size effect and geometrical effect of solids in micro-indentation test.pdf

12
ACTA M ECHANICA SINICA (English Series), Voi.19, No.l,February 2003 The Chinese Society of Theoretical and Applied M echanics Chinese Journal of Mechanics Press, Beijing, China Allerton Press, INC., New York, U.S.A. ISSN 0567-7718 SIZE EFFECT AND GEOMETRICAL EFFECT OF SOLIDS IN MICRO -I NDENTA TION TEST* WEI Yueguang (~f-)t WANG Xuezheng (~!~) ZHAO Manhong (NN~) CHENG Che-Min (~g~) BAI Yilong (~t~;~) (LNM, Institute of Mechanics, Chinese Academy of Sciences, Beijing 100080, China) ABSTRACT: Micro-indentation tests at scales of the order of sub-micron show that the measured hardness incr eas es strongly with decreasing indent depth or indent size, which is frequently referred to as the size effect. At the same time, at micron or sub-micron sc ale , another effect, which is referred to as the geometrical size effects such as crystal grain size effect, thin film thickness effect, etc., also inf luences the measured material hardness. Howeve r, the trends are at odds with the size-independence implied by the conventional elastic-plastic theory. In the present research, the strain gradient plasticity theory (Fleck and Hutchinson) is used to model the composition effects (size effect and geometrical effect) for polycrystal material and metal thin film/ceramic substrate systems when materials undergo micro-indenting. The phenomena of the "pi le- up" and "sink-in" appeare d in the indentation test for the poly crysta l materials are also discussed. Meanwhile, the micro -indent ation experiments for the polycrystal A1 and for the Ti/SisN4 thin film/substrate system are carried out. By comparing the theoretical predictions with experimental measurements, the values and the variation trends of the micro-scale parameter included in the strain gradient plasticity theory are predicted. KEY WORDS: micro-indentation tests, size effect, geometrical effect, strain gradient plasticity 1 INTRODUCTION Indentation test is an important and effective experimental method, and has been used extensively to estimate the plastic properties of solids undergoing plastic deformation. Through indentation test, the loading-unloading relation between hardness and in- dent depth is measured. Thereby, the material pa- rameters, such as the yielding stress, strain hard- ening exponent, Young's modulus, etc. are esti- mated. Recently, with the advancement of experi- mental technique and measuring precision, it is pos- sible to carry out the indentation tests at the scale of one micron or sub-micron for obtaining more de- tailed material information. Such small-scale indenta- tion experiments are frequently referred to as micro- indentation tests (or nano-indentation tests). In the micro-indentation test, new results, different from the conventional ones, the size-dependent results, were obtained extensively [1~9]. For metal materials, the measured hardness may double or even triple the Received 3 0 April 2001, revised 29 October 2001 conventional hardness as the indent size (or depth) decreases to a fifth micron. The effect is often re- ferred to as the size effect. In addition, at the micron scale, if material is of some micro-geometrical struc- tures and if the geometrical structure size is compara- ble to the indent depth, the size-dependent hardness mentioned above may be influenced additionally by the geomet rica l size. We call this effect as the geo- metrical effect in the present research. However, the trends of both size effect and geometrical effect are at odds with the size-independence implied by the conventional elastic-plastic theory. Otherwise, from a dimensional consideration [1~ the hardness was only dependent of macroscopic parameters of material, i.e., was size-independent. In order to predict the size effect phenomena, re- cently, several strain gradient plasticity theories have been developed [n~13]. These theories include the strain gradient effects and go beyond the conventional elastic-plastic theo ry frame. In the new constitutive * The project supported by the National Natural Science Foundation of China (19891180 and 19925211) and Bai Ren Plan o f CAS t E-maih [email protected]

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Page 1: Size effect and geometrical effect of solids in micro-indentation test.pdf

7/29/2019 Size effect and geometrical effect of solids in micro-indentation test.pdf

http://slidepdf.com/reader/full/size-effect-and-geometrical-effect-of-solids-in-micro-indentation-testpdf 1/12

AC TA M EC HA NIC A SINICA (Eng li sh Ser ies ) , Vo i .19, N o. l ,Februa ry 2003

Th e Chinese Society of Theoret ical a nd Appl ied M echanics

Chinese Journal o f M echanics Press, Bei j ing, China

Al lerton Press, INC., New York, U .S.A.

ISSN 0567-7718

S I Z E E F F E C T A N D G E O M E T R I C A L E F F E C T O F S O L I D S

I N M I C R O - I N D E N T A T I O N T E S T *

WEI Yueguang (~f -) t WANG Xuezheng (~! ~) ZHAO Manhong (N N~)

CHENG Che-Min (~ g~ ) BAI Yilong (~t~;~)

(LNM, Institute of Mechanics, Chinese Academy of Sciences, Beijing 100080, China)

A B S T R A C T : Micro-indentation tests at scales of the order of sub-micron show that the measured

hardness increases strongly with decreasing indent depth or indent size, which is frequently referred to

as the size effect. At the same time, at micron or sub-micron scale, another effect, which is referred

to as the geometrical size effects such as crystal grain size effect, thin film thickness effect, etc., also

influences the measured material hardness. However, the trends are at odds with the size-independence

implied by the conventional elastic-plastic theory. In the present research, the strain gradient plasticity

theory (Fleck and Hutchinson) is used to model the composition effects (size effect and geometrical

effect) for polycrystal material and metal thin film/ceramic substrate systems when materials undergo

micro-indenting. The phenomena of the "pile-up" and "sink-in" appeared in the indentation test for

the polycrysta l materials are also discussed. Meanwhile, the micro-indentation experiments for the

polycrystal A1 and for the Ti/SisN4 thin film/substrate system are carried out. By comparing the

theoretical predictions with experimental measurements, the values and the variation trends of the

micro-scale parameter included in the strain gradient plasticity theory are predicted.

KEY WORDS: micro-indentation tests, size effect, geometrical effect, strain gradient plasticity

1 INTRODUCTION

Indentation test is an important and effective

experimental method, and has been used extensively

to estimat e the plastic pro perties of solids undergoing

plastic deformation. Throu gh indentation test, the

loading-unloading relation between hardness and in-

dent depth is measured. Thereby, the material pa-

rameters, such as the yielding stress, strain hard-

ening exponent, Young's modulus, etc. are esti-

mated. Recently, with the advancement of experi-

mental technique and measuring precision, it is pos-sible to carry out the indentation tests at the scale

of one micron or sub-micron for obtaining more de-

tailed material information . Such small-scale indenta-

tion experiments are frequently referred to as micro-

indentation tests (or nano-indentation tests). In the

micro-indentation test, new results, different from the

conventional ones, the size-dependent results, were

obtai ned extensively [1~9]. For metal materials, the

measured hardness may double or even triple the

Received 30 April 2001, revised 29 October 2001

conventional hardness as the indent size (or depth)decreases to a fifth micron. The effect is often re-

ferred to as the size effect. In addition, at the micron

scale, if material is of some micro-geometrical struc-

tures and if the geometrical structure size is compara-

ble to the indent depth, the size-dependent hardness

mentioned above may be influenced additionally by

the geomet rica l size. We call this effect as the geo-

metrical effect in the present research. However, the

trends of both size effect and geometrical effect are

at odds with the size-independence implied by the

conventional elastic-plastic theory. Otherwise, from adimensional consi deration [1~ the hardnes s was only

dependent of macroscopic parameters of material, i.e.,

was size-independent.

In order to predict the size effect phenomena, re-

cently, several strain gradient plasticity theories have

been developed [n~13]. These theories include th e

strain gradient effects and go beyond the conventional

elastic-plastic theo ry frame. In the new constitu tive

* The project supported by the National Natural Science Foundation of China (19891180 and 19925211) and Bai Ren Plan ofCAS

t E-maih [email protected]

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7/29/2019 Size effect and geometrical effect of solids in micro-indentation test.pdf

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6O

r e l a ti o n s , t h e s t r a i n t e r m s a r e m a t c h e d w i t h t h e n e w

s t r a i n g r a d i e n t t e r m s t h r o u g h s e v e r a l l e n g t h p a r a m e -

t e rs . T h u s t h e m a t e r i a l s iz e e f fe c t c a n b e c h a r a c t e r -

i z e d b y t h e l e n g t h - s c a l e p a r a m e t e r s .

O n t h e r e s e a r c h e s o f t h e s i ze e ff e c t i n t h e i n d e n -

t a t i o n t e s t s b y u s i n g st r a i n g r a d i e n t p l a s t i c i ty t h e o -r i es , in R e f .[ 4 ], t h e c a s e w h e n t h e m i c r o - s c a l e p a r a m e -

t e r w a s s m a l l e r t h a n t h e c o n t a c t r a d i u s w a s a n a l y z e d

b y a d o p t i n g t h e c o u p l e s t r e s s t h e o r y I n ] u n d e r a n i n -

c o m p r e s s i b l e a s s u m p t i o n . I n R e f. [3 ] , t h e s i m i l a r c a se

t o [ 4] b u t a d o p t i n g t h e F l e c k a n d H u t c h i n s o n ' s s t r a i n

g r a d i e n t p l a s t i c i t y [11] w a s a n a l y z e d . B y a p p l y i n g t h e

p r e d i c t i o n r e s u l t t o t h e m i c r o - i n d e n t a t i o n t e s t f o r m a -

t e r ia l t u n g s t e n ( W ) I s] , t h e m i c r o - s c a l e p a r a m e t e r f o r

m a t e r i a l W w a s o b t a i n e d w i t h i n 0 . 2 5 ~ 0 .5 2 p m .

A l t e r n a t i v e l y , a d i s lo c a t i o n m o d e l h a s b e e n u s e d

t o s t u d y t h e s i z e e f fe c t f o r t h e m i c r o - i n d e n t a t i o n t e s t

i n R e f. [1 ] . B y u s i n g t h e T a y l o r ' s r e l a t i o n , y o n M i s e s '

p l a s t ic f l o w la w a n d t h e c o n v e n t i o n a l r e l a t i o n o f t h e

h a r d n e s s ( t r i p l e t h e f lo w s t r e s s ) , a n i n v e r s e s q u a r e

r o o t r e la t i o n b e t w e e n h a r d n e ss a n d i n d e n t d e p t h w a s

o b t a i n e d .

C o m p a r i n g t h e m i c r o - i n d e n t a t i o n t e s t re s u l t s f o r

c o n v e n t i o n a l m e t a l s ( C u , A g , A 1 ) [2,7 '91 w i t h t h a t f o r

t h e u n i q u e l y h i g h m o d u l u s m e t a l W [ s] , i t i s c l e a r t h a t

t h e s e n s i t i v e z o n e s c a l e o f t h e s i ze e f f e ct o f t h e f o r -

m e r is sm a l l e r t h a n t h a t o f t h e l a t t e r f o r a n o r d e r

o f m a g n i t u d e . C o r r e s p o n d i n g l y , t h e s c al e o f t h e c o n -

t a c t r a d i u s o f t h e f o r m e r is al s o s m a l l e r t h a n t h a t o f

t h e l a t t e r f o r a n o r d e r o f m a g n i t u d e . F u r t h e r m o r e ,

i n v i e w o f t h e p r e v i o u s i n v e s t i g a t i o n s [ 3 ,4 ] w h i c h w e r e

f o c u s e d o n t h e c a s e w h e n t h e m i c r o - s c a l e p a r a m e t e r

w a s s m a l l e r t h a n t h e c o n t a c t r a d i u s , i t is n e c e ss a r y

t o d i s c u s s t h e c a s e w h e n t h e m i c r o - s c a l e p a r a m e t e r

i s g r e a t e r , e v e n s e v e r a l t i m e s g r e a t e r t h a n t h e c o n -

t a c t r a d i u s f o r t h e c o n v e n t i o n a l m e t a l s ( C u , A g , A 1,

e t c . ). F o l l o w i n g [ 9 ] , i n t h e p r e s e n t r e s e a r c h , t h e F l e c k

a n d H u t c h i n s o n ' s s t r a i n g r a d i e n t p l a s t i c i ty m o d e l [11],

a n d a c o m p r e s s i b l e g e n e r a l c o n s t i t u t i v e r e l a t i o n a r e

c o n s i d er e d . E x p e r i m e n t a l r e se a r c h e s o f t h e m i c r o -

i n d e n t a t io n t e s ts f o r p o l y c r y s t a l a l u m i n u m a n d t h e

m e t a l t h i n f i l m / c e r a m i c s u b s t r a t e s y s t e m a r e c a r r i e d

o u t . F o r t h e p o l y c r y s t a l A1 , t h e e x p e r i m e n t a l p r o -

g r a m m i n g a d o p t e d h e r e is d i f fe r e n t f r o m t h e c o n v e n -

t i o n a l c o n t i n u u m s t i ff n e ss m e t h o d ( C S m e t h o d ) , a n d

t h e m e a s u r e d h a r d n e s s c u r v e is b a s e d o n a u n i q u e

l o a d i n g p o i n t o n t h e s u r f a ce , a n d d e p e n d s o n t h e s t a -

t u s o f t h e l o a d i n g p o i n t . I n t h e p r e s e n t e x p e r i m e n t ,

m a n y l o a d i n g p o i n t s a r e se l e c te d r a n d o m l y , a n d o n e

t e s t p o i n t c o r r e s p o n d s t o o n l y o n e m e a s u r e d v a l u e fo r

h a r d n e s s / d e p t h r e l a t io n . A l t h o u g h a d a t a s tr i p f o r

A C T A M E C H A N I C A S I N I C A ( E n g li sh S e rie s ) 2 0 03

h a r d n e s s / d e p t h r e l a t i o n w il l b e o b t a i n e d b y u s i n g t h e

C S m e t h o d , i t s d e f e c ts c a n b e a v o id e d . B y c o m p a r -

i n g t h e t h e o r e t i c a l p r e d i c t i o n w i t h t h e s t r i p t e s t d a t a ,

t h e m i c r o - s c a l e p a r a m e t e r a n d i t s v a r i a t i o n t r e n d s f o r

d i f fe r e n t m a t e r i a l c a n b e p r ed i c t e d . F o r c o m p a r i s o n ,

i n t h e i n d e n t a t i o n e x p e r i m e n t f o r t h e T i / S i 3 N 4 , a

t h i n f i l m / s u b s t r a t e s y s t e m , t h e C S m e t h o d w i ll b e

a d o p t e d . T h r o u g h c o m p a r i n g t h e t h e o r e t i c a l p r e d i c -

t i o n s w i t h t h e e x p e r i m e n t a l r e s u l ts , t h e v a l u e s a n d t h e

v a r i a t i o n t r e n d s o f t h e m i c r o - s c a l e l e n g t h p a r a m e t e r

f o r d i f fe r e n t m a t e r i a l , r e l a t e d w i t h m i c r o - g e o m e t r i c a l

s i z e , a r e p r e d i c t e d .

2 D E F O R M A T I O N A L T H E O R Y O F S T R -

A I N G R A D I E N T P L A S T I C I T Y

I n t h e p r e s e n t s e c t i o n , t h e . c o m p r e s s i b l e g e n e r a l

f o r m o f t h e d e f o r m a t i o n a l t h e o r y o f t h e s t r a i n g r a d i -e n t p l a s t i c i t y i s o u t l i n e d a s f o ll o w s .

2 .1 C o n s t i t u t i v e R e l a t i o n s

T h e d e f i n i ti o n s o f t h e s t r a i n a n d s t r a i n g r a d i e n t

a r e1 e e

e i j = ~ (u i , j + u s , i ) = c i j + ~ i ~( 1 )

e ~]p? ] i j k = U k , i j = ? ] i j k ~ - i j k

T h e e x p r e s s io n s r e l a t e d w i t h t h e c o n s t i t u t i v e r e l a t i o n s

a r e l i s t e d a s f o l l o w s

M g e 2 1W e E2 (1 + @ ( 1 - - 2 . ) k k + ~ 2 ( 1/ Q % ' e ' ~ +

-~Le2 e(I) e(1)'~I = 1 I ? ] i j k ~ ] i j k )

= ow~ . = owe/o, 5

2 , , ~ - ' , L 2 ( I ) ( I )= ~ g i j g i j ~ - ~ I ~ l i jk ? ~ i j k

/ = 1

I = 1

7 ( i )~ ( z )

i j k = A i j k l r n n ~ ] lr n n

p _ _ 3 0 J 2 3 ,

r 2 h e O G i j - 2 h e G i j

r i ( I ) = T ( I ) ~ -j k i j k l m n l m n

3p 3 O J e 1 V " r . - 2 ~ , ' ( z )

~ i j k - - 2hP O T ij k - - h P ~ I ~ij klmn TlrnnI = 1

h e -_ Z / ( Z - X / E )

( 2 )

w h e r e X a n d ~ a r e t h e e f f e c ti v e s t r e s s a n d e f f e c ti v e

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Vol.19, No.1 W ei Yu egu ang et al.: Size EfFect and Geometr ical Effect of Solids 61

s t r a i n , r e s p e c t i v e l y . L ~ a n d L I ( I = 1 , 4 ) a r e t h e

m i c r o - s c al e p a r a m e t e r s f o r t h e e l a st i c a n d p l a s t i c c a se ,

r e s p e c t i v e l y . F r b m t h e d i s c u s s i o n i n [ 1 1 ] , t h e r e e x i s t s

a g e n e r a l r e l a t i o n a m o n g t h e m i c r o - sc a l e s ( S G t h e o r y )

1 L L 3 = ( 3 )L1 = L L2 = 2

I n a d d i t i o n , t a k e L 4 = L / 2 . S i m i l a r l y , ( 3 ) i s v a l i d

a l s o f o r t h e e l a s t i c i t y s t r a i n g r a d i e n t c a s e , w i t h L re -

p l a c e d b y L ~ i n ( 3 ) . M o r e o v e r , t h e p r e v i o u s r e s e a r c h

h a s s h o w n t h a t t h e s o l u t i o n i s i n s e n s i t i v e t o t h e v a l u e

o f L ~ / L w i t h i n t h e r e g i o n 0 < L ~ / L < 1 [14] . T hu s ,

t a k e L ~ / L = 0 .5 in t h e p r e s e n t r e s e a r c h . I n t h e l a s t

r e l a t i o n o f ( 2 ) , h p i s t h e e f f e c t iv e p l a s t i c m o d u l u s .

C o n s i d e r i n g t h e s t r a i n h a r d e n i n g m a t e r i a l

= S o < _

( 4 )= ~--'0 (~ /C rY ) 1 /N ~ > O'y

w e h a v e

h P : E [ ( ~ / C r y ) l / N - l - 1 ] - i (5 )

T (I) ( f = 1 , 4 ) is t h e p r o j e c t i o nn f o r m u l a ( 2 ) , i jklm~

t e n s o r o f t h e s t r a i n g r a d i e n t, a n d t h e d e t a i l e d e x p r e s -

s i o n s a r e g i v e n i n [ 1 4 ] . T h u s , b y u s i n g t h e f o r m u l a s

( 1 ) a n d ( 2 ) a n d t h e p r o j e c t i o n t e n s o r n o r m a l i t y , t h e

c o m p r e s s i b l e g e n e ra l f o r m o f t h e d e f o r m a t i o n a l t h e o r y

o f t h e s t r a i n g r a d i e n t p l a s t i c i t y c a n b e e x p r e s s e d a sE

(7ij : ,:{ gi j@

1 + u + 2 E / h p

3 1 - 2 u l + u + ~ E / h P ](6 )

3

L ~

" I= 1 L ~ /L ~ 2 + 2 E / h P i j m , , ~ "

L e42Ti~21mn ?~lmn

2 . 2 E q u i l i b r i u m a n d V a r i a t i o n a l R e l a t i o n s

F r e q u e n tl y , e q u i l i b r i u m e q u a t i o n s c a n b e d e -

s c r i b e d b y th e d i s p l a c e m e n t - v a r i a t i o n a l r e l a t io n , f o r

t h e f in i te e l e m e n t i m p l e m e n t a t i o n . T h e d i s p l a c e m e n t -

v a r i a t i o n a l r e l a t i o n f o r th e s t r a i n g r a d i e n t p l a s t i c i t y

t h e o r y i s g i v e n b y Ira ]

/ v ( a~ jS c~ j + r ~ jk S ~ j k ) d V = f v f k S u k d V +

f s t k 6 u k d S + / ; r k ( D ~ u k ) d S (7 )

B a s e d o n ( 7 ) , t h e t r a c t i o n o n S i s d e f i n e d b y

0 i ; kt k = n i a i k O X j ] + n i n j w i j k ( D p n p ) -

D j (n i~ - ijk ) (8 )

a n d t h e s u r f a ce t o r q u e b y r k = n i n j T i j k . T h e o p e r a -

t o r s D a n d D j i n (7 ) a n d ( 8 ) a r e d e f i n e d as

D j = O / O x j - n j n k O / O X k D = n k O / X k (9 )

w h e r e n i i n ( 7 ) ~ ( 9 ) i s t h e d i r e c t i o n c o s i n e o n S .

3 P R O B L E M F O R M U L A T I O N S

3 . 1 B o u n d a r y C o n d i t i o n s o f I n d e n t a t i o n T e s t

P r o b l e m

C o n s i d e r t h a t t h e p r e s s u r e h e a d i s a c i r c u l a r

c o n e. T h e u s u a l p y r a m i d p r e s su r e h e a d c a n b e re -

p l a c e d a p p r o x i m a t e l y w i t h a c i r c u l a r c o n e a c c o r d i n g

t o t h e c r o s s - s e c t i o n a r e a e q u i v a l e n c e f o r s i m p l i f y i n g

t h e an a l y s i s. A t r a c t i o n c o n d i t i o n o n t h e r e m o t e

b o u n d a r y i s u s e d h e r e, i n s t e a d o f t h e d i s p l a c e m e n t

b o u n d a r y c o n d i t i o n s a s i s u s u a l l y d o n e . T h e a d v a n -

t a g e s o f s u c h a t r e a t m e n t a r e in e i t h e r c a t c h i n g t h e

f u n d a m e n t a l f e a t u r e o f i n d e n t a t i o n t e s t , o r m a k i n g

t h e d e s c r i p t i o n a n d a n a l y s i s m u c h s i m p l e r .

E l a s t i c s tr e s s d i s t r i b u t i o n s o n t h e r e m o t e b o u n d -

a r y a r e g i v e n b y ( s e e F i g . l ) [15]

Pcr~ -- 2 ~ 2 \ 1 - t- s in 0 3 cos 2 0 s in 0

3 P s in 3 0Cr z : - - 271 .~2

3 P ( 1 0 )

- - cos 0 s in 2 0~ r z - - 2 7 r f 2

( 1 - 2 u ) P ( s i n 0 1 )c ry - 2 - -- - 1 + s i n 0

w h e r e f 2 = r 2 + z 2 . T h e d e f i n i t i o n s o f t h e o t h e r s a r es h o w n in F i g .1 . T h e m i x e d b o u n d a r y c o n d i t i o n s o n

t h e m a t e r i a l s u r f a ce ( z = 0 ) fo r t h e s m a l l d e f o r m a t i o n

c a s e a r e

u z = - r t a n / 3 R r = 0

R z < 0 0 < r < R = h / t a n / 3 ( 1 1 )

R r = R z = 0 R < r

w h e r e t h e r e f e r e n c e ( o r i g i n a l ) p o i n t o f v e r t i c a l d i s -

p l a c e m e n t Uz i s c h o s e n a t t h e c o n i c a l a p e x , R i s t h e

c o n t a c t r a d i u s , h i s t h e p e n e t r a t i o n d e p t h o f t h e i n -

d e n t e r , R r a n d R z a r e t h e s u r f a ce t r a c t i o n s .

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62 A C TA ME C H A N IC A S IN IC A (E ng l i sh S e r i e s )

i N i i i : j , i N-*-~---- d ----~

N , L )

2003

Z ~3

r

Fig .1 S impl i fi ed mod e l fo r po lyc rys t a l ma te r i a l undergoing the m ic ro- indent

F o r t h e c o n v e n i e n c e o f t h e a n a l y s is , d e f in e a

l o a d i n g - l e n g t h p a r a m e t e r a s

R o = ~ / P / ( 3 ~ y ) (12)

R 0 i s t h e c o n v e n t i o n a l c o n t a c t r a d i u s ( w h e n t h e s i z e

e f f ec t i s n e g l e c t e d ) f o r t h e l o w - h a r d e n i n g m e t a l m a t e -

r i a l i n t h e c a s e o f f l a t p r e s s u r e h e a d [ 1 6] . T h e h a r d n e s s

d e f i n i t i o n a n d t h e r e l a t i o n s w i t h t h e g e o m e t r i c a l p a -

r a m e t e r a n d i n d e n t d e p t h a r e

P - - 3c ry = 3Cry t an /3 (13)H -- 7rR~

3 . 2 P o l y c r y s t a l M a t e r i a l U n d e r g o i n g t h e

M i c r o - I n d e n t

C o n s i d e r a p o l y c r y s t a l m a t e r i a l w h o s e c r y s t a l

g r a i n si ze i s c o m p a r a b l e w i t h th e i n d e n t d e p t h . I n

t h i s c a se , t h e g e o m e t r i c a l e f f ec t o n t h e h a r d n e s s m u s t

b e c o n s id e r e d . W h e n t h e p r e s s u r e h e a d is a p p l i e d

t o a c r y s t a l g r a i n o n t h e m a t e r i a l s u r f a c e , t h e p l a s -

t i c s li p z o n e w i ll b e c o n s t r a i n e d t o t h e r e g i o n o f t h e

c r y s t a l g r a i n u n t i l t h e p r e s s u r e h e a d a p p r o a c h e s t h e

g r a i n b o u n d a r y , d u e t o t h e s h i e l d i n g e f f ec t o f t h e g r a i n

b o u n d a r y . E f f e c t s o f a l l o t h e r c r y s t a l g r a in s c a n b e

a p p r o x i m a t e l y d e s c r i b e d b y a n e l a s ti c al l y a n d h o m o -

g e n e o u s ly e q u iv a l e nt b o d y w i t h Y o u n g ' s m o d u l u s a n d

P o i s s o n ' s r a t i o ( E s , u s ) b y u s i n g t h e H i l l' s c o n s i s t e n t

a p p r o a c h [ 1 7 1 . T h e e q u i v a l e n t Y o u n g ' s m o d u l u s v a l u e

E s f o r th e p o l y c r y s t a l m a t e r i a l i s s m a l l e r t h a n E , t h e

e q u i v a l e n t Y o u n g ' s m o d u l u s o f t h e s in g l e c r y s t a l m a -

t e r i a l. T h e s im p l i f ie d m o d e l f o r p o l y c r y s t a l m a t e r i a l

u n d e r g o i n g a m i c r o - i n d e n t i s s h o w n i n F i g . 1 . t i s t h e

c r y s t a l g r a i n s i ze i n t h e i n d e n t d i r e c t io n , d i s a n o t h e r

s i ze o f t h e c r y s t a l g r a i n .

I n a l l r e l a t i o n s g i v e n a b o v e , a l l p a r a m e t e r s o r

v a r i a b l e s w i t h l e n g t h d i m e n s i o n c a n b e n o r m a l i z e d b y

R 0 , a n d a l l q u a n t i t i e s w i t h s t r e s s d i m e n s i o n c a n b e

n o r m a l i z e d b y ~ y , s u c h th a t t h e n o r m a l i ze d h a r d n e s s

c a n b e t a k e n t o b e a f u n c t i o n o f t h e i n d e p e n d e n t a n d

n o n - d i m e n s i o n a l p a r a m e t e r s a s f o l l o w s

H f (E _ _ y E s L t d ) ( 1 4 )~ y ' E ' u , u s , N , / 3 , R 0 R 0 '

w h i l e c o n t a c t r a d i u s a n d i n d e n t d e p t h a r e r e l a t e d t o

t h e h a r d n e s s b y ( 1 3) . T h e d e t a i l e d e x p r e s s i o n o f (1 4 )

w i l l b e i m p l e m e n t e d b y s o l v i n g t h e i n d e n t a t i o n p r o b -

l e m n u m e r i c a l l y , u s i n g t h e s t r a i n g r a d i e n t p l a s t i c i t y

t h e o r y .

3 .3 T h i n F i l m / S u b s t r a t e S y s t e m U n d e r g o i n g

t h e M i c r o - I n d e n t

A d d i t i o n a l l y , c o n s i d e r a m e t a l t h i n f i l m / c e r a m i c

s u b s t r a t e s y s t e m u n d e r g o i n g t h e m i c r o - i n d e n t o n t h e

s u r f a c e o f a t h i n f i lm . W h e n t h e t h i c k n e s s o f t h e t h i nf i lm is c o m p a r a b l e w i t h t h e i n d e n t d e p t h , t h e e f f e ct

o f t h e g e o m e t r i c a l si ze o n t h e h a r d n e s s m u s t b e c o n -

s i d e r e d . I n t h i s c a s e , t h e h a r d n e s s - p a r a m e t e r r e l a t i o n

c a n b e w r i t t e n a s

g f u , u s , N , / 3 , - - ( 1 5 )c ry E R0

w h e r e t is t h e t h i n f i l m t h i c k n e s s , E s i s Y o u n g ' s

m o d u l u s o f t h e s u b s t r a t e m a t e r i a l . F o r m e t a l t h i n

f i l m / c e r a m i c s u b s t r a t e s y s t e m , u s u a ll y , E s / E ~ 6 .S i m p l if i ed m o d e l f o r t h i n f i l m / s u b s t r a t e s y s t e m m l -

d e r g o i n g t h e m i c r o - i n d e n t i s s h o w n i n F i g . 2 .

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Vol.19, N o. l We i Yueguang et al,: Siz e Effect and Geom etr ical Effect of Solids

: : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : : :::::::::::::::::::::::::::::::::::::::::::::::::::::::::ir

subs t r a te

N , L )

: : : : : : : : : : : : : : : : : : : : : : : : : :

i i ' , i i i i i H i i i i i ! i i i i : i i i i i i i '' ' ' ii ! i i i i i i i i i i i i l

F i g .2 S i m p l if i ed m o d e l f o r t h e m e t a l t h i n f i l m / c e r a m i c s u b -

s t r a t e s y s t e m u n d e r g o i n g th e m i c r o - i n d e n t

63

4 F I N I T E E L E M E N T M E T H O D F O R T H E

D E F O R M A T I O N A L T H E O R Y O F T H E

S T R A I N G R A D I E N T P L A S T I C I T Y

F o r t h e c o n s t i t u t i v e r e l a t i o n t h a t t a k e s a c -

c o u n t o f t h e s t r a i n g r a d i e n t e f f e ct , g e n e r a l l y s p e a k -

i n g , t h e c o n v e n t i o n a l f i n i t e e l e m e n t m e t h o d c a n

n o t b e u s ed , a n d a s p e c i a l f i n i te e l e m e n t m e t h o d

w i t h t h e d i s p l a c e m e n t d e r i v a t i v e s a s t h e n o d a l

v a r i a b l e s i s n e e d e d [ 1 3 '1 s ' 1 9 ]. H o w e v e r , f o r t h e

s t r e t c h i n g - d o m i n a t e d s t r a i n g ra d i e n t p l a s t i c i ty p r o b -

l e m , o n e c a n o b t a i n a n e f f ec t iv e r e s u l t b y a d o p t i n g

t h e i s o - p a r a m e t r i c d i s p l a c e m e n t e l e m e n t w i t h n i n e

n o d e s [1 4'1 9'2 ~ O b v i o u s l y , t h e i n d e n t a t i o n p r o b l e m

is s t r e t c h i n g - d o m i n a t e d . T h e r e f o r e , i n t h e p r e s e n t

a n a l y s i s , s u c h a n e l e m e n t w i ll b e u s e d . I n a d d i t i o n ,

2 • 2 G a u s s i n t e g r a t i o n p o i n t s a r e a d o p t e d f o r e a c h

e l e m e n t .

F o r t h e a x i s y m m e t r i c a l p r o b l e m o f i n d e n t a t io n

t e s t , c o n s i d e r t h a t t h e e l a s t i c s t r e s s f i e l d a c t s o n t h e

r e m o t e b o u n d a r y , a n d t h e p r e s s u r e h e a d a p e x i s t a k e n

a s t h e r e f e r e n c e p o i n t ( z e ro p o i n t ) o f v e r t i c a l d i s p l a c e -

m e n t . T h u s , i m a g i n e t h a t u n d e r t h e a c t io n o f t h e

r e m o t e s t r e s s fi el d, m a t e r i a l w o u l d m o v e b a c k t o t h e

p r e s s u r e h e a d s u r f a c e , n e a r t h e a p e x , m a t e r i a l w o u l d

c o n t a c t w i t h c o n i c a l s u r f a c e , a n d t h e c o n t a c t r a d i u s

w o u l d b e e q u a l to R . T h e d i s p l a c e m e n t c o n s t r a i n t c o n -

d i t i o n s i n t h e c o n t a c t r e g i o n a r e d e s c r i b e d b y ( 1 1 ) .

U s i n g t h e p l a s t i c d e f o r m a t i o n a l t h e o r y , t h e s o -

l u t i o n p r o c e d u r e s c a n b e o u t l i n e d a s f o ll o w s . F i r s t ly ,

c a l c u l a t e t h e e l a s t ic s o l u t io n . S e c o n d l y , t a k i n g e l a s-

t i c s o l u t i o n a s t h e i n i t i a l t r i a l , f i n d t h e s o l u t i o n f o r

t h e h i g h e r - h a r d e n i n g m a t e r i a l b y it e r a t in g . T h i r d l y ,

t a k i n g t h e l a s t s o l u t i o n a s t h e n e w i n i t i a l t r i a l , f i n d

t h e c o n v e r g e n t s o l u t io n f o r t h e l o w e r - h a rd e n i n g m a -

t e r i a l ca s e b y i t e r a t i n g . F o r e x a m p l e , t h e s o l u t i o n

p r o c e d u r e s f o r N - - 0 .1 c a s e a r e d e s c r i b e d a s fo l lo w s .

F i r s t l y , f i n d i n g t h e e l a s t i c s o l u t i o n a n d t h e n t a k i n g i t

a s t h e i n i t i a l s o l u t i o n , c a l c u l a t e t h e c o n v e r g e n t s o l u -

t i o n f o r N = 0 . 3 c a se b y i te r a t i n g . S e c o n d l y , t a k i n g

t h e l a s t s o l u t i o n ( N = 0 . 3 ) a s a n e w i n i t i a l t r i a l , f i n d

t h e c o n v e r g e n t s o l u t i o n f o r t h e c a s e o f N = 0 .2 b y

i t e r a t i n g . F i n a l l y , b a s e d o n t h e s o l u t i o n o f N = 0 . 2 ,f i n d t h e c o n v e r g e n t s o l u t i o n f o r N = 0 .1 b y i t e r a t i n g .

F o r t h e t r u e c a s e o f t h e m i c r o - i n d e n t a t i o n t e s t

p r o b l e m , t a k e t h e r e m o t e b o u n d a r y a s t h e r e f e r e n c e

p o i n t o f v e r t i c a l d is p l a c e m e n t . T h u s , t h e v e r t i c a l d is -

p l a c e m e n t f i e l d c a n b e e x p r e s s e d b y

v ( r , z ) = u z ( r , z ) - u 7 ( 16 )

w h e r e u ~ i s t h e v e r t i c al d i s p l a c e m e n t a t t h e r e m o t e

b o u n d a r y f o r c a s e w h e n t h e c o n i c a l a p e x i s d e f in e d

a s t h e r e fe r e n c e p o i n t o f v e r t i c a l d i s p l a c e m e n t . T h e

f o r m o f f i n it e e l e m e n t m e s h a d o p t e d i n th e p r e s e n t r e -s e a rc h i s s i m p l y f a n - s h a p e d u s i n g t h e a x i s y m m e t r i c a l

c o n d i t i o n .

5 N U M E R I C A L A N D E X P E R I M E N T A L

R E S U L T S F O R P O L Y C R Y S T A L M A -

T E R I A L

5 .1 N u m e r i c a l R e s u l t s

I n t h e n u m e r i c a l a n a l y s e s f o r t h e c o n v e n t i o n a l

m e t a l m a t e r i a ls , m a t e r i a l p a r a m e t e r s a r e t a k e n a s

( E / ~ y , ~ , N ) = ( 30 0 , 0 .3 , 0 .1 ) a n d th e f ia t p r e s s u r e

h e a d c a s e (/3 = 2 0 ~ i s c o n s i d e r e d . F i r s t l y , t h e r e l a -

t i o n s o f t h e h a r d n e s s a g a i n s t t h e n o r m a l i z e d l e n g t h

p a r a m e t e r a n d t h e n o r m a l i z e d c r y s t a l g r a i n s iz e a r e

p r e d i c t e d ( s ee (1 4 ) ) . S e c o n d l y , t h e r e l a t i o n s o f t h e

h a r d n e s s a g a i n s t t h e i n d e n t d e p t h a n d c r y s t a l g r a in

s i ze a re o b t a i n e d . T h e s i z e e f fe c t a n d g e o m e t r i c a l e f-

f e ct in t h e m i c r o - i n d e n t a t i o n t e s t c a n b e o b v i o u s l y

i d e n ti fi e d . N o t e t h a t t h e c o n v e n t i o n a l fl a t p y r a m i d

c o n e p r e s s u r e h e a d w i l l b e e q u i v a l e n t l y r e p l a c e d b y

t h e f i a t c i r c u l a r c o n i c a l h e a d f o r t h e c o n v e n i e n c e o f

a n a l y s i s , a n d t h e e q u i v a l e n t c o n i c a l a n g l e / 3 i s a b o u t

2 0 d e g r e e s . T h e r e f o r e , i n t h e p r e s e n t r e s e a r c h , t h e

p r e s s u r e h e a d a n g l e i s t a k e n a s / 3 = 2 0 ~

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64

F i g u r e 3 s h o w s t h e r e l a t i o n b e t w e e n t h e n o r m a l -

i z e d h a r d n e s s a n d t h e n o r m a l i z e d m a t e r i a l l e n g t h p a -

r a m e t e r s a n d t h e n o r m a l i z e d c r y s t a l g ra i n s iz e s. T h e

n o r m a l i z i n g q u a n t i t y o f h a r d n e s s ( 3 a y ) i s t h e h a r d -

n e s s v al u e f or t h e t y p i c a l m e t a l m a t e r i a l s w h e n t h e

s i ze e f fe c t i s n e g l e c t e d . T h e n o r m a l i z i n g q u a n t i t y ( R 0 )

f o r t h e l e n g t h p a r a m e t e r a n d f o r t h e c r y s t a l g r a i n s iz e

i s t h e l o a d - l e n g t h p a r a m e t e r , w h i c h i s t h e r a d i u s o f

t h e c o n t a c t z o n e w h e n t h e s i ze e ff e c t i s n o t c o n s i d -

e r e d . I n F i g .3 , a w i d e re g i o n o f t h e n o r m a l i z e d q u a n -

r

30

25

20

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F i g .3 V a r i a t i o n o f h a r d n e s s w i t h n o r m a l i z e d p a r a m e t e r s :

l e n g th p a r a m e t e r L/Ro, g r a i n s i ze t / R o , a n d t/L

A C T A M E C H A N I C A S I N I C A ( E n g l i s h S e r i e s ) 2003

t i t y L / R o f r o m 0 t o 3 a n d a w i d e r e g i o n o f t/Ro a r e

c o n s i d e r e d . F r o m F i g . 3 , t h e h a r d n e s s i n c r e a s e s w i t h

L/Ro q u i c k l y , e s p e c i a l l y f o r s m a l l v a l u e o f t /Ro . A s

t/Ro i n c r e a s e s f r o m 0 .3 6 4 ( t a n 2 0 ~ t o 1 0, t h e h a r d -

n e s s c u r v e d e c r e a s e s v e r y q u i c k l y a t s t a r t i n g , a n d t h e n

a p p r o a c h e s a s t a b l e v a l u e , w h i c h c o r re s p o n d s t o a h o -

m o g e n e o u s m a t e r i a l h a r d n e s s c u r v e ( w h e r e t h e g e o -

m e t r i c a l e f fe c t i s v e r y w e a k ) . N o t e t h a t t h e m a t e r i a l

h a r d n e s s s h a r p l y i n c r e a s e s w h e n t h e i n d e n t d e p t h a p -

p r o a c h e s t h e c r y s t a l g r a i n s i z e v a l u e ( h = 0 . 3 6 4 R ) .

. . . . I . . . . I . . . . i . . . . I , , , , I . , , . I . , , ,

t Ro=O364E / c ~ z : 3 0 0 , u : u ~ : 0 . 3 , E~/E:O.67,N : 0 . 1 ~ / "

j , -

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F i g u r e 3 s h o w s t h e c a s e w h e n t h e c r y s t a l g r a i ns i z e i s l a r g e r t h a n 0 . 3 6 4 R 0 ( t h e i n d e n t d e p t h f o r c o n -

v e n t i o n a l m a t e r i a l ) . T h e e f fe c t o f t h e n o r m a l i z e d p a -

r a m e t e r t/Ro o n t h e h a r d n e s s c h a r a c t e r iz e s e i t h e r t h e

c r y s t a l g r a i n s i z e e f f e c t , o r t h e l o a d e f f e c t . W h e n t h e

c o m p o s i t i o n p a r a m e t e r v a l u e i s s m a l l , i t i s e i t h e r a

s m a l l c r y s t a l g r a i n s i z e c a s e w h e n a p p l i e d l o a d i s f i x e d

o r a b i g l o a d c a s e w h e n g r a i n s i ze is f i x ed . I n o r d e r

t o e x p l a i n t h e e f f ec t o f t h e c r y s t a l g r a i n s iz e , is o l in e s

o f t h e n o r m a l i z e d p a r a m e t e r t /L a r e p l o t t e d b a s e do n t h e h a r d n e s s r e l a t i o n a g a i n s t L / R o a n d t /Ro, see

d a s h e d l i n e s s h o w n i n F i g . 3 . W e a l s o i n v e s t i g a t e t h e

i n f l u e n c e o f Y o u n g ' s m o d u l u s E ~ o f t h e e q u i v a l e n t

b o d y o n th e m a t e r i a l h a r d n e s s. T h e r e s u l t s a re s h o w n

i n F i g . 4 . F r o m F i g . 4 , c l e a rl y , t h e i n f l u e n c e o f t h e

Y o u n g ' s m o d u l u s R a t i o E ~ / E o n t h e m a t e r i a l h a r d -

n e s s is v e r y w e a k w i t h i n a w i d e r e g i o n o f E~/E = 0 . 67

t o 6 . 7 0 .

3 0 . . . . i . . . . I . . . . i . . . . i , . , j I , , , , I , , a ,

E / ~ y = 3 0 0 , u = u ~ = 0 . 3 , N = 0 . 1 ,

d=5t" ' "

25 so l id l ines: E ~/E = 0.67 . " ~ f / = 0 . 3 6 4

20 dashe d lines: E ~/E :6 .7 0 . . . . ~ . f ~

~ / ' " ' " . . .~ " 0 .5

~ 15 "" '~"

~" 0.610 . .""" 'Y'~ " . . . . . '~

5

0 . . . . i . . . . i . . . . ! . . . . i . . . . i . . . . i . . . .

0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5

L/RoF i g .4 T h e i n fl u en c e o f Y o u n g ' s m o d u l u s r a t i o o n t h e h a r d n e s s c u r v e s

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Vol. 19, No .1 Wei Y u e g u a n g et a l.: S ize Effec t and G eom etrical Effec t of Solids 6 5

F u r t h e r m o r e , t h e d a s h e d l in e s in F ig . 3 c a n b e

r e p l o t t e d i n t h e c o o r d i n a t e s: h a r d n e s s / i n d e n t d e p t h ,

s e e F i g . 5 . F r o m F i g . 5 , t h e s i z e e f f e c t a n d t h e c r y s t a l

g r a i n s i z e e f fe c t a r e c l e a r l y s h o w n . W h e n t h e i n d e n t

d e p t h i s s m a l l , i .e ., w h e n t h e i n d e n t t i p i s f a r a w a y

f r o m t h e c r y s t a l b o u n d a r y , t h e s i z e e f f e c t i s d o m i -

n a n t . A s t h e i n d e n t d e p t h i n c r e a s e s , t h e si z e e f f ec t

d e c r e a s e s a n d t h e g e o m e t r i c a l e f fe c t i n c r e a s e s . W h e n

t h e i n d e n t d e p t h a p p r o a c h e s t h e g r a i n b o u n d a r y , t h e

g e o m e t r i c a l e ff e ct b e c o m e s d o m i n a n t a n d m a k e s t h e

h a r d n e s s c u r v e s h a r p l y g o u p . W i t h t h e d e c r e as e o f

t h e c r y s t a l g r a i n s i z e , b o t h t h e s i z e e f f e c t a n d c r y s t a l

g e o m e t r i c a l s i z e e f fe c t a re e n l a r g e d . T h e e f f e c t s o f t h e

c r y s t a l g r a i n s i z e d a n d t h e s i z e i n t h e h o r i z o n t a l d i -

r e c t i o n o n t h e m a t e r i a l h a r d n e s s a r e s h o w n i n F ig . 6 .

I n F i g . 6 , t h e g e o m e t r i c a l e f f e c ts f o r t w o v a l u e s o f d,

d = 5 t a n d d = 1 0 0 t , r e s p e c t i v e l y , a r e d i s p l a y e d . T h e

r e s u l t s s h o w t h a t t h e e f f e c t o f t h e c r y s t a l g r a i n s i z e

i n t h e h o r i z o n t a l d i r e c ti o n o n t h e m a t e r i a l h a r d n e s s i s

v e r y w e a k . T h e c o n c l u s io n i m p l ie s t h a t a l t h o u g h t h e

a n a l y s i s is fo r th e p o l y c r y s t a l m a t e r i a l , i t c a n a p p r o x -

i m a t e l y b e a p p l i e d fo r t h e t h i n f i l m / s u b s t r a t e s y s t e m

t o b e d i s c u s s e d i n t h e n e x t s u b - s e c t i o n .

T h e p h e n o m e n a o f " p i l e- u p " a n d " s in k - i n" in

t h e m i c r o - i n d e n t a t i o n t e s t f o r t h e p o l y c r y s t a l m a t e -

r i a l a r e a ls o i n v e s t i g a t e d h e r e . T h e r e s u l t s a r e s h o w n

i n F i g .7 . F r o m F i g . 7 , w i t h t h e i n c r e a s e o f t h e m a -

t e r ia l l e n g t h p a r a m e t e r o r w i t h t h e d e c r e a s e o f t h e

a p p l i e d l o a d ( R 0 = V/P/37ray), c o r r e s p o n d i n g l y w i t h

t h e i n c r e a s e o f L/Ro , t h e " p i l e - u p " p h e n o m e n o n d i s -

a p p e a r s a n d t h e " s in k - i n " fe a t u r e g e ts p r o m i n e n t i n

t h e m i c r o - i n d e n t a t i o n t e st . T h e p il e - u p p h e n o m e n o n

i s f a v o r a b l e fo r t h e b i g f o r ce a n d s m a l l l e n g t h p a r a m e -

t e r . T h i s c o n c l u s i o n i s c o n s i s t e n t w i t h t h e s i n g l e c ry s -

t a l m a t e r i a l c a s e [9 ]. W h e n t h e c r y s t a l g r a i n s iz e is

l a r g e , t h e g e o m e t r i c a l e f f e c t i s w e a k , a n d t h e s i z e e f -

f e c t i s d o m i n a n t . A s t h e c r y s t a l g r a i n s i z e d e c r e a s e s ,

t h e g e o m e t r i c a l e ff e c t i n c r e a s e s , a n d t h e i n d e n t d e p t h

d e c r e a s e s c o n s i d e r a b l y f o r a f i x e d a p p l i e d l o a d .

10

9

8

7

6

4

3

I

0.364i l2

1

I , I , i ,

E/o'y=300, u = u ~ = 0 . 3 ,

E ~ / E = 0 . 6 7 , N = 0 . 1

0, 7

t/L=lO.Oi I i i

0.0 0.2 0.4 0,6 0.8 1.0

h lL

F i g .5 S iz e e f fe c t a n d g e o m e t r i c a l e f fe c t o n t h e h a r d n e s s / d e p t h r e l a t i o n s

3 0 . . . . i . . . . i . . . . i . . . . i . . . . i , , , . i , . , ,

E/~y=300, ~=~=0 .3 , E~/E=0.67, N = 0 . 1 ~

25 solid ines: d=5t / . . - " "20 dashed ines: d = l O O t ~ . - " " t/t/o=0.364

i " "

~ " . . J . . - - ' " " " 0 .6

5

0 , , , , I , , , ' I , , , , I . . . . I . . . . I . . . . I ' ' , '

0.0 0.5 1.0 1.5 2.0 2.5 3.0 3.5

L/ Ro

F ig . 6 E f f ec t o f the c r ys ta l g r a in size in the h or izon ta l d i r ec t ion on the h a r dness

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66 ACTA MECHANICA SINICA (English Series)

0.40

0.35

0.30

0.25

0.20

0.15

0.10

0.05

0.00

--0.05

, I , I ,

,. E/~ry= 300, u=~, ,=0.3, N= 0.1,

::~"~i~:., /3=20 ~ d=5t, E~/E=0.67

-,~:, solid lines: t /R 0 = 0 . 5

\ 'i:~. dashed lines: t/Ro=5.0

' :k

"'i:~ L/R0=2.0k i n.~:. 1.0

~ 0.0

~ : ~ . , ; @ m l ~ ! ~ ' ~ . . . . . . . . . . . . . . . . . . . . . . . . . . .

i i

0 1 2 3

r/R0

Fig.7 The simulation of the phenom ena "pile-up" and "sink-in"

for polycrysta l in micro- indentation test

2003

5 . 2 M i c r o - I n d e n t a t i o n E x p e r i m e n t f o r P o l y -

c r y s t a l A 1

I n o r d e r t o s t u d y th e m ic r o - g e o m e t r i c a l e f f e c t s

e x p e r im e n ta l l y , w e d e s ig n t h e t e s t sp e c im e n s f o r p o ly -

c rys ta l A1 wi th seve ra l d i f fe ren t c rys ta l g ra in s izes .

T h e i n d e n t a t i o n e x p e r i m e n t a l m e t h o d i s s i m i l a r w i t h

R e f. [9 ] fo r t h e s i n g l e c r y s t a l m a te r i a l . T h e e x p e r im e n -

t a l m e th o d c o n s i s t s o f c h o o s in g m a n y lo a d in g p o in t s

a r b i t r a r i l y o n t h e sp e c im e n su r f a c e , a n d f o r o n e l o a d -

in g p o in t , o n ly o n e s e t o f e x p e r im e n ta l d a t a a b o u t

h a r d n e s s a n d i n d e n t d e p th b e in g o b t a in e d . I n su c h am e t h o d w e s h a ll o b t a i n a d a t a s t r i p a b o u t t h e h a r d -

n e s s / i n d e n t d e p t h r e la t io n . T h e s c a t t e r d e g r ee o f t h e

d a t a s t r i p d e p e n d s o n t h e f e a tu r e o f t h e s e l e c t e d l oa d -

in g p o in t o n t h e sp e c im e n su r f a c e . I f a n i n d e n t p o in t

i s j u s t l o c a t e d a t a f a u l t r e g io n o n t h e sp e c im e n su r -

f a c e , a l o w h a r d n e s s w i l l b e o b t a in e d , w h e n th e i n -

dent de pth i s f ixed . I f an indent poin t i s jus t chosen

a t a ha rd pa r t ic le , a h igh ha rdness va lue i s ob ta ined .

F ig u r e 8 sh o w s th e su r f a c e p r o f i l e o f t h e p o ly c r y s t a l

A 1 sp e c im e n f or a SE p h o to g r a p h . F r o m F ig . 8, o n

the spec imen sur face , some fau l t s ex is t inevi tab ly . I f

t h e c o n t in u u m s t i f f n e s s m e th o d i s u se d , t h e o b t a in e d

h a r d n e s s c u r v e m u s t d e p e n d o n t h e i n d e n t l o c a t io n .

T h e r e f o r e , w e sh a l l u se t h e e x p e r im e n ta l m e th o d h e r e

b y s e l ec t i n g t h e i n d e n t l o a d in g p o in t s o n t h e sp e c im e n

su r f a c e a r b i t r a r i l y a s i n [ 9 ], r a th e r t h a n a d o p t in g t h e

c o n t in u u m s t i f f n e s s m e th o d , so t h a t t h e i n f lu e n c e o f

the fau l t s and the d i f fe ren t loading poin t se lec t ions on

th e e x p e r im e n ta l r e su l t s w i l l b e d i sp l a y e d c l e a r ly .

Fig.8 The prof ile of the spec imen surface for the p olycrysta l A1

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Vo l .19 , No .1 W e i Y u e g u a n g e t a l .: S i z e E fF ec t a n d G e o m e t r i c a l E f f e c t o f S o l id s 6 7

I n F ig . 9, t h e e x p e r i m e n t a l h a r d n e s s r e s u l ts f o r

p o l y c r y s t a l A 1 f o r s e v e r a l c r y s t a l g r a i n s i z e s a r e

s h o w n . F r o m F i g s . 9 ( a ) t o ( d ) , t h e s e r ie s o f t h e g r a i n

s iz e s, 0 .6 # m , 1 # m , 2 # m a n d i n f i n i t ly l a r g e s i ze ( s in -

g l e c r y s t a l A 1), a re sh o w n s e p a r a t e l y . T h e r e s u l t s

s h o w t h a t t h e f e a t u r e o f t h e h a r d n e s s v a r i a t i o n w i t h

t h e i n d e n t d e p t h i s i n a " U " f o r m . W h e n t h e i n d e n t

d e p t h i s sm a l l , a s t r o n g s i z e e f fe c t i s c h a r a c t e r i z e d . A s

t h e in d e n t d e p t h i n c r e a s e s , t h e h a r ( b w s s d e c r e a s e s a n d

p a s s e s t h r o u g h a l o w e r l i m i t v a l u e , t h e n i n c r e a s e s w i t h

t h e in d e n t t i p a p p r o a c h i n g t h e g r a in b o u n d a r y . C o m -

p a r i n g t h e r e s u l t s s h o w n i n F i g s . 9 ( a ) , ( b ) , ( c ) a n d ( d )

f o r d i f f e r e n t c r y s t a l g r a i n s i z e s , w i t h t h e d e c r e a s e o f

t h e c r y s t a l g r a i n s i z e , t h e h a r d n e s s i n c r e a s e s i n g e n -

e r al . F o r c o m p a r i s o n , t h e t h e o r e t i c a l p r e d i c t i o n s o f

t h e h a r d n e s s u s i n g t h e s t r a i n g r a d i e n t p l a s t i c i t y a r e

a l s o s h o w n i n F i g . 9 . F o r e a c h c a se , t w o c u r v e s c o r -

r e s p o n d i n g t o d i f f e r e n t l e n g t h p a r a m e t e r v a l u e s a r e

p l o t t e d . T h e s e t w o c u r v es c a n b e t a k e n a s t h e b o u n d s

o f t h e e x p e r i m e n t a l d a t a . A s t h e c ry s t a l g r a in s iz e

i n c r e a s e s , t h e l e n g t h p a r a m e t e r v a l u e s d e c r e a s e , a n d

a p p r o a c h 1 # m a n d 2 # m , c o r r e s p o n d i n g t o t h e l o w e r

b o u n d c u r v e a n d u p p e r b o u n d c u r v e , r e s p e ct i v e ly , fo r

t h e s in g le c r y s t a l c a se . T h e m a t e r i a l h a r d n e s s a p -

p r o a c h e s t h e c o n v e n t i o n a l v a l u e a s t h e i n d e n t d e p t h

i n c r e a s e s in f i n it e l y . F o r t h e s i n g l e c r y s t a l c a s e , t h e

c u r v e f e a t u r e o f t h e h a r d n e s s v a r i a t i o n w i t h t h e i n -

d e n t d e p t h i s i n a n " L " f o r m .

:n

6 0 0 0

5 000-

4 000-

3 000

2 000

1 00 0

0

I I I I I I

exper iment for po lycrysta l AI

0

L = l . 4 # mi i i i i i

50 100 150 200 250 300 350

h /nm

( a )

5 000

4 000

3 000'

2 0 0 0

1 0 0 0

I , I I I

expe r imen t for polycrysta l AI

t = 1 0 0 0 n m

00

k ~ N L = 2 . 9 # m

L = l . 3 # m, , i i i

100 200 300 400 500 600

h /nm

( b )

4 000

3000"

a~

2 o o o .

1 0 0 0

I I I I

experiment for polycrystal AI

0 0 0 ~ 0 % 2 0 0 0 n i I 1

0 i

0 200

L = l . 2 p m

i i i

400 600 800

h /nm

( c )

2 000 ~ , , i ,

single crystal AI. (110)

1 6 0 0

0~t 2 o 0 -

a :

800"

0

0 ~ k L = 2 ttm

400 . . . . .200 400 600 800 1000 12000 0 0 0

h/nm

(d )

F i g .9 E x p e r i m e n t a l a n d n u m e r i c a l r e s u l t s o f t h e h a r d n e s s / i n d e n t

dep th r e la t ions f o r d i f f e r en t c r ys ta l g r a in s izes

A s m e n t i o n e d a b o v e , i f o n e a d o p t s t h e m e t h o d

o f a r b i t r a r i l y s e l e c t i n g th e l o a d i n g p o i n t s o n t h e s p e c -

i m e n s u r f a c e i n t h e i n d e n t a t i o n e x p e r i m e n t , o n e w i l l

o b t a i n t h e h a r d n e s s v a r i a ti o n s w i t h t h e i n d e n t d e p t h

i n t h e f o r m o f t h e d a t a s t ri p . F i g u r e 9 s ho w s s u c h

s t ri p s , t h e s c a t t e r e d d a t a s t ri p s . O b v i o u s l y , t h e w i d t h

o f t h e s c a t t e r e d s t r i p o f t h e h a r d n e s s f o r t h e p o l y -

c r y s t a l s p e c i m e n is s o m e w h a t l a r g e r t h a n t h a t f o r t h e

s i n g l e - c r y s t a l s p e c i m e n , c o m p a r i n g F i g s . 9 ( a ), ( b ) , ( c)

w i t h F i g . 9 ( d ) . T h i s r e s u l t i s r e a s o n a b l e a n d s e e m s t o

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6 8

b e e x p e c t e d . T h i s i s b e c a u s e f o r a p o l y c r y s t a l s p e c i-

m e n t h e e x p e r i m e n t a l h a r d n e s s i s i n fl u e n ce d b o t h b y

t h e l o a d i n g p o i n t s t a t u s ( f a u l t s , r e i n f o r c e d - p a r t i c l e s ,

e t c . ) a s f o r a s i n g l e - c r y s t a l s p e c i m e n c a s e , a n d b y t h e

g r a i n b o u n d a r i e s a n d t h e g r a i n si z e d i f fe r e n c es . T h e

l a t t e r e f fe c t i s s p e c i f ic a l l y i m p o r t a n t f o r t h e p r e s e n t r e -

s e a r c h ca s e w h e n i n d e n t d e p t h s a r e c o m p a r a b l e w i t h

t h e g r a i n s iz e s. A l t h o u g h t h e p o l y c r y s t a l s p e c i m e n

i s e x p e c t e d c o n s i s t i n g o f t h e u n i f o r m g r a i n s i ze , it i s

r a r e l y th e c a s e. F r o m t h e S E p h o t o g r a p h o f t h e s u r -

f a c e p r o fi l e fo r a p o l y c r y s t a l A 1 s p e c i m e n w i t h 1 p m

g r a i n s i z e s h o w n i n F i g . 8 , b e s i d e s t h e m a n y f a u l t s b e -

i n g o b s e r v e d o n t h e s u r f a c e , t h e g r a i n s i z e s a r e n o t

u n i f o r m . I n F ig . 8 , t h e l o n g e r b l a c k c u r v e s c h a r a c t e r -

i ze th e g r a i n b o u n d a r i e s a n d t h e s m a l l b l a c k z o n es a r e

t h e f a u l t s . S o m e i n d e n t l o a d i n g l o c a t i o n s a r e c l e a r l y

o b s e r v e d i n t h e f i g u r e .

6 T i F I L M L A I N O N T H E S i3 N 4 C E R A M I C

S U B S T R A T E U N D E R G O I N G M I C R O -

I N D E N T I N G

L e t u s d i s c u s s t h e h a r d n e s s o f a t h i n f i l m l a i n o n

a c e ra m i c s u b s t r a t e . W h e n t h e t h i n f i lm t h i c k n e ss is

c o m p a r a b l e w i t h t h e in d e n t d e p t h , t h e s u b s t r a t e a n d

f i l m / s u b s t r a t e i n t e r f a c e w i l l h a v e a s t r o n g i n f l u e n c e o n

t h e h a r d n e s s ( g e o m e t r i c a l e ff e c t) . I n t h e p r e s e n t c a s e ,

t h e p a r a m e t e r r e l a t i o n b e t w e e n h a r d n e s s a n d o t h e r

m a t e r i a l a n d g e o m e t r i c a l p a r a m e t e r s i s g i v e n i n ( 1 5) .

F r o m d i s c u s s i o n s i n s u b s e c t i o n 4 . 1 , t h e p r e d i c t e d

h a r d n e s s r e l a t i o n f o r t h e p o l y c r y s t a l m a t e r i a l s h o w n

i n F i g . 5 c a n b e a p p l i e d t o t h e t h i n f i l m / s u b s t r a t e s y s -

t e m a p p r o x i m a t e l y w i t h i n a p a r a m e t e r r e g i o n 0 . 6 7 <

E , / E < 6 . 7 0 . I n t h e p r e s e n t c a s e , t h e Y o u n g ' s m o d u -

l u s r a t i o f o r t h e c e r a m i c s u b s t r a t e ( S i a N 4 ) a n d m e t a l

t h i n f i l m ( T i ) i s a b o u t 6 . 0 . I n o r d e r t o i n v e s t i g a t e

t h e h a r d n e s s v a r i a t i o n w i t h t h e t h i n f i l m t h i c k n e s s ,

w e h a v e d e s i g n e d t h r e e k i n d s o f t h e s p e c i m e n s c o r r e -

s p o n d i n g t o a s e r i e s o f t h e t h i n f i l m t h i c k n e s s . F o r

a c o m p a r i s o n , w e a d o p t t h e c o n v e n t i o n a l c o n t i n u u m

s t i f f n e s s m e t h o d i n t h e e x p e r i m e n t , i . e . , t h e c u r v e o f

t h e h a r d n e s s v a r i a t i o n w i t h t h e i n d e n t d e p t h i s o b -

t a i n e d f r o m o n e l o a d i n g p o i n t o n t h e s p e c i m e n s u r -

f a c e . I n s u c h a t e s t m e t h o d , t h e e x p e r i m e n t a l h a r d -

n e s s c u r v e w i l l b e a s m o o t h o n e .

F i g u r e i 0 s h o w s t h e e x p e r i m e n t a l h a r d n e s s f o r

t h e T i f i l m l a i n o n t h e S i 3 N 4 s u b s t r a t e f o r t h r e e d i f -

f e r e n t t h i c k n e s s e s o f t h e t h i n f i l m . F i g u r e s 1 0 ( a ) , ( b )

a n d ( c ) c o r r e s p o n d t o t h e t h i n f i l m t h i c k n e s s 1 . 2 p m ,

1 . 8 # m a n d 1 3 # m , r e s p e c t i v e l y . F r o m F i g . 1 0 , t h e f e a -

t u r e o f t h e h a r d n e s s v a r i a t i o n w i t h t h e i n d e n t d e p t h

i s i n a " U " f o r m a n d i t c a n b e d e s c r i b e d a s f o l l o w s :

ACT A ME CH ANICA SINICA (Engl ish Ser ies) 2003

W h e n i n d e n t d e p t h i s s m a l l , t h e r e s u l t s h o w s a s t r o n g

s iz e e f fe c t. A s t h e d e p t h i n c r e a s e s , t h e h a r d n e s s d e -

c r e a s e s q u i c k l y u n t i l t h e i n d e n t d e p t h r e a c h e s s o m e

f r a c t i o n o f t h e t h i n f i lm t h i c k n e s s , t h e h a r d n e s s a s -

s u m e s a l o w e s t v a l u e . F r o m t h e l o w e s t v a l u e t h e

h a r d n e s s t u r n s t o i n c r e a s e a s t h e i n d e n t d e p t h i n -

c r e a s e s f u r t h e r . A l t e r n a t i v e l y , a s t h e t h i n f i l m t h i c k -

n e s s i n c r e a se s ; t h e h a r d n e s s d e c r e a s e s a l l o v e r t h e r e -

g i o n a n d t h e d e p t h v a l u e c o r r e s p o n d i n g t o t h e l o w e s t

h a r d n e s s p o i n t i n c r e a s e s. W h e n t h e t h i n fi l m t h i c k -

n e s s i n c r e a s e s to a c e r t a i n e x t e n t ( 1 3 # m ) , t h e i n -

f l u en c e o f t h i n f i lm t h i c k n e s s o n t h e h a r d n e s s c u r v e

c a n b e n e g le c t e d , s o t h a t t h e h a r d n e s s / d e p t h c u r v e

a p p r o a c h e s t h e c o n v e n t i o n a l h a r d n e s s v a l u e a s t h e

i n d e n t d e p t h i n c r e a s e s u n t i l t h e p r e s s u r e h e a d a p -

p r o a c h e s t h e i n t e r f a c e . F o r t h e s m a l l t h i n f i lm th i c k -

n e s s , s e e F i g . 1 0 ( a ) ( c a s e I ) , d u e t o t h e s t r o n g s i z e e f -

f e c t a n d g e o m e t r i c a l e f f e c t , t h e h a r d n e s s i s v e r y h i g h ,

b u t t h e s i ze ef fe c t i s d o m i n a n t w h e n t h e i n d e n t d e p t h

i s s m a l l . W i t h i n c r e a s i n g d e p t h , t h e s i ze e f fe c t d e -

c r e a s e s a n d t h e g e o m e t r i c a l e f f e c t ( th e e f fe c t o f t h i n

f i lm t h i c k n e s s a n d i n t e r fa c e ) i n c r e a s e s . U n t i l a d e p t h

e q u a ls t o a b o u t 3 00 n m ( a b o u t o n e f o u r t h o f t h i n f i lm

t h i c k n e s s ) , t h e g e o m e t r i c a l e f fe c t is so la r g e t h a t t h e

h a r d n e s s c u r v e t u r n s t o i n cr e a se . T h e h a r d n e s s o b -

t a i n s a lo w e r l im i t v a l u e 5 .6 G P a a t t h e t u r n i n g p o i n t .

F r o m F i g . 1 0 ( b ) , i n c r e a s i n g t h e t h i n f i l m t h i c k n e s s b y

0 . 6 # m , i .e ., t = 1 . 8 # m ( c a s e I I ) , t h e g e o m e t r i c a l el -

f e ct d e c re a s e s r e m a r k a b l y c o m p a r i n g w i t h c a s e I. F o r

e x a m p l e , t h e h a r d n e s s i s a b o u t 1 0 G P a a t h = 1 00 n m

f o r c a s e I , f r o m F i g . 1 0 ( a ) , w h i l e t h e c o r r e s p o n d i n g

h a r d n e s s a t t h e s a m e d e p t h i s a b o u t 8 G P a f o r ca s e I I,

f r o m F ig . 1 0 ( b ). W h e n t h e i n d e n t d e p t h i s s m a l l, th e

s iz e e f fe c t i s d o m i n a n t . A s t h e i n d e n t d e p t h i n c r e a s e s

a n d t h e h a r d n e s s d e c r e a s e s u n t i l t h e t u r n i n g p o i n t a t

a b o u t h = 5 8 0 n m ( a b o u t o n e t h i r d o f t h e t h i n f i l m

t h i c k n e s s ) is a p p r o a c h e d , f r o m F i g . 1 0 ( b ) . T h e r e a f t e r ,

t h e g e o m e t r i c a l e f fe c t i s d o m i n a n t . C o n s i d e r i n g t h a t

t h e t h i n f i lm t h i c k n e s s i n c r e a s e s a n d b e c o m e s v e r y

l a r g e , s ee F i g . 1 0 ( c ) ( c a se I I I ) , t h e g e o m e t r i c a l e f fe c t

c a n b e n e g l e c te d . W i t h t h e i n c r e a se o f d e p t h , t h e

s iz e e f fe c t d e c r e a s e s . W h e n t h e h a r d n e s s d e c r e a s e s t o

a m a c r o - s c M e h a r d n e s s v a l u e , t h e s i z e e f f e c t c a n b e

n e g l e c t e d .

I n F i g s . lO ( a ) , ( b ) a n d ( c ), t h e t h e o r e t i c a l p r e -

d i c t io n s o f t h e t h i n f i l m / s u b s t r a t e h a r d n e s s f r o m t h e

s t r a i n g r a d i e n t p l a s t i c i t y t h e o r y a r e a l s o s h o w n . O b -

v i o u s ly , t h e c h a r a c t e r i s t i c s o f th e t h e o r e t i c a l p r e d i c -

t i o n s a re c o n s i s t e n t w i t h t h o s e o f t h e e x p e r i m e n t a l

r e su l ts . T h r o u g h p l o t t i n g t h e t h e o r e t i c a l p re d i c t io n s

a n d t h e e x p e r i m e n t a l r e s u l t s t o g e t h e r i n F i g s . l O ( a ) ,

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Vo1.19, No.1 W e i Y u e g u a n g e t a l . : Size Effect and G eometr ica l E ffect of Sol ids 6 9

( b ) a n d ( c ), t h e d e p e n d e n c e o f t h e m a t e r i a l l e n g t h

p a r a m e t e r o n t h e t h i n f il m t h i c k n e s s i s o b t a i n e d . T h e

c o r r e s p o n d i n g v a lu e s o f t h e m a t e r i a l l e n g t h p a r a m e t e r

a r e a l s o s h o w n i n F i g s . 1 0 ( a ) , ( b ) a n d ( c ) , r e s p e c t iv e l y .

O b v i o u sl y , t h e l e n g t h p a r a m e t e r a ls o d e p e n d s o n t h e

m i c r o - g e o m e t r i c a l s iz e ( t h i n f i lm t h i c k n e s s ) .

10

8

2

0

, I f I , I ~ I ,

o o o o o o

~ exper iment for

"~Ti/Si3N4

theoreticalpredieition

t = l . 2 p m , L = 4 . 5 p mE / c r y = 3 0 0 , u = u ~ = 0 . 3 ,

E ~ / E = 6 . 0 , N = 0 . 1

200 400 600 800 1 000 200 400 600 800

h/nm h/nm

8

7

6

5

4

a

2

1

00

I , I I I ,

E / a z = 3 0 0 , L ' = u ~=0.3 ,

E~/E=6.0,N = 0 . 1t = 1 . 8 p m , L = 2 . 6 p m

booO ~

t h e o r e t i c a l

p r e d i d t i o n e x p e r i m e n t f o r

T i / S i 3 N 4

( a ) ( b )

1 000

8 i I ~ I , I I

E / ~ ry = 3 0 0 , p = ~ = 0 .3 ,

7 E~/E=6.0, = 0 . 16 ~ t = 1 3 p m , L = l . 3 p m

e 5 ~ ~

2

e x p e ri m e n t f o r T i / S ~ '3 ~ 4 . . . . .0 i i i i

0 200 400 600 800 1 000

h/nm

( c )

F i g .1 0 E x p e r i m e n t a l a n d n u m e r i c a l r e s u lt s o f t h e h a r d n e s s / i n d e n t d e p t h f o r

T i /S iaN4 th in f i lm/su bs t ra t e fo r d i ffe ren t th i cknes s of th in f i lm

7 C O N C L U D I N G R E M A R K S

I n t h e p r e s e n t r e s e a r c h , t h e s i z e e f f e c t s a n d g e -

o m e t r i c a l e ff e c ts i n t h e m i c r o - i n d e n t a t i o n t e s t s h a v e

b e e n s i m u l a t e d a n d p r e d i c t e d b y u s i n g t h e f i n i t e e l -

e m e n t i m p l e m e n t a t i o n b a s e d o n t h e s t r a i n g r a d i e n t

p l a s t i c i t y t h e o r y . M e a n w h i l e , t h e e x p e r i m e n t a l r e -

s e a r c h e s o f t h e m i c r o - i n d e n t a t i o n t e s t f o r p o l y c r y s t a l

a l u m i n u m a n d f o r t h e T i / S i 3 N 4 t h i n f i l m / s u b s t r a t e

s t r u c t u r e h a v e b e e n c a r r i e d o u t .

F o r t h e p o l y c r y s t a l m a t e r i a l a n d f o r t h e t h i n

f i l m / s u b s t r a t e s y s t e m , w h e n t h e c r y s t a l g r a i n s i z e o r

t h e t h i n f i l m t h i c k n e s s i s c o m p a r a b l e w i t h t h e i n d e n t

d e p t h , t h e c o m p o s i t i o n e f f e c ts f r o m s i z e ef f e ct a n d

f r o m g e o m e t r i c a l e f f ec t o n t h e m a t e r i a l h a r d n e s s a r e

c o n s i d e ra b l y s t ro n g . F o r t h e h a r d n e s s / d e p t h c u r ve ,

w h e n t h e d e p t h i s s m a l l, t h e s iz e e ff e c t i s d o m i n a n t .

A s t h e i n d e n t d e p t h i n c r ea s e s, t h e s iz e e ff e c t d e c r e a s e s

a n d t h e g e o m e t r i c a l e f f ec t i n c r ea s e s . B e f o r e a d e p t h( a t u r n i n g p o i n t ) i s r e a c h e d , t h e g e o m e t r i c a l ef f e ct i n -

c r e a se s , d o m i n a t e s a n d m a k e s t h e h a r d n e s s c u r v e g o

u p s h a r p l y .

T h e s i m u l a t i o n r e s u l t s u s i n g t h e s t r a i n g r a d i e n t

p l a s t i c i t y t h e o r y f o r t h e s i z e e f f e c t a n d t h e g e o m e t -

r i c a l e f f e c t a r e c o n s i s t e n t w i t h e x p e r i m e n t a l r e s u l t s .

T h r o u g h c o m p a r i n g t h e s i m u l a t io n r e s u lt s w i t h e x p e r -

i m e n t a l r e s u l t s , t h e v a l u e s a n d t h e v a r i a t i o n t r e n d s o f

t h e m a t e r i a l l e n g t h p a r a m e t e r i n c l u d e d i n t h e s t r a i n

g r a d i e n t p l a s t i c i t y t h e o r y h a v e b e e n p r e d i c t e d .

F r o m e x p e r i m e n t a l r e s u l t s f o r p o l y c r y s t a l A 1 ,

e v e n t h o u g h t h e c r y s t a l g r a i n s i z e i s f i x e d , t h e h a r d -

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7O ACTA MECHANICA S INICA

nes s/d ept h relation is still a scatte r strip. The feature

mainly comes from the status of the indenting point

on the specimen surface. Certainly, it is possible that

the prepared specimens always and inevitably include

some faults or reinforced phases and the differences

amon g the crystal sizes and shapes. From experimen-

tal results for Ti/Si3N4 thin film/substrate system

using the continuum stiffness method, the composi-

tion effects of the size effect and geometrical effect are

clearly displayed. The experimen tal results show tha t

the material length parameter has a fixed value for a

uniform material, however, when the micro-structure

is considered and the length parameter increases, de-

pending on the micro-geometrical size.

Ac kn ow le dg em en t A great help for preparing poly-

crys tal A1 speci men from Dr. Wu Xiaolei, is sincerely

acknowledged.

R E F E R E N C E S

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