nanotest™ nt600 - a de vice for anal y ses of me chan i

4
NanoTest™ NT600 - A DEVICE FOR ANALYSES OF MECHANICAL PROPERTIES OF MATERIALS R. Ètvrtlík, M. Stranyánek, P. Boháè, L. Jastrabík Institute of Physics of Academy of Sciences of the Czech Republic, Na Slovance 2, 182 21 Prague, Czech Republic Keywords: NanoTest™, nanoindentation, Oliver-Pharr method, scratch test, impact test, impulse test, acoustic emission, pin on disc Abstract Thin films and coatings technology have become the cru- cial aspect in a wide range of production processes. It is used with success for instance in electro technical industry, electronics, optics, mechanical engineering, energetics and medicine. On this account the mechanical properties me- trology of thin films and coatings has become very impor- tant due to their optimization as well as high-quality production. There are numbers of devices available for the measurement of these properties, either specialized for cer- tain test or universal which are available to carry out the en- tire analysis of mechanical properties of thin films and surfaces. The special rank belongs to the modular measur- ing system NanoTest™ (Micro Materials Ltd.) significant by its unique construction, which enables horizontally loading of the specimen. Introduction Modular measuring system NanoTest™ NT600 is a device designed for measurement of mechanical properties of thin films and coatings. The platform can measure hardness, evaluate elastic modulus, adhesion, wear as well as fracture and dynamic properties. At the heart of the NanoTest™ system there is a pendulum that can rotate on a friction-less pivot. A coil is mounted at the top of the pendulum; as a coil current is applied, the coil is attracted towards a perma- nent magnet, producing motion of the diamond towards the sample and into the sample surface. The displacement of the diamond is measured by means of a parallel plate ca- pacitor, one plate of which is attached to the diamond holder; when the diamond moves, the capacitance changes, and this is measured by means of a capacitance bridge [1]. The NanoTest™ flexibility consists directly in its mod- ular conception. Number of measuring methods and tech- niques can be very easily accessed by mere implementation of additional modules such as friction probe, microscope with high resolution, AFM, acoustic emission system, pin on disk tribometer, etc. Furthermore, it is possible to per- form the named tests at high temperature. The basic platform consists of four independent mod- ules which enable indentation, scanning, dynamic impact and impulse tests. For all these modules can be used either the low load head (0.1-500 mN) for films thickness of 20 nm - 5 mm or the high load “MicroTest” head (0.1-20 N). High load head is suitable for investigation of layers of thickness up to 50 mm. The whole measuring system oper- ates on anti-vibration table in a special cabinet in order to minimize thermal drift, reduce air turbulence upsetting the NanoTest™ pendulum and provide sound-proofing to re- duce acoustic disturbance. System control and data collec- tion are completely assured by personal computer by means of special software, communication proceeds over IEEE bus [1]. Nanoindentation Nanoindentation is an important and effective experi- mental method. It is extensively used to estimate the plastic and elastic properties of thin films and surface layers of submicron thickness. Through nanoindentation test, the material parameters, such as hardness, Young’s modulus, yield strength, and strain hardening exponent, as well as fracture toughness can be estimated. The examination prin- ciple is the penetration of a diamond tip of known propor- tion and geometry into the investigated surface at accurately defined loading force and subsequent analysis. Testing by NT600 is based on Depth Sensing Indenta- tion (DSI) at which the loading force P and corresponding Ó Krystalografická spoleènost 90 Materials Structure, vol. 13, no. 2 (2006) Fig. 1. NanoTest™ platform concept.

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Page 1: NanoTest™ NT600 - A DE VICE FOR ANAL Y SES OF ME CHAN I

NanoTest™ NT600 - A DE VICE FOR ANAL Y SES OF ME CHAN I CALPROP ER TIES OF MA TE RI ALS

R. Ètvrtlík, M. Stranyánek, P. Boháè, L. Jastrabík

In sti tute of Phys ics of Acad emy of Sci ences of the Czech Re pub lic, Na Slovance 2, 182 21 Prague, Czech Re pub lic

Keywords: NanoTest™, nanoindentation, Ol i ver-Pharr method,scratch test, im pact test, im pulse test, acous tic emis sion,pin on disc

Ab stractThin films and coat ings tech nol ogy have be come the cru -cial as pect in a wide range of pro duc tion pro cesses. It isused with suc cess for in stance in elec tro tech ni cal in dus try,elec tron ics, op tics, me chan i cal en gi neer ing, energetics and med i cine. On this ac count the me chan i cal prop er ties me -trol ogy of thin films and coat ings has be come very im por -tant due to their op ti mi za tion as well as high-qual itypro duc tion. There are num bers of de vices avail able for themea sure ment of these prop er ties, ei ther spe cial ized for cer -tain test or uni ver sal which are avail able to carry out the en -tire anal y sis of me chan i cal prop er ties of thin films andsur faces. The spe cial rank be longs to the mod u lar mea sur -ing sys tem NanoTest™ (Mi cro Ma te ri als Ltd.) sig nif i cantby its unique con struc tion, which en ables hor i zon tallyload ing of the spec i men.

In tro duc tion

Mod u lar mea sur ing sys tem NanoTest™ NT600 is a de vicede signed for mea sure ment of me chan i cal prop er ties of thinfilms and coat ings. The plat form can mea sure hard ness,eval u ate elas tic modulus, ad he sion, wear as well as frac ture and dy namic prop er ties. At the heart of the NanoTest™sys tem there is a pen du lum that can ro tate on a fric tion-lesspivot. A coil is mounted at the top of the pen du lum; as acoil cur rent is ap plied, the coil is at tracted to wards a per ma -nent mag net, pro duc ing mo tion of the di a mond to wards the sam ple and into the sam ple sur face. The dis place ment ofthe di a mond is mea sured by means of a par al lel plate ca -pac i tor, one plate of which is at tached to the di a mondholder; when the di a mond moves, the ca pac i tance changes, and this is mea sured by means of a ca pac i tance bridge [1].

The NanoTest™ flex i bil ity con sists di rectly in its mod -u lar con cep tion. Num ber of mea sur ing meth ods and tech -niques can be very eas ily ac cessed by mere im ple men ta tion of ad di tional mod ules such as fric tion probe, mi cro scopewith high res o lu tion, AFM, acous tic emis sion sys tem, pinon disk tribometer, etc. Fur ther more, it is pos si ble to per -form the named tests at high tem per a ture.

The ba sic plat form con sists of four in de pend ent mod -ules which en able in den ta tion, scan ning, dy namic im pactand im pulse tests. For all these mod ules can be used ei therthe low load head (0.1-500 mN) for films thick ness of

20 nm - 5 mm or the high load “MicroTest” head (0.1-20N). High load head is suit able for in ves ti ga tion of lay ers of

thick ness up to 50 mm. The whole mea sur ing sys tem op er -

ates on anti-vi bra tion ta ble in a spe cial cab i net in or der tomin i mize ther mal drift, re duce air tur bu lence up set ting theNanoTest™ pen du lum and pro vide sound-proof ing to re -duce acous tic dis tur bance. Sys tem con trol and data col lec -tion are com pletely as sured by per sonal com puter bymeans of spe cial soft ware, com mu ni ca tion pro ceeds overIEEE bus [1].

Na no in den tati on

Nanoindentation is an im por tant and ef fec tive ex per i -men tal method. It is ex ten sively used to es ti mate the plas ticand elas tic prop er ties of thin films and sur face lay ers ofsubmicron thick ness. Through nanoindentation test, thema te rial pa ram e ters, such as hardness, Young’s modulus,yield strength, and strain hard en ing ex po nent, as well asfrac ture tough ness can be es ti mated. The ex am i na tion prin -ci ple is the pen e tra tion of a di a mond tip of known pro por -tion and ge om e try into the in ves ti gated sur face atac cu rately de fined load ing force and sub se quent anal y sis.

Test ing by NT600 is based on Depth Sens ing In den ta -tion (DSI) at which the load ing force P and cor re spond ing

Ó Krystalografická spoleènost

90 Ma te ri als Struc ture, vol. 13, no. 2 (2006)

Fig. 1. NanoTest™ plat form con cept.

Page 2: NanoTest™ NT600 - A DE VICE FOR ANAL Y SES OF ME CHAN I

in den ta tion depth h is con tin u ously re corded dur ing thewhole in den ta tion cy cle. In a typ i cal in den ta tion cy cle, load is ap plied to an in denter that is in con tact with the sur face of a spec i men. The load and depth of pen e tra tion are re cordedas load is ap plied from zero to a pre-de fined max i mum andthen from max i mum load back to zero [2]. As the in denteris held at max i mum load for a de sired time, this pe riod en -ables to in ves ti gate creep. A sche matic il lus tra tion of a typ -i cal load-dis place ment curve is pre sented in Fig. 2. Therehave been de vel oped sev eral an a lyt i cal ap proaches for an a -lyz ing of the mea sured load-dis place ment data. NT600uses for eval u a tion of hard ness H and re duced modulus Er

the method by Ol i ver and Pharr [3], which ex tends the ap -proach by Doerner and Nix [4].

In most cases the three-sided py ram i dal Berkovich in -denter with an in cluded half-an gle of 65,27° is used. Its ge -om e try gives the same ra tio of pro jected area to in den ta tion depth as Vickers in denter (four-sided pyr a mid). TheBerkovich in denter is pre ferred for nanoindentation due tothe fact that three fac ets the o ret i cally con verge to a sin glepoint [5].

Oli ver-Pharr method

The most com mon method for eval u a tion of hard ness andre duced modulus from the load-dis place ment data ob tained with Berkovich in denter was pro posed by Ol i ver and Pharrin 1992. This pro ce dure con sists in the anal y sis of un load -ing pro cess schematically shown in Fig. 3.

The data anal y sis starts with fit ting the un load ing curveto the power-law re la tion

P h h fm= -a( ) , (1)

where P is the in den ta tion load, h is in den ta tion depth, hf isthe depth of re sid ual im pres sion af ter com plete un load ing,

and a, m are em pir i cal fit ting pa ram e ters. The un load ingstiff ness S is de fined as the ini tial slope of the un load ingcurve

SP

hm h h

h h

fm=

é

ëêù

ûú= -

=

-d

dmax

( )maxa 1 (2)

The widely used re la tion ship for re duced modulus Er

which re lates pro jected area A and con tact stiff ness S isgiven by

ES

AT =

p

2. (3)

Elas tic modulus of the spec i men E has the fol low ing re la -tion ship with the mea sured re duced modulus Er

1 1 12 2

E E ET i

=-

+-n n i , (4)

where Ei and ni are the elas tic modulus and Pois son’s

ra tio of the in denter, n is the Pois son’s ra tio of the spec i -

men, re spec tively. For di a mond, Ei = 1141 GPa and ni =0.07 [6].

Pro jected area of the in denter A is de fined as thecross-sec tional area at con tact depth hc, for ideal Berkovich in denter

A hc= 24 5 2. . (5)

Func tion that re lates pro jected area to the con tact depth iscalled Di a mond Area Func tion. Con tact depth hc is thedepth at which is re al ized con tact be tween side boards ofin denter and sam ple at max i mal load (Fig. 3). It can be es ti -mated af ter

h hP

Sc = -max

maxe . (6)

where Pmax is the peak load and e is geo met ri cal con stant,

for Berkovich in denter e = 0.75. In den ta tion hard ness HIT

is de fined as the mean con tact pres sure and is given by

HP

A hIT

c

= max

( ). (7)

Scratch test

Nano-Scratch test is one of the fun da men tal tests of me -chan i cal prop er ties at sub-mi cron scale and is used for their qual i ta tive and quan ti ta tive char ac ter iza tion. The test is re -al ized by the slid ing of a sty lus over the sam ple sur face un -

Ó Krystalografická spoleènost

R. Ètvrtlík, M. Stranyánek, P. Boháè, L. Jastrabík 91

Fig. 3. Sche matic rep re sen ta tion of the un load ing pro cess

Fig. 2. Sche matic il lus tra tion of the P-h curve.

Page 3: NanoTest™ NT600 - A DE VICE FOR ANAL Y SES OF ME CHAN I

der ei ther con stant or pro gres sively in creas ing load. Dur ing the whole ex per i ment the load and sty lus po si tion are con -tin u ously re corded. In con ven tional scratch test ing,scratches are gen er ated on the sam ple us ing a di a mond sty -lus usu ally a Rockwell [7]. For some spe cial mea sure mentthe Cube-cor ner in denter is used.

Dur ing scratch ing a num ber of var i ous pro cesses oc -curs in the sys tem coat ing-sub strate. It is gen er ally knownthat the fail ures of coat ing-sub strate sys tem in a scratch test arise ow ing to a com bi na tion of elasto- plas tic in den ta tionstresses, fric tional stresses and re sid ual in ter nal stress pres -ent in the coat ing [7]. The in creas ing load leads to de vel op -ment of mi cro-cracks, co he sion fail ures and delamination.The min i mum load at witch cracks oc cur is termed thelower crit i cal load Lc1 [8]. This value is called as crack ingre sis tance [10, 11], or scratch tough ness [12, 13]. The to taldelamination is char ac ter ized by the value Lc2, see Fig. 4.Some au thors de fine more crit i cal loads cor re spond ingwith oth ers per tur ba tions of the coat ing-sub strate sys tem.The goal of scratch test is to find these crit i cal loads Lc.NT600 can eval u ate these val ues in sev eral ways:

• by the de tec tion of abrupt change in pen e tra tiondepth,

• by a sud den change in the fric tional force be tweenthe sty lus and the sur face,

• by mi cro scopic ob ser va tion,• by means of acous tic emis sion.

Top o graphic test

Top o graphic test is per formed only with very low load. It is suit able for in ves ti ga tion of sur face re lief or film thick ness.

Multipass Wear Test

Abra sive wear per for mance can be es ti mated by means ofMultipass Wear Test (MWT), which is based on suc ces -sively al ter ing of scratches and to pog ra phy mea sure mentsover the same wear track. MWT uses a con stant load for the scratches so that slower fa tigue pro cesses (e.g. crackgrowth) can be in ves ti gated [1]. Some times for ad he sionmea sure ment the fric tion probe is used, so the fric tionprop er ties of the sur faces can be es ti mated. Sig nif i cant forNT600 is pos si bil ity of the si mul ta neous uti li za tion of thefric tion probe and acous tic emis sion trans ducer.

Dy namic prop er ties mea sure ment

In ves ti ga tion of me chan i cal prop er ties of thin films at static loads is gen er ally known. Uti li za tion of such re sults inprac tice, where the sur faces are ex posed to dy namic ef -fects, is prob lem at i cal. Of ten the ma te rial fail ure oc curssooner than pre dicted by static tests. That means that ma te -rial char ac ter iza tion in terms of in den ta tion (hard ness, elas -tic modulus, and creep) and scratch test is in prac ticein suf fi cient [13]. There fore the dy namic in ves ti ga tion ofthe sur faces for prac ti cal use is nec es sary. NT600 can mea -sure dy namic hard ness, frac ture and im pact re sis tance, per -form test ing of con tact fa tigue, ero sive wear or ad he sion.

For these pur poses NanoTest™ NT600 uti lizesNano-Im pact test. It is in es sence an ac cel er ated ul tra-lowload fa tigue wear test. The Nano-Im pact test is based on the sam ple os cil la tions which are gen er ated by spe cial pi ezo -

elec tric sam ple holder on which the spec i men is fixed. Im -pact test ing is es sen tial for sur faces where the abil ity towith stand re pet i tive con tact is crit i cal to the prod uct per for -mance. This tech nique is very use ful for de sign and pro cess op ti mi za tion of new high du ra bil ity thin films and coat ingstoo.

Cer tain mod i fi ca tion of Im pact test is Im pulse test. Themain dif fer ence be tween these two tech niques is a mo tiongen er a tion. Whereas the Im pact test is based on the sam plevi bra tions, the im pulse tech nique is based on pen du lum os -cil la tions (Fig. 5). In this case the pen du lum mo tion is gen -er ated elec tro mag net i cally by means of spe cial so le noidthat is sit u ated in the bot tom part of pen du lum, see Fig. 1.An other dif fer ence of these two tech niques is the max i -mum ap plied load. For Im pulse test the load is much lowerdue to to tally dif fer ent con struc tion prin ci ple. High cy cleex per i ments are com monly per formed by os cil lat ing thesam ple with Nano-Im pact test. For low-cy cle test with de -fined en ergy is used im pulse test. The in ves ti gated sur faces can be com pared in terms of these tests ac cord ing to threeba sic cri te ri ons: type of fail ure, time to fail ure and en ergyto fail ure.

Acous tic emis sion

Abrupt changes in ma te rial co he sion caused due to changes in state of stress are ac com pa nied by gen er a tion of tran sient acous tic waves (usu ally in the range of 150-300 kHz). Thisphe nom e non is re ferred as the acous tic emis sion and is de -tected by means of ul tra sonic sen sor. Or i gin and growth ofmicrocracks, in ter fa cial bond fail ure and delamination aretyp i cal ex am ples of events which pro duce acous tic emis -sion.

The uti li za tion of acous tic emis sion trans ducer al lowsob tain ing ad di tional de tailed in for ma tion on var i ous pro -cesses which oc cur dur ing in den ta tion or scratch test - of -ten till the fail ure is vis i ble. For acous tic emis sion de tec tion NanoTest™ NT600 uses pi ezo elec tric trans ducer that iscou pled with the mea sured spec i men.

Pin on disc tribometer

Pin on disc test ing is a tech nique usu ally used for in ves ti ga -tion of wear re sis tance and slid ing prop er ties of sur faces. The prin ci ple of the ex am i na tion is con tact of the di a mond

Ó Krystalografická spoleènost

92 NanoTest™ NT 600 - a de vice for anal y ses of me chan i cal prop er ties of ma te ri als

Fig. 4. Typ i cal re sult of scratch test. [8]

Page 4: NanoTest™ NT600 - A DE VICE FOR ANAL Y SES OF ME CHAN I

in denter with the in ves ti gated disc-shaped sam ple. Pin ondisc ex per i ment is based on con tin u ous mon i tor ing of co ef -fi cient of fric tion by fric tion probe dur ing slid ing pro cess.The main vari able pa ram e ters which af fect fric tion andwear are ve loc ity and ap plied load. NanoTest™ NT600 al -lows to ap ply con tin u ously in creas ing load in the rangefrom 0,1 mN to 20 N and max i mum ve loc ity 120 rev o lu tion per min ute. Ex cept the broad ex tent of ve loc ity and load ing force there are other ad van tages like ver ti cal disc ori en ta -tion so ma te rial particulates fall off. There is pos si ble de -fine the stop con di tions like max i mum load, depth orfric tion force, too.

Con clu sions

In this pa per the pos si bil i ties of NanoTest™ NT600 forme chan i cal prop er ties me trol ogy were de scribed. NT600 is a high-tech mea sure ment sys tem sig nif i cant by its pen du -lum-based con cept. Plat form al lows per form ing a num berof tests such as nanoindentation, high tem per a ture

nanoindentation, scratch test and re lated test, dy nam i caltests (im pact and im pulse test, dy namic hard ness mea sure -ment). Both pin on disc tribometer and acous tic emis siontrans ducer are also avail able. NT600 can mea sure hard -ness, eval u ate elas tic modulus, ad he sion, wear as well asfrac ture and dy namic prop er ties.

Ac knowl edge mentThis work was sup ported by In sti tu tional Re search PlanNo. AV0Z10100522.

Ref er ences

1. B.D. Beake, et al.: Mi cro Ma te ri als NanoTest User Man -

ual. Wrexham, 2004. Mi cro Ma te ri als Ltd.

2. A.C. Fischer-Cripps, Vac uum, 58 (2000) 569-585.

3. W.C. Ol i ver, G.M. Pharr, J. Ma ter. Res., 7 (1992)

1564-1583.

4. M.F. Doerner, W.D. Nix, J. Ma ter. Res., 1 (1986) 601-609.

5. T. Sawa, K. Tanaka, J. Ma ter. Res., 16 (2001) 3084-3096.

6. G. Simmons, H. Wang: Sin gle Crys tal Elas tic Con stantsand Cal cu lated Ag gre gate Prop er ties: A Hand book. Cam -bridge, MA, 1971. MIT Press.

7. N.X. Randall, G. Favaro, C.H. Frankel, Surf. Coat.

Technol., 137 (2001) 146-151.

8. S. Zhang, D. Sun, Y. Fu & H. Du, Surf. Coat. Technol.,

2004 (in print).

9. A.A. Voevodin, C. Rebholz, J.M. Schnei der, P. Stevenson,

A. Matthews, Surf. Coat. Technol., 73 (1995) 185-197.

10. E. Harrry, A. Rouzaud, P. Juliet, Y. Pauleau, M. Ignat,

Surf. Coat. Technol., 116-119 (1999) 172-175.

11. A.A. Voevodin, J.S. Zabinski, Thin Solid Films, 370 (2000)

223-231.

12. A.A. Voevodin, J.S. Zabinski, J. Ma ter. Sci., 33 (1998)

319.

13. B.D. Beake, S.R. Goodes, J.F. Smith, Surf. Eng., 17(2001)187-191.

Ó Krystalografická spoleènost

R. Ètvrtlík, M. Stranyánek, P. Boháè, L. Jastrabík 93

Fig. 5. Prin ci ple of pen du lum im pulse test ing.