCHEW PHENG McchEng.USM 06'

- XIV -

(15)

list ofplates

LIST OF PLATES

Page

Plate 5.1 Illustration of load frame 79

Plate 5.2 Real-time

interferometry set-up

for cantilever evaluation 83

Plate 5.3 Cantilever beam 90

Plate

5.4(a)

Cantilever

image

96

Plate

5.4(b)

Initial

fringes pattern

96

Plate

5.4(c)

Loaded

fringes pattern,

case

study

1 96

Plate

5.4(d)

Loaded

fringes pattern,

case

study

2 96

Plate 5.5

Graph

paper as

rectangular grid pattern

on cantilever 97

beam

during analysis

of

perspective

distortion

Plate 5.6

Fringes pattern

for AI

plate,

2.45mm crack

length

loaded 107

with 4N

Plate 5.7

Fringes pattern

for epoxy

plate,

1mm crack

length

111

loaded with 1N

Plate

5.8(a) Hologram

with

fringes

in its initial condition 117 Plate

S.8(b) Hologram

with

fringes

in its initial condition 117

TANCHEW PHENGMechEng.USM06' - XV -

(16)

List ofabbreviations

LIST OF ABBREVIATIONS

Page

1-0 One-dimensional 8

2-D Two-dimensional

8,20,22,25-28

3-D Three-dimensional

20,26,28,52,78-92,121

Ag

Silver 23

AI Aluminum

51,60-64,

70-77,104-109

Anhyd. Anhydrides

88

ASTM American

Society

for

Testing

and Materials 55

8S1 British Standards Institute 55

BT Bismaleimidetriazine

22,23,37

-40

CCD

Charge-coupled

device

83,95

CI Conventional

interferometry

19

C-SAM C-mode

scanning

acoustic

microscopy

8

CPU Central

processing

unit 83

CTE Coefficient of thermal

expansion 15,17

Cu

Copper 17,24,51,60-66,70-75

O.E.R Dow epoxy resins

(trademark

ofthe Dow

49,77,110-121

Chemical

Company)

OHI

Digital holography interferometry 19,20

EMC

Epoxy molding compound

1-6,

16,23,30�34,

77,114-121

ESPI Electronic

speckle pattern interferometry

19

FE Finite element

3,9,25,30,78

TANCHEW PHENG McchEng,USM06' - XVI -

(17)

List ofabbrevintions

FEA Finite element

analysis 4,9121-23,29,34,35.40, 45,49,52,59,119,121

FEM Finite element method 18,25,26

GI

Grating (moire) interferometry

19

HI

Holographic interferometry 4-7,18-21,68,74-89,

98-107,111-121

IC

Integrated

circuit

1,8,9,17

IR InfraRed 1

JEDEC Joint Electron Device

Engineering

Council 40

LED

Lig

ht

emitting

diode

38,39,41,42

LEFM Linear elastic fracture mechanics 15.25,69

MGGI Modified crack closure

integral 5,24,26,30- 32,36,49,119,121

NOT Non-destructive test 18

PBGA Plastic ball

grid

array

2-8,22,23,36-49.

77,114-120

PCB Printed circuit board

22,23,37

-39

PQFP Plastic

quad

flat

package

53

QFN Quad flat non-lead 9

RH Relative

humidity 5,22,40-43

SERR Strain energy release rate

4,15-17,22-27,30, 35,36,45-49,58

Si Silicon

23,33

SiC Silicon carbide 49

SIF Stress

intensity

factor

4-6,13-17,22-31,

46-53,59,114,118-121

SMD Surface mount device 7

SMT Surface mount

technology

1,15

TANCHEW PH ENG McchEng,USM 06' - XVll -

(18)

Listof abbreviations

SOJ

TQFP

VPR

Small outline J-Ieaded

Thin

quad

flat

package Vapor phase

reflow

TANCHEW PHENG MechEng,USM 06'

40,43 5,15,16,32-36,49

1,9

- XVlll -

(19)

List of syrnbo!s

LIST OF SYMBOLS

Page

t;

Reflow

soldering temperature (OC)

2

Ix

Soldering

time

(s)

2

as Control

sample's

crack

length (m) 6,70-73,106-113

t Thickness

(m) 10-15,26-35,45,52-69

78,95,98,109,114

F

Applied

load

(N) 10-14,31,35,45,52-73,

94-99,105-113

8 Crack

edge

extension

(m) 10-12,55-62,108,112

a Crack

length (m) 10-14,25,26,31-36,

45-73,78,109-114

W

Sample

width

(m) 10-15,52-73,78,

95,98,109-114

G Strain energy release rate

(J/m2) 11,12,25,26

U Stored strain energy

(J) 11,12,56,57

C

Compliance,

the

slope

of extension-load

12,71-73,108-114 (mIN)

Ke

Critical stress

intensity

factor

(MPa

m

1/2) 12-17,49-54,59- 69,74,1

09,114

Ge

Critical strain energy release rate

(J/m2) 12,15,58,59

E

Young's

modulus

(GPa) 12,15,23,26,32,33,46,

51-73,94,98,109-114

Fe

Critical

loading (N) 12-15,58,59,

70-74,106-114

L

Length

distance

(m) 13-15,33,52-69,90-113

S Distance between two

pin support (m)

13

K Stress

intensity

factor

(MPa

m

1/2) 13,14,28

TANCHEW PHENGMcchEng,USM 06' - X1X -

(20)

Li,1 ofsymbols

Moment inertia of

multilayer (dimensionless)

15

E" Effective

Young's

modulus

(GPa) 15,32,46

Jr Pi

(=3.142) 15,25,31,32,46

f2 Bimaterial constant

(dimensionless) 15,31.32,46

J Crack

driving force,

J

integral (J/m2) 15,16,27,32.49,53 KJI

Mode II stress

intensity

factor

(MPa

m

1/2) 16,26

KlIC

Critical mode II stress

intensity

factor

(MPa

16

m

1/2)

v Poisson's ratio

(dimensionless) 23,32,33,45, 46,51,62-73

ji Shear modulus

(GPa) 24,31,32,45,46

ljI Work ofthe external tractions per unit 25 thickness

(Jim)

Strain energy of the

body

per unit thickness 25

(jim)

Normal stress

(N/m2) 25,29,56

r Shear stress

(N/m2) 25,29

v

Opening displacement

on crack surfaces

(m) 25,26,29,31,35,45

u

Sliding displacement

on crack surfaces

(m) 25,26,29 GI

Mode I strain energy release rate

(J/m2) 26,31-36,45-48 G"

Mode II strain energy release rate

(J/m2)

26

KI

Mode I stress

intensity

factor

(MPa

m

1/2) 26,32,46-49,114

TJ

Multiplier depending

Poisson's ratio u and

26,46,59 geometry (dimensionless)

77=

1/(I-u2)

for

plane strain;

17;:: l for

plane

stress

�.

Normal force

(N)

26

Fe

Shear force

(N)

26

T AN CHEWPHENGMcchEng,USM 06' - XX-

(21)

Li51ofsymbols

o

Strain energy

density (J/m3)

27

T Traction vector

(N/m2)

27

u

Displacement

vector

(m)

27

ds Element of arc

length

around the contour r 27

(m)

r Contour in crack

driving

force 27

(dimensionless)

N

Fringe

order number

(dimensionless) 29,79-81,90-96,

100-107,112

r. Optical sensitivity

constant

(N/m.lines)

29

fi Fringe sensitivity (miIines)

29

B Additional non-strain-related motion

(lines)

29

la

Photoelastic constant for material

(N'rn.lines)

29

T

Temperature (OC)

29

w Wetness fraction

(dimensionless) 29,40

p Material

density (kg1m3) 29,30,37

k Thermal

conductivity (W/mOC) 29,30,37

D Moisture

diffusivity (m2/s) 29,30,39

C\O{ Saturated concentration

(kg/rn3) 29,30,39

Cp

Specific

heat

(J/kgoC) 29,30,37

pr

Vapor

pressure in the delamination

during 30,35,43-48

reflow

(Pa)

�(�)

Saturation water vapor pressure

30,38,43 corresponding

to reflow

soldering

temperature (Pa)

RHIII Relative

humidity

at moisture

conditioning 30,43 (dimensionless)

lV"Jr

Wetness in the delamination

during

reflow

30,40,43 (dimensionless)

TAN CHEWPHENG McchEng.USM 06' - XXi -

(22)

Listofsymbols

K

Multiplier depending

Poisson's ratio v and

geometry (dimension less)

K=

(3

-

4u)

for

plane strain;

K=

(3-u)/(l+v)

for

plane

stress

f

Length

of die

pad (m)

e

Length

of

chip (m)

ar Thermal

diffusivity (m2/s)

h Convective heat transfer coefficient

(W/m20C)

Wo Initial wetness fraction

(dimensionless)

ao Initial delamination

length (m)

ae Allowed

length (m)

K/c

Plane strain fracture

toughness (MPa

m

1/2)

(Jrs Tensile

strength (MPa)

(Jy Yield

strength (MPa)

5' Total extension

(m)

5e

Critical crack

edge (m)

c Linear strain

(dimensionless)

M External moment

(Nm)

/ Moment inertia

(rn")

6:;.-

Deflection at load F

(m)

q Distributed load

(N/m)

F;

Virtual load

(N) MI

Virtual moment

(Nm) 58

Deflection of beam

(m)

5{)

Crack

edge en.largement by plate

deformation

(m)

TAN CHEWPHENGMechEng,USM 06' - xxii -

31,32,45,46

33.35,36 33,45-48,114

37

37

40

49

49

49,51-55,62,66,114

51,59-69,110

52-56,62,71-73, 78,105-112

55

56,106-113

56,57

56-59,94-98 57,58,94-102

57,58 57,58 57,58,94

58

58

(23)

LISIofsymbols

A Area atthe center of thin

plate (m2)

59

K/c

Mean

plane

strain fracture

toughness (MPa

60

m

1/2)

ar Mean

yield strength (MPa)

60

<:

Maximum

plane

strain fracture

toughness 62,64,69 (MPa

m

1/2)

KIC,,"n Minimum

plane

strain fracture

toughness 62,64,69 (MPa

m

1/2)

p Pressure

loading (MPa)

63,65,67

r;

Tensile

loading,

70% less than critical 70-74

loading (N)

Laser

wavelength (nm) 79-81,90-93.99.103

Illumination vector

(dimensionless) 79-82,90-94

o Observation vector

(dimensionless)

79-82,90-94

d

Displacement

vector

(m) 79-81,90-94,99-112

¢>

Deflection

angle (0) 80,90,94

r

Angle

between vectord and x- z

plane (0)

80

PLD Path

length

difference

(m)

84

Lb

()y Path

length

of

object

beam

(m)

84

LIe! Path

length

of reference beam

(m)

84

BR Beam

intensity

ratio

(dimensionless)

86

I'd

Reference beam

intensity (Lux)

86

Ir/hj Object

beam

intensity (Lux)

86

eo

Observation

angle (0) 91,92

o,

Illumination

angle (0) 91,92,100

e

Rays angle (0) 92,93,103

TANruewPHENGMcchEng.USM06' - XXlH -

(24)

Listofsymbols

fJ

Rotation

angle (0) 93,103

!3,mg Image turning angle (0)

97,98

x' Cantilever's coordinate

along

x' axes

(m) 97,98

X

Image pixel along

X axes

(pixel) 97,98

y

Image pixel along

y axes

(pixel)

97,98

r

Scaling

factor

along

X axes

(m/pixel)

98

� Correcting

scale for

holographic analysis 105,107,112 (dimensionless)

8u

Initial crack

edge (m)

108

TANCHEWPHENG McchEng.USM06' - XXIV -

(25)

l.istofequations

Equation

2.1

Equation

2.2

Equation

2.3

Equation

2.4

Equation

2.5

Equation

2.6

Equation

2.7

Equation

2.8

Equation

2.9

Equation

2.10

Equation

2.11

LIST OF EQUATIONS

Gtda=OFF'

=OFE+EFF'E'-OF'E'

G-JUI

taa F

V=-F.o1 2

c=!_

F

G=

[2

(aci

2t Da

)

Ke =�GcE'

=

F;

(8C)EI

2t aa

K=

3FS1/-:;- [1.93 (.::)V2

-

3.07(!:)l!Z

+

14.53(.::)51

-

zs.u:

.1

�':

+25.8 "

-;

l

21 W .. It' JIl JI" II. ii J

=_6�_[1.93(�)V2

tW,,2 IV

-3.o7'l.::)Ji: +14.53(")��

JI' \11 -25.11,II",:�:+25.S".H

":l

F

[ ()V2 (

\)12

( .5 .

'= ":

=- 11.58.E..

-18.42.E..)

+87,181�, -150.66" +JS·U·J

tWV2 IV w ,,,"': II H_

K -

_fL_

f(!!_)

c

-

tWl/2

W

( ) [

1'2 J"�

,' "

, "-

f E_ =

11.58(�).' -IU2(!:)

-

+87.18:( -d

-

-150.66 ,I

+15H ,1

-

i

W W II' \WJ ,II JI J

Ke

=

t�J' ./(;)

f( �1_)=[177.6(!:.))lI2 _1113(!:.}l'� +3934.2'::"';'=

-6102 .1 ': ....)S33,� ,0:-

JV JI' IV \11 II "_

TANCHEWPHENG McchEng.USM 06' - XXV-

Page

11

11

11

12

12

12

12

12

13

13

14

(26)

LISI ofequations

Equation

2.12

Equation

2.13

Equation

3.1

Equation

3.2

Equation

3.3

Equation

3.4

Equation

3.5a

Equation

3.5b

Equation

3.6

Equation

3.7

Equation

3.8

Equation

3.9

Equation

3.10

Equation

3.11

G

=_1

(g(FcLJ2J

__l

(_!3_(FeLJ2J

eII f3 W 2£' " 3 W

I 2 l)

15

Ke

=

JGcE· cosh(nn)

15

G=dlf_dc!>

da da

25

G = lim

_1_

r

(7

(

Sa- r,

O)

v

(r,

Jr

)

dr

&l-O2Lla

+lim

_1_

r

r

(

Doa- r,

O)

u

(r,

K

)

dr

60-02�a

25

K2

K 2 G=GI +G11 =�I +_11

E E

26

26

GI =lim�l-Fy

- 2D.a1 .s, 26

26

(

. au

J

J =

Sr Udy

- Taxds

27

p,. = PK"

(T ).

RHm Wd.Tr

30

31

31

32

K)

=

JGIE· cosh(nn)

32

TANCHEWPHENG McchEng.USM06' - XXVI -

(27)

List ofequations

Equation

4.1a

Equation

4.1 b

Equation

4.2a

Equation

4.2b

Equation

4.3

Equation

4.4

Equation

4.5

Equation

4.6

Equation

4.7

Equation

4.8

Equation

4.9

Equation

4.10

Equation

4.11

Equation

4.12

Equation

4.13

54

54

F

CJ=::---

(W-a)t

56

8'

E=-

L

56

(J=E'E 56

U=_l_

2EI

fM2dx

56

g

=8U

:F 8F

=_1

El

fM(8M'Lv

8F

r

57

F q=­w

57

57

BMx_:r

--=X

8F;

57

l

( qx' J

8_F

i =- F .x+M. +-

(x')dx

El

I I

2

58

8 == qa :Fj 8EI

58

8 ;::;

Fa4

:fj 8WE]

58

8B =

2(0

:Fj

)

= 4WEI

Fa4

58

58

TANCHEW PHENGMechEns.USM06' - XXVll

-

(28)

Listofequations

Equation

4.14

p2a3

58

Ge-- c 2tWEI

Equation

4.15

1 =

t(L/2)3

59

12

Equation

4.16 Fe =

Aars

59

=(W-a)tars

Equation

4.17

a3 (W _a)2

f 2 59

Ge

= (J'rs

2WEI

Equation

4.18

Ke =JGeE'

59

=W'[(; r -(; rl(;� r

u�

Equation

5.1

( o-i)

. d=NA 80

Equation

5.2

[::=}=[:�}A

81

o) -I

N) Equation

5.3a

0=0 i+o j+o.k=

(Xc)i+(Yc)j+(z,)k

81

x y

J(

XC

/ +(Yc )2 +(

Z,

)�

Equation

S.3b

_

'. '. .

_

(

-Xa

)i+(

-Ya

)j+{ -Za)k

81

l-lxl+1yJ+lzk-

2 2 .,

�(Xa) +(Yo) +(zoY

Equation

5.3c d=

d)+dyj+d;k

81

Equation

5.4

[

Ox,

-ix 0)'1 -iy

O"

-

i,

f' J [N, J

81 0x2 -

�x 0y2

-

ly

0,,

= i, d,

=

�' (A J

0x3 - Ix

0y]

-

iy

o., l:

d:

3

Equation

5.5

(

Ox,

-

�x

0,,

= i: J(d}( N, }AJ

81

0x2 - Ix 0:2 lz

d, Nz

Equation

5.6a .

(xc)i+(Zc)k

82

0=0xl+O.k- =

J(

XC

)2 +( Zc)2

TANCIIEWPHENGMechEng.USM 06' - XXVlll -

(29)

List ofequations

Equation

5.6b

Equation

5.7

Equation

5.8

Equation

5.9

Equation

5.10

Equation

5.11

Equation

5.12

Equation

5.13

Equation

5.14

Equation

5.15

Equation

5.16

Equation

5.17

82

PLD =

Lob}

-

Lrej

=0

84

86

d;:

_

Lsin¢

d( L(l-cos¢)

90

(O; -iJ(d;:)=(N){A)

o -i :;::

(zc)

_

(-za)

z z

J(Xc)2 +(zc)2 J(Xa)2 +(za)�

=cos

80

-

(

- cos

� )

91

91

91

d = NA

z

1+ cos

91

92

(sinO. +sinB,

cose;

+COSll.)(�:J =(N)(A)

92

92

dz = NA 2cos8

92

Equation

5.18a d. =

dx

cos

f3

+

d;

sin

fJ

93

Equation

5.18b

d..

=

-dx

sin

f3

+

dz

cos

f3

93

Equation

5.19

d;

=0 93

Equation

5.20 d, =

-dz tanfJ

93

TAN CHEW PHENGMcchEng.USM06' - XXIX -

(30)

LISI ofequations

Equation

5.21 d. 93

d,. ;:::_-_

cos

f3

Equation

5,22 NA 93

d.' ;:::

2cos()cos

p

Equation

5.23 Mx-x =F.x+MI 94

Equation

5.24

8Mx_x

94

--=x

of

Equation

5.25

0,

F =

;/ f (

Fx+

M;) (

x

)dx

94

Equation

5.26

F(L -0.015)3

94

b:F

=

3£1

Equation

5.27

Wt3

95

1=- 12

Equation

5.28a x'cos

Pimg

98

r=

X

Equation

5.28b

-f)

98

Amg

=tan X

Equation

5.29

d=,

=0 103

Equation

5.30

d;:::�

x 103

tan

f3

Equation

5.31

d,=�

r 103

sin

f3

Equation

5.32 d = NA 103

x

'

2cos()sin

fJ Equation

5.33

d,= N 104

x

0.7644x

106 Equation

5.34

C= ae

(8 )

108 aL o

TANCHEWPHENGMechEng,USM 06' - XXX-

(31)

\ 1"11,'�

PENGUKURAN KEKUATAN PATAH DALAM PAKEJ PBGA DENGAN MENGGUNAKAN KAEDAH UNSUR TERHINGGA DAN EKSPERIMEN

ABSTRAK

Pakej

elektronik

khususnya jenis 'plastic

ball

grid array' (PBGA) mempunyai kegagalan

retakan dalaman yang unik yang berlaku disebabkan proses memateri.

Kewujudan kelembapan setempat

yang meresap ke dalam

pakej menghasilkan

tekanan wap. Semasa proses memateri

Jenis

aliran

(215°C), kelembapan

yang meresap akan mengewap dan kemudian

mengakibatkan

retakan

'popcorn'.

Oleh

itu,

kaedah

berangka diperlukan

untuk

memperihalkan rintangan patah

dalam bentuk faktor keamatan

tegasan (SI F) geometri. Kemudian, kajian

ke atas kekuatan

patah

bahan

epoksi

sebatian

acuan

(EMC)

menentukan keadaan

sempadan

untuk retakan

pakej,

Dalam

kajian ini, perisian Ansys

telah

digunakan

untuk melakukan

simulasi taburan

kelembapan

dan terma demi menentukan tekanan wap

pada bahagian

retak.

Daya

tekanan wap ini ditindak ke atas PBGA untuk

memperolehi

SIF

geometri dengan

penggunaan kaedah

penutupan

retak terubahsuai

(MCCI). Didapati

bahawa kenaikan tekanan wap dan

penambahan

saiz

lekangan menghasilkan

SIF

geometri

yang

tinggi. Perhubungan daya- pemanjangan

celah retakan yang

diperolehi

menerusi kaedah

holoqrafik

interferometri

(HI)

dan

daya

kritikal D.E.R. 331

sebagai

EMC telah

digunakan

untuk menganggar kekuatan

patah.

Kekuatan

patah

D.E.R 331 ialah 0.488MPa

Akhirnya,

kekuatan

patah

D.E.R. 331 ini telah

dibandingkan dengan

SIF

geometri

untuk PBGA. Graf

menunjukkan pelbagai

keadaan

sempadan

1·\ '\('IIIW1'111.N(j Mcch1·:Il�.LJS,\.1 0(,' - XXXI -

(32)

selamat

pakej

telah

diperolehi. Daripada graf ini,

boleh

disimpulkan

bahawa

PBGA masih selamat semasa proses

memateri,

iaitu tekanan wap 1.21MPa dan nisbah

lekangan kurang daripada

0.6.

Kegagalan pakej

elektronik ini

dapat

dikawal

dengan

pengurangan kesan tekanan wap dan

lekangan

antara

permukaan chip

dan EMC.

- XXXII -

(33)

DETERMINATION OF FRACTURE TOUGHNESS IN PBGA PACKAGES USING FINITE ELEMENT AND EXPERIMENTAL METHODS

ABSTRACT

Electronic

packages especially

the

plastic

ball

grid

array

(PBGA)

has its

unique

crack failure

arising

from the

soldering

process. The existence of moisture absorbed in

package

from ambient condition causes vapor pressure.

During

reflow

soldering

processes

(215°C),

the moisture absorbed

vaporizes

and

eventually

causes popcorn

cracking. So,

numerical method is used to

characterize the fracture resistance in terms of

geometric

stress

intensity

factor

(SIF). Then,

the

investigation

of fracture

toughness

on epoxy

molding compound (EMC)

material

provided boundary

conditions of

package cracking.

In this

research, Ansys

software was used to simulate moisture diffusion and thermal transfer to determine the vapor pressure at the crack

region.

The

vapor pressure

loading

was

applied

on PBGA to obtain

geometric

SIF

using

modified crack closure

integral (MCCI)

method. It was found that the increased in vapor pressure and

higher

delamination size created

high geometric

SIF.

Load-crack

edge

extension relation obtained from

holographic interferometry (HI)

method and critical load for D.E.R. 331 as EMC material were used to evaluate fracture

toughness.

The fracture

toughness

for D.E.R 331 was found

to be 0.488MPa m

1/2.

Eventually,

the fracture

toughness

for D.E.R. 331 was

compared

with

PBGA's

geometric

SIF. A

graph

with

package safety

conditions was obtained.

From the

graph,

it can be concluded that the PBGA is

typically

to be saved

during soldering

process, where vapor pressure is 1.21MPa and delarnmatron

I \, {III \\ PIli N{I Mcch I II!,:. llSM (lCl' - XXXlIl -

(34)

Abstract

ratio is less than 0.6. This EP's failure can be controlled

through minimizing

the

effect

of

vapor pressure

and reducin_g die/EMC interface

delamination.

TAN ('I mw I'III�NQM.:�hEna.USM 06' - XXXIV-

(35)

ChapterI

CHAPTER 1

INTRODUCTION

1.1

Background

of research

Electronic

packaging (EP) designing

and

manufacturing

tend to become

a

challenging global industry.

The

challenges emphasize

on

making

the EP

lighter, higher packaging density (miniaturization)

with the

complexity

in

functions and increased electrical

performance

while the cost remains at low

level.

However,

these

challenges

of

packaging

are hard to achieve and

bring

difficulties in

processing, handling

and

understanding

of smaller

components particularly

with the use of thinner dies. The matter

arising

now is how to

produce

a

high reliability

EP.

Higher density

and more

compact developed systems

are

turning

the

manufacturers to surface mount

technology (SMT)

which needs full concern of failure mechanism inside

plastic package

which is known as popcorn

cracking.

The

package

is

highly

sensitive to moisture and

humidity

conditions. Its

applications mostly

include consumer

electronics,

household

appliances, computing, automotive, telecommunications, flight control, robotics, military equipments

and astronautics.

Plastic failure

usually happens

when the moisture diffused in the

package during storage

becomes

vaporized

and exerts a pressure known as vapor pressure that could result in the popcorn effect.

Wong,

E.H. et al.

(1998)

found that vapor pressure is

responsible

for the eventual popcorn

cracking

of

plastic integrated

circuit

(Ie) packages during soldering

process.

Tay,

A.A.D. et al.

(1994)

mentioned that

during soldering by

vapor

phase

reflow

(VPR)

or infrared

(IR)

reflow

(Figure 1.1)

or wave

soldering techniques.

TANCHEW PHENG MechEng.USM 06' - l -

(36)

Chapter I

the EP is heated up to solder

melting temperature

in the

region

of

215°C

and

exposed

to humid environment.

High

thermal stresses were induced within the EP as the result of enhanced thermal mismatch between dissimilar materials.

Meanwhile,

the

evaporation

of moisture caused

high

stress

typically

between

molding compound (MC)

and

chip

interfaces. These stresses

mainly

contributed to the

phenomenon

of

cracking

inside the EP

especially

the

plastic

ball

grid

array

(PBGA) during

the reflow

soldering

process.

250--�---/---�-,---�

o T:

nl.l\.=24S0C±SOC

200 Tr=183°C 's=70s

Q)

- - - - - - - - - - - - - - - - - -

'-

:J Rampup

ro"- ISO Ramp down

2-30C/S/

el)

c.. 2�3°C/s

E

2O)c:: 100

�, /

'i::el)

/

Dry-out Reflow

-o i Pre-heat

C<n 50

) Ambientcondition Cooling

o 2SoC

Cl)

O

a::::

O 60 120 180 240 300

�oldering time, ts (s)

Figure

1.1: IR reflow

soldering profile (OSRAM catalog, 2006, p.97)

From these

circumstances,

it is

important

to

study

the micro mechanics of interface delam ination and popcorn

cracking.

Pa

rk,

Y. B. et al.

(1997)

noted

that the popcorn

cracking phenomenon

inside the surface mounted

packages

was known

by assuming

an inherent

edge

crack at die

pad/epoxy molding compound (EMC)

interface and

subsequently

interface delamination under thermal arid vapor pressure

loadings. According

to<

Rujukan

Outline

DOKUMEN BERKAITAN

The measured results of the commercial fountain solution using IPA show the similar wettability of CTP Kodak offset plate (see in Figure 5). This behavior of the CTP Kodak

Linear elastic fracture mechanics (LEFM) crack orientation is modelled with the finite element method in SENT model considering its geometry functions a/W ratio

Figure 5 shows the 2 and 3-parameter Weibull distribution for strain and strain and Young's modulus of untreated flax fibers treated at different concentrations of NaHCO 3..

Figure 5- 4 The name of different data source to handle query request 45 Figure 5- 5 The name of the analysis file in the server 45 Figure 5- 6 Different kind of panels in

Conclusions This paper presents finite element simulations of mixed-mode fatigue crack propagation in 2D problems based on linear elastic fracture mechanics by adopting the

At different composition of CO 2 in methane, there is variation in mass fraction in the axial and radial direction within the flame as shown in Figure 5.. The

Table 5 shows the comparison of runoff volume and peak flow reduction from different literature source at different location and Figure 5 shows the graph comparison of maximum range

Figure 6.4 Flexural crack propagation at rail seat under static load 241 Figure 6.5 Load-deflection relationship of HSC sleepers 245 Figure 6.6 Stress-strain behaviour of