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The Effect of Kinematic Conditions and Synovial Fluid Composition on the Frictional Behaviour of Materials for Artificial Joints

Abstract

The paper introduces an experimental investigation of frictional behaviour of materials used for joint replacements. The measurements were performed using a ball-on-disc tribometer, while four material combinations were tested; metal-on-metal, ceramic-on-ceramic, metal-on-polyethylene, and ceramic-on-polyethylene, respectively. The contact was lubricated by pure saline and various protein solutions. The experiments were realized at two mean speeds equal to 5.7 mm/s and 22 mm/s and two slide-to-roll ratios, -150% and 150%. It was found that the implant material is the fundamental parameter affecting friction. In general, the metal pair exhibited approximately two times higher friction compared to the ceramic. In particular, the friction in the case of the metal varied between 0.3 and 0.6 while the ceramic pair exhibited friction within the range from 0.15 to 0.3 at the end of the test. The lowest friction was observed for polyethylene while it decreased to 0.05 under some conditions. It can be also concluded that adding proteins to the lubricant has a positive impact on friction in the case of hard-on-hard pairs. For hard-on-soft pairs, no substantial influence of proteins was observed. The effect of kinematic conditions was found to be negligible in most cases.

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The Effect of Kinematic Conditions and Synovial Fluid Composition on the Frictional Behaviour of Materials for Artificial Joints

Author: Nečas, David; Vrbka, Martin; Křupka, Ivan; Hartl, Martin
Publisher: MDPI
Year: 2018
DOI: 10.3390/ma11050767
Source: https://dspace.vut.cz/bitstreams/dc3d02f0-354e-43e8-a638-1104abf24420/download
ma e ials
A icle
The E ec o Kinema ic Condi ions and Syno ial
Fluid Composi ion on he F ic ional Beha iou o
Ma e ials o A i icial Join s
Da id Neˇcas * ID , Ma in V bka, I an Kˇ upka and Ma in Ha l
Facul y o Mechanical Enginee ing, Ins i u e o Machine and Indus ial Design, B no Uni e si y o Technology,
Technická2896/2, 616 69 B no, Czech Republic; [email p o ec ed] (M.V.); [email p o ec ed].cz (I.K.);
[email p o ec ed] (M.H.)
*Co espondence: [email p o ec ed]; Tel.: +420-541-143-239
Recei ed: 23 Ap il 2018; Accep ed: 8 May 2018; Published: 10 May 2018


Abs ac :
The pape in oduces an expe imen al in es iga ion o ic ional beha iou o ma e ials used
o join eplacemen s. The measu emen s we e pe o med using a ball-on-disc ibome e , while ou
ma e ial combina ions we e es ed; me al-on-me al, ce amic-on-ce amic, me al-on-polye hylene, and
ce amic-on-polye hylene, espec i ely. The con ac was lub ica ed by pu e saline and a ious p o ein
solu ions. The expe imen s we e ealized a wo mean speeds equal o 5.7 mm/s and 22 mm/s and
wo slide- o- oll a ios,
−
150% and 150%. I was ound ha he implan ma e ial is he undamen al
pa ame e a ec ing ic ion. In gene al, he me al pai exhibi ed app oxima ely wo imes highe
ic ion compa ed o he ce amic. In pa icula , he ic ion in he case o he me al a ied be ween
0.3 and 0.6 while he ce amic pai exhibi ed ic ion wi hin he ange om 0.15 o 0.3 a he end o
he es . The lowes ic ion was obse ed o polye hylene while i dec eased o 0.05 unde some
condi ions. I can be also concluded ha adding p o eins o he lub ican has a posi i e impac on
ic ion in he case o ha d-on-ha d pai s. Fo ha d-on-so pai s, no subs an ial in luence o p o eins
was obse ed. The e ec o kinema ic condi ions was ound o be negligible in mos cases.
Keywo ds: join eplacemen ; ic ion; ma e ial; p o eins; kinema ic condi ions
1. In oduc ion
To al join a h oplas y is an e icien and well-es ablished su gical p ocedu e imp o ing he
li e o pa ien s su e ing om join diseases. Acco ding o he Heal h a a Glance 2015 epo [
1
],
161 ope a ions pe 100,000 inhabi an s we e pe o med in O ganisa ion o Economic Co-ope a ion and
De elopmen (OECD) coun ies in 2013. Howe e , despi e he apid imp o emen o he implan ed
ma e ials in he las ew decades [
2
], limi ed longe i y is s ill ecognized as he main d awback o
he eplacemen s. I should be highligh ed ha ailu e o he implan is accompanied by he need
o a e ising ope a ion, which is an economic bu den and subs an ially de e io a es he com o
o he pa ien . As he numbe o young ac i e people wi h a i icial join s s ill inc eases [
3
], i is
necessa y o ensu e a su icien se ice-li e o implan s o a oid any incon enience associa ed wi h i s
imp ope unc ion. Since he main cause o he ailu e is os eolysis [
4
] ollowed by asep ic loosening,
he ibological pe o mance o implan s has o be unde s ood in he con ex o he u he de elopmen
o eplacemen s.
Se e al aspec s ha e o be aken in o accoun conside ing ibological p ocesses wi hin a i icial
join con ac . Ma aki and Cann [
5
] employed a ball-on-disc con igu a ion when e alua ing he
coe icien o ic ion (CoF) as a unc ion o mean speed. Me al-on-me al con ac was in es iga ed,
while se e al es lub ican s we e es ed. In gene al, CoF was kep be ween 0.1 and 0.4 while he es
Ma e ials 2018,11, 767; doi:10.3390/ma11050767 www.mdpi.com/jou nal/ma e ials
Ma e ials 2018,11, 767 2 o 12
luid had a signi ican impac on esul s. I was ound ha bo ine se um (BS) and simple p o ein
solu ions lead o a educ ion o ic ion in a slow-speed egime. I was also highligh ed ha he choice
o bu e solu ion a ec s he lub ica ion condi ions. Finally, i was concluded ha ic ion as well as
lub ica ing ilm hickness a e ime and sliding-dis ance dependen , indica ing he impo ance o he
adso bed p o ein laye on he su aces.
One o he i s s udies which was ocused on he in luence o lub ican composi ion on ic ion
be ween polyme and me al su ac was unde aken by Yao e al. [
6
]. A pin-on-disk ibome e was
used o he e alua ion o CoF, while a ious es luids we e used as he lub ican s; pa icula ly
deionized wa e , dilu ed (25%, 50%, 75%) and undilu ed bo ine cal se um (BCS), bo ine syno ial
luid (SF) and human pe ip os he ic SF. A signi ican a iance o CoF esul s was obse ed, a ibu ed
mainly o he subs an ial changes o p o ein concen a ions and heological p ope ies o he luids.
The lowes ic ion (
≈
0.013) was exhibi ed by human SF ollowed by deionized wa e . Rema kably,
highe ic ion was de ec ed o bo ine SF and undilu ed BCS (
≈
0.024). The highes CoF was de ec ed
o 25% BCS, which was a ound 0.028. Scholes and Unswo h [
7
] demons a ed he impo ance o
lub ican composi ion in ela ion o he ma e ial combina ion o he implan s. The au ho s es ed
a ious model luids inding ha he highes ic ion can be de ec ed in he case o me al-me al implan s.
No signi ican di e ence be ween he ce amic-ce amic and me al-polye hylene pai was obse ed.
Al hough he e was a apid in luence o he model luid on he CoF, he e ec o p o eins could no
be gene alized, since bo h dec ease and inc ease o ic ion could be obse ed dependen on implan
ma e ial. The ole o indi idual cons i uen s con ained in SF was demons a ed by Sawae e al. [
8
].
The con ac be ween an ul a-high molecula weigh polye hylene (UHMWPE) pin sliding agains
me al/ce amic disc was s udied, while a clea posi i e e ec o hyalu onic acid added o saline solu ion
on ic ion was de ec ed.
Mo eo e , i was well epo ed ha he ic ional beha iou o he con ac pai is subs an ially
in luenced by he su ace condi ions. Widme e al. [
9
], in es iga ed he ce amic-polye hylene sliding
pai , inding ha he oxygen-plasma based ea men o polye hylene (PE) led o imp o ed abili ies o
p o ein adso p ion on o ubbing su aces, hus educing bo h s a ic and dynamic ic ion. Subsequen ly,
i was poin ed ou ha con o ma ional changes ha e o be aken in o accoun [
10
]. The au ho s
showed ha hyd ophilic na u e o he su aces suppo s adso p ion o he p o eins in a na i e s a e,
o ming hicke lub ica ing ilm leading o lowe ic ion be ween he componen s. An ex ensi e
in es iga ion o he e ec o model luid composi ion on CoF dependen on kinema ic condi ions was
p o ided in ou p e ious s udy [
11
]. Recip oca ing pin-on-pla e (me al-UHMWPE) es was conduc ed,
showing ha he kinema ic condi ions ha e a c ucial impac on he con o ma ional changes o p o eins,
hus in luencing ic ional beha iou o he con ac pai . A a slow speed egime (10 mm/s), a e y
sligh inc ease o ic ion wi h inc easing p o ein concen a ion was obse ed o bo h albumin and
γ
-globulin solu ion. The highes ic ion occu ed when a mix u e o he men ioned p o eins was
used as he es lub ican . An inc ease o sliding speed o 50 mm/s caused jus a negligible change o
ic ion. Independen o sliding speed, CoF was subs an ially highe when compa ing p o ein solu ions
(
≈
0.17–0.27) wi h phospha e-bu e ed saline (PBS) wi hou any cons i uen s. In ha case, ic ion was
lowe han 0.05. These esul s a e in good ag eemen wi h he obse a ion p o ided p e iously [
12
,
13
].
In he s udy men ioned, he e ec o albumin unde going con o ma ional changes on he ic ion
be ween he UHMWPE pin and s ainless s eel pla e was e alua ed. A subs an ial e ec o he applied
load on he esul s was obse ed; while a low loads, pos - ic ion deg aded albumin added o PBS led
o a dec ease o ic ion compa ed o esh p o ein. The opposi e beha iou occu ed a highe loads.
Based on he abo e e e ences [
11
,
12
], i can be concluded ha ic ion be ween he ubbing su aces is
a ec ed by bo h kinema ic and loading condi ions.
The e ec o eplacemen geome y has o be aken in o accoun as well. Dowson e al. [
14
]
conduc ed a p edic i e nume ical analysis o ic ion and wea o me al-me al implan , inding ha
he ic ional o que inc eases wi h inc easing nominal diame e ; howe e , i is a ec ed jus a li le by
he ini ial clea ance be ween he su aces. An expe imen al s udy o he e ec o diame ic clea ance
Ma e ials 2018,11, 767 3 o 12
oge he wi h he ole o model luid was unde aken by B ocke e al. [
15
]. Nominal diame e o he
implan was 54.6 mm, while h ee di e en clea ances we e conside ed; 53
µ
m, 94
µ
m, and 194
µ
m,
espec i ely. The lowes ic ion ac o was de ec ed o he medium size o he clea ance. Lowe ing
he clea ance led o a negligible inc ease o ic ion; howe e , in he case o he highes clea ance,
a subs an ial inc ease o ic ion o almos double was de ec ed. Rega ding he model luid, 25% and
100% BS we e es ed, wi h he inding ha lowe ic ion could be eached in he case o highe p o ein
concen a ion, in gene al, which is in a good ag eemen wi h one o he p e ious s udies [
6
]. Finally,
an expe imen al in es iga ion o he ic ion coe icien using a pendulum hip join simula o ocusing
on he e ec o implan ma e ial and diame e was conduc ed by V bka e al. [
16
]. This applied
25% BS o a o al p o ein concen a ion o 22.4 mg/mL, es ing 28 mm and 36 mm me al-UHMWPE,
ce amic-UHMWPE and ce amic-ce amic pai s. The highes CoF (
≈
0.16) was de ec ed in he case o he
me al-UHMWPE pai wi h no clea e ec o nominal diame e . Ce amic-UHMWPE exhibi ed lowe
ic ion (
≈
0.14), while a la ge diame e led o a u he dec ease (
≈
0.13). The lowes ic ion (0.12)
was de ec ed in he ce amic-ce amic pai wi h he same e ec o diame e as in he p e ious case.
Based on he abo e e e ences, i is appa en ha he ibological beha iou o a i icial join s
is in luenced by se e al aspec s, such as composi ion o he model SF, implan ma e ial, geome y,
kinema ic and loading condi ions. Howe e , mos o he au ho s ocused on one pa icula ma e ial
combina ion o speci ic composi ion o he es lub ican . The e o e, he aim o he p esen pape is o
p o ide a de ailed analysis o ic ional beha iou conside ing a ious implan ma e ials, kinema ic
condi ions, and he composi ion o model syno ial luid. Acco ding o he au ho s’ bes knowledge,
such an ex ensi e in es iga ion has no been pe o med be o e.
2. Ma e ials and Me hods
The measu emen s o he CoF we e conduc ed u ilizing a comme cial ball-on-disc es de ice
Mini T ac ion Machine (MTM, PCS Ins umen s, London, Uni ed Kingdom). Bo h he componen s, he
ball and he disc, could be d i en independen ly, hus enabling he applica ion o a ious kinema ic
condi ions. The mean dynamic (some imes also called kine ic o sliding) ic ion coe icien [
17
]
is e alua ed based on he a io o ic ion and no mal o ce measu ed by he load cell. CoF was
e alua ed wi h he acquisi ion equency o 0.1 Hz. A con ac pai consis ed o me al (cobal -ch omium-
molybdenum—CoC Mo) and alumina ce amic balls o diame e 19.05 mm sliding agains 46 mm-
diame e discs o me al, ce amic, and highly-c osslinked PE (HXPE), espec i ely. The hickness o he
discs was 6 mm. A schema ic illus a ion o he measu emen con igu a ion is displayed in Figu e 1.
Ini ial su ace opog aphy o he es specimens was checked using he phase-shi ing in e e ome y
me hod (Con ou GT-X8, B uke , Bille ica, MA, USA). Fi e poin s which we e expec ed o be in he
con ac d ag o each sample we e measu ed, while he su ace oughness esul s a e shown in Table 1.
To cla i y he e ec o kinema ic condi ions, he expe imen s we e ealized unde wo di e en
mean speeds, 5.7 mm/s and 22 mm/s. Mean speed ep esen s he a e age alue o he ball and he disc
speed unde a ious olling/sliding condi ions. In he ollowing ex , he e ms posi i e and nega i e
sliding a e used. In he case o nega i e sliding, he ball o a es as e han he disc. By con as , unde
posi i e sliding he disc is as e . The cou se o he speeds o he indi idual componen s conside ing
nega i e and posi i e sliding is demons a ed using he ed a ows in he bo om pa o Figu e 1.
Rega ding he human body, i can be assumed ha he hip join ope a es unde pu e nega i e sliding
condi ions, which means ha he cup is s a iona y, while he head o a es. Conside ing he ball-on-disc
con igu a ion, pu e sliding ep esen s bi se e e condi ions and so signi ican wea o he samples
appa en ly in luencing he esul s o CoF could be expec ed. The e o e, he expe imen s we e ealized
unde pa ial sliding o 150%. To a oid inaccu acies coming om he slippage o he componen s,
he es s we e ealized unde bo h posi i e (150%) and nega i e (
−
150%) sliding. The slide- o- oll
a io (SRR) which de e mines he le el o slip, can be easily de e mined ollowing he equa ion
SRR = 2(u
D−
u
B
)/(u
D
+ u
B
), whe e u
d
is he speed o he disc and u
b
is he speed o he ball. Combined
olling/sliding condi ions no mally occu in he knee join ; howe e , i should be highligh ed ha he
Ma e ials 2018,11, 767 4 o 12
p esen s udy is no ocused on one pa icula join ype, bu on he gene al assessmen o ic ional
beha iou o ma e ials used o join implan s. Applied load was 0.5 N in he case o he me al and 0.4
in he case o he ce amic balls, leading o he ollowing con ac p essu es: me al-on-me al (264.7 MPa),
me al-HXPE (9.9 MPa), ce amic-ce amic (280.5 MPa), ce amic-HXPE (9.5 MPa).
Ma e ials 2018, 11, x FOR PEER REVIEW 4 o 12
howe e , i should be highligh ed ha he p esen s udy is no ocused on one pa icula join ype,
bu on he gene al assessmen o ic ional beha iou o ma e ials used o join implan s. Applied
load was 0.5 N in he case o he me al and 0.4 in he case o he ce amic balls, leading o he
ollowing con ac p essu es: me al-on-me al (264.7 MPa), me al-HXPE (9.9 MPa), ce amic-ce amic
(280.5 MPa), ce amic-HXPE (9.5 MPa).
Figu e 1. Schema ic illus a ion o he measu emen con igu a ion.
Table 1. Su ace opog aphy pa ame e s o he es samples.
Pa ame e Ball Disc
- Me al Ce amic Me al Ce amic HXPE
A e age su ace oughness Ra (μm) 0.087 0.035 0.008 0.998 0.841
S anda d de ia ion SD (μm) ±0.00587 ±0.00414 ±0.00039 ±0.10707 ±0.13631
The main in e es o he cu en s udy was in he e ec o he composi ion o model luid.
The e o e, i e es lub ican s we e p epa ed while he esul s we e compa ed wi h hose o pu e
PBS. The model luids con ained he dominan p o eins o SF; albumin and γ-globulin, espec i ely.
Lub ican s we e p epa ed 24 h p io o he es s and we e s o ed in a e ige a o o enable a
comple e solu ion o he p o eins in PBS. Bo ine se um albumin (9048-46-8, Biomol GmbH,
Hambu g, Ge many) and γ-globulin om human blood (G4386, Sigma Ald ich, Da ms ad ,
Ge many) we e added o PBS in a ious concen a ions, while he simple p o ein solu ions we e
in es iga ed as well. A summa y o he es luids is p o ided in Table 2. Despi e he abili y o he
es de ice o con ol he empe a u e o he po , he expe imen s we e ealized unde ambien
labo a o y empe a u e o 22 °C, since i was p e iously e e enced in li e a u e ha he inc ease o
body empe a u e does no in luence he esul s subs an ially [18]. The expe imen s we e conduc ed
unde ully looded condi ions o a oid any e ec s coming om s a a ion o he con ac . Eigh y
expe imen s we e ealized in o al, while Table 3 p o ides he comple e o e iew o he pe o med
es s o be e o ien a ion. The de ailed in o ma ion abou he speeds o he ball and he disc du ing
a ious es s is gi en in Table 4. Random es s we e conduc ed h ee imes o check he epea abili y
o he esul s. Since he e was excellen da a ag eemen in e ms o bo h he ends and he absolu e
alues o CoF (s anda d de ia ion no la ge han 0.04), he es o he expe imen s we e pe o med
only once.
Figu e 1. Schema ic illus a ion o he measu emen con igu a ion.
Table 1. Su ace opog aphy pa ame e s o he es samples.
Pa ame e Ball Disc
- Me al Ce amic Me al Ce amic HXPE
A e age su ace oughness Ra (µm) 0.087 0.035 0.008 0.998 0.841
S anda d de ia ion SD (µm) ±0.00587 ±0.00414 ±0.00039 ±0.10707 ±0.13631
The main in e es o he cu en s udy was in he e ec o he composi ion o model luid.
The e o e, i e es lub ican s we e p epa ed while he esul s we e compa ed wi h hose o pu e
PBS. The model luids con ained he dominan p o eins o SF; albumin and
γ
-globulin, espec i ely.
Lub ican s we e p epa ed 24 h p io o he es s and we e s o ed in a e ige a o o enable a comple e
solu ion o he p o eins in PBS. Bo ine se um albumin (9048-46-8, Biomol GmbH, Hambu g, Ge many)
and
γ
-globulin om human blood (G4386, Sigma Ald ich, Da ms ad , Ge many) we e added o PBS
in a ious concen a ions, while he simple p o ein solu ions we e in es iga ed as well. A summa y o
he es luids is p o ided in Table 2. Despi e he abili y o he es de ice o con ol he empe a u e
o he po , he expe imen s we e ealized unde ambien labo a o y empe a u e o 22
◦
C, since i
was p e iously e e enced in li e a u e ha he inc ease o body empe a u e does no in luence he
esul s subs an ially [
18
]. The expe imen s we e conduc ed unde ully looded condi ions o a oid
any e ec s coming om s a a ion o he con ac . Eigh y expe imen s we e ealized in o al, while
Table 3p o ides he comple e o e iew o he pe o med es s o be e o ien a ion. The de ailed
in o ma ion abou he speeds o he ball and he disc du ing a ious es s is gi en in Table 4. Random
es s we e conduc ed h ee imes o check he epea abili y o he esul s. Since he e was excellen
da a ag eemen in e ms o bo h he ends and he absolu e alues o CoF (s anda d de ia ion no
la ge han 0.04), he es o he expe imen s we e pe o med only once.
Ma e ials 2018,11, 767 5 o 12
Table 2. Summa y o he applied model luids.
Model Syno ial
Fluid (MSF) Volume (mL) P o ein Con en (mg/mL) To al P o ein
Concen a ion (mg/mL)
- - Albumin γ-globulin -
Alb70+Glob35 10 7 3.5 10.5
Alb35+Glob70 10 3.5 7 10.5
Alb140+Glob70 10 14 7 21
Albumin70 10 7 - 7
γ-globulin35 10 - 3.5 3.5
PBS 10 - - -
Table 3. O e iew o he pe o med expe imen s.
Expe imen Se Ma e ial Combina ion Mean Speed
(mm/s)
Slide-To-Roll
Ra io (%) Model Syno ial Fluid
1Me al-on-Me al
(MoM) 5.7; 22 150; −150
Alb70+Glob35;
Alb35+Glob70;
Alb140+Glob70; PBS
2
Me al-on-highly c osslinked
polye hylene (HXPE)
(MoP)
5.7; 22 150; −150
Alb70+Glob35;
Alb35+Glob70;
Alb140+Glob70; PBS
3Ce amic-on-Ce amic
(CoC) 5.7; 22 150; −150
Alb70+Glob35;
Alb35+Glob70;
Alb140+Glob70; PBS
4Ce amic-on-HXPE
(CoP) 5.7; 22 150; −150
Alb70+Glob35;
Alb35+Glob70;
Alb140+Glob70; PBS
5 MoM 22 150; −150 Albumin70;
γ-globulin35
6 MoP 22 150; −150 Albumin70;
γ-globulin35
7 CoC 22 150; −150 Albumin70;
γ-globulin35
8 CoP 22 150; −150 Albumin70;
γ-globulin35
Table 4. A de ailed o e iew o he kinema ic condi ions.
Slide-To-Roll Ra io (%) Mean Speed (mm/s) Ball Speed (mm/s) Disc Speed (mm/s)
−150 5.7 9.975 1.425
−150 22 38.5 5.5
150 5.7 1.425 9.975
150 22 5.5 38.5
3. Resul s and Discussion
3.1. The E ec o Ma e ial and Kinema ic Condi ions
Ini ially, he expe imen s we e pe o med wi h pu e PBS o all he ma e ial combina ions,
conside ing bo h posi i e and nega i e sliding a lowe (5.7 mm/s) and highe (22 mm/s) speed.
The esul s showed ha independen o kinema ic condi ions, he MoM combina ion exhibi s he
highes ic ion; howe e , his e ec was signi ican mainly unde nega i e sliding, when he ic ion
a he end o he expe imen eached almos 0.6. By con as , he lowes ic ion was de ec ed o
MoP and CoP, while in he case o CoP, he ic ion le el was less han 0.1, pa icula ly a ound
0.05 o he dominan pe iod o he expe imen s, which is in a good co ela ion wi h p e ious
obse a ions [
11
,
19
,
20
]. CoC ic ional beha iou was ound o be somewhe e be ween, while he
ic ion eached abou 0.25. Ne e heless, i should be aken in o accoun ha he su ace oughness o

Ma e ials 2018,11, 767 6 o 12
he employed ce amic disc was an o de o magni ude highe han he su ace o he ball, which could
a ec he esul s. Based on he p e ious indings, i migh be expec ed ha i ealis ic oughness o he
disc could be achie ed, he ic ion coe icien would be lowe . Howe e , wi hou he expe imen al
esul s, he po en ial le el o CoF educ ion can be only es ima ed. Ne e heless, i should be
emphasized ha he p esen s udy is a he compa a i e, no p edic ing he ic ion wi hin eal
implan s. Wi h he excep ion o MoM unde posi i e sliding condi ions, he e was no a subs an ial
e ec o speed. Conside ing he e ec o ime, only in he case o MoM was he de elopmen o ic ion
wi h ime obse ed. Fo he es o he ma e ial combina ions, CoF was s able wi hou any luc ua ions
o e he en i e expe imen . All he esul s can be seen in Figu e 2. I should be no ed ha e en he
acquisi ion equency was 0.1 Hz; o be e cla i y o he esul s, he plo ed do s ep esen a e age
CoF in pa icula ime s eps (1 s, 15 s, 30 s
. . .
300 s). The inse igu es a e shown o illus a e he
kinema ic condi ions. The ed a ows ep esen he speed cou se.
Ma e ials 2018, 11, x FOR PEER REVIEW 6 o 12
could be achie ed, he ic ion coe icien would be lowe . Howe e , wi hou he expe imen al
esul s, he po en ial le el o CoF educ ion can be only es ima ed. Ne e heless, i should be
emphasized ha he p esen s udy is a he compa a i e, no p edic ing he ic ion wi hin eal
implan s. Wi h he excep ion o MoM unde posi i e sliding condi ions, he e was no a subs an ial
e ec o speed. Conside ing he e ec o ime, only in he case o MoM was he de elopmen o
ic ion wi h ime obse ed. Fo he es o he ma e ial combina ions, CoF was s able wi hou any
luc ua ions o e he en i e expe imen . All he esul s can be seen in Figu e 2. I should be no ed
ha e en he acquisi ion equency was 0.1 Hz; o be e cla i y o he esul s, he plo ed do s
ep esen a e age CoF in pa icula ime s eps (1 s, 15 s, 30 s … 300 s). The inse igu es a e shown o
illus a e he kinema ic condi ions. The ed a ows ep esen he speed cou se.
Figu e 2. De elopmen o coe icien o ic ion (CoF) as a unc ion o ime o ou ma e ial
combina ions a lowe and highe mean speed unde nega i e (a) and posi i e (b) sliding condi ions.
Con ac is lub ica ed by phospha e-bu e ed saline (PBS).
Adding he p o eins in o he saline solu ion in ela i ely low concen a ion (10.5 mg/mL in
o al) led o a sligh change o CoF e olu ion, see Figu es 3 and 4 Compa ed o he pu e PBS esul s,
ime-dependen beha iou was obse ed o MoM and also o CoC con ac pai s, while he
maximum a he end o he es was om 0.3 o 0.4 o me al. Fo ce amic, he ic ion le el was abou
0.2, while he e y same beha iou was obse ed in li e a u e, whe e he con ac o a ce amic ball
sliding agains a ce amic pla e lub ica ed by BS was analyzed [21]. To de e mine he in luence o
luid composi ion, i can be seen ha e en i he concen a ion o albumin and γ-globulin was
swi ched, see Figu e 3 s. Figu e 4, almos he same esul s could be ob ained o mos o he
ma e ials and kinema ic condi ions. Only in he case o MoP did highe con en o γ-globulin lead o
a dec ease o ic ion, as can be seen in Figu e 4a.
Figu e 3. De elopmen o CoF as a unc ion o ime o ou ma e ial combina ions a lowe and
highe mean speed unde nega i e (a) and posi i e (b) sliding condi ions. Con ac is lub ica ed by
model luid Alb70+Glob35.
Figu e 2.
De elopmen o coe icien o ic ion (CoF) as a unc ion o ime o ou ma e ial
combina ions a lowe and highe mean speed unde nega i e (
a
) and posi i e (
b
) sliding condi ions.
Con ac is lub ica ed by phospha e-bu e ed saline (PBS).
Adding he p o eins in o he saline solu ion in ela i ely low concen a ion (10.5 mg/mL in
o al) led o a sligh change o CoF e olu ion, see Figu es 3and 4Compa ed o he pu e PBS esul s,
ime-dependen beha iou was obse ed o MoM and also o CoC con ac pai s, while he maximum
a he end o he es was om 0.3 o 0.4 o me al. Fo ce amic, he ic ion le el was abou 0.2, while he
e y same beha iou was obse ed in li e a u e, whe e he con ac o a ce amic ball sliding agains a
ce amic pla e lub ica ed by BS was analyzed [
21
]. To de e mine he in luence o luid composi ion, i
can be seen ha e en i he concen a ion o albumin and
γ
-globulin was swi ched, see Figu e 3 s.
Figu e 4, almos he same esul s could be ob ained o mos o he ma e ials and kinema ic condi ions.
Only in he case o MoP did highe con en o
γ
-globulin lead o a dec ease o ic ion, as can be seen
in Figu e 4a.
Ma e ials 2018, 11, x FOR PEER REVIEW 6 o 12
could be achie ed, he ic ion coe icien would be lowe . Howe e , wi hou he expe imen al
esul s, he po en ial le el o CoF educ ion can be only es ima ed. Ne e heless, i should be
emphasized ha he p esen s udy is a he compa a i e, no p edic ing he ic ion wi hin eal
implan s. Wi h he excep ion o MoM unde posi i e sliding condi ions, he e was no a subs an ial
e ec o speed. Conside ing he e ec o ime, only in he case o MoM was he de elopmen o
ic ion wi h ime obse ed. Fo he es o he ma e ial combina ions, CoF was s able wi hou any
luc ua ions o e he en i e expe imen . All he esul s can be seen in Figu e 2. I should be no ed
ha e en he acquisi ion equency was 0.1 Hz; o be e cla i y o he esul s, he plo ed do s
ep esen a e age CoF in pa icula ime s eps (1 s, 15 s, 30 s … 300 s). The inse igu es a e shown o
illus a e he kinema ic condi ions. The ed a ows ep esen he speed cou se.
Figu e 2. De elopmen o coe icien o ic ion (CoF) as a unc ion o ime o ou ma e ial
combina ions a lowe and highe mean speed unde nega i e (a) and posi i e (b) sliding condi ions.
Con ac is lub ica ed by phospha e-bu e ed saline (PBS).
Adding he p o eins in o he saline solu ion in ela i ely low concen a ion (10.5 mg/mL in
o al) led o a sligh change o CoF e olu ion, see Figu es 3 and 4 Compa ed o he pu e PBS esul s,
ime-dependen beha iou was obse ed o MoM and also o CoC con ac pai s, while he
maximum a he end o he es was om 0.3 o 0.4 o me al. Fo ce amic, he ic ion le el was abou
0.2, while he e y same beha iou was obse ed in li e a u e, whe e he con ac o a ce amic ball
sliding agains a ce amic pla e lub ica ed by BS was analyzed [21]. To de e mine he in luence o
luid composi ion, i can be seen ha e en i he concen a ion o albumin and γ-globulin was
swi ched, see Figu e 3 s. Figu e 4, almos he same esul s could be ob ained o mos o he
ma e ials and kinema ic condi ions. Only in he case o MoP did highe con en o γ-globulin lead o
a dec ease o ic ion, as can be seen in Figu e 4a.
Figu e 3. De elopmen o CoF as a unc ion o ime o ou ma e ial combina ions a lowe and
highe mean speed unde nega i e (a) and posi i e (b) sliding condi ions. Con ac is lub ica ed by
model luid Alb70+Glob35.
Figu e 3.
De elopmen o CoF as a unc ion o ime o ou ma e ial combina ions a lowe and highe
mean speed unde nega i e (
a
) and posi i e (
b
) sliding condi ions. Con ac is lub ica ed by model luid
Alb70+Glob35.
Ma e ials 2018,11, 767 7 o 12
Ma e ials 2018, 11, x FOR PEER REVIEW 7 o 12
Figu e 4. De elopmen o CoF as a unc ion o ime o ou ma e ial combina ions a lowe and
highe mean speed unde nega i e (a) and posi i e (b) sliding condi ions. Con ac is lub ica ed by
model luid Alb35+Glob70.
An inc ease o p o ein concen a ion o 21 mg/mL led o a e y sligh inc ease o ic ion o
ce amic and me al pai s. In he case o MoP and CoP, he ic ion emained he same o dec eased a
li le bi . Howe e , since he change is negligible, see Figu es 3 and 4 s. Figu e 5, i can be concluded
ha he p o ein con en does no play an impo an ole ega ding hese so-called ha d-on-so
bea ing pai s. Finally, ocusing on he pa icula ma e ial combina ions, i can be seen ha he
beha iou co esponds well o he pu e PBS esul s, while he highes ic ion is exhibi ed by MoM,
ollowed by CoC, MoP and CoP (Figu es 2–5). The highes ic ion in he case o me al-me al con ac
was epo ed also by Scholes and Unswo h [7]. Ne e heless, i should be no ed ha he esul s do
no comple ely co espond o obse a ions p o ided by V bka e al. [16], who de e mined he
ic ion coe icien o a ious implan pai s. In he e e ence, he au ho s measu ed he lowes
ic ion when conside ing a ce amic head sliding agains a ce amic cup. Howe e , i mus be no ed
ha di e en expe imen al condi ions we e employed; in pa icula , BS was employed as he es
lub ican , and he expe imen s we e ealized in di e en geome ical con igu a ions. Mo eo e , as
men ioned abo e, he oughness o ce amic discs used in he p esen s udy was an o de o magni ude
highe han is he oughness o eal ace abula cups, which can also play a signi ican ole.
Figu e 5. De elopmen o CoF as a unc ion o ime o ou ma e ial combina ions a lowe and
highe mean speed unde nega i e (a) and posi i e (b) sliding condi ions. Con ac is lub ica ed by
model luid Alb140+Glob70.
3.2. The E ec o Model Syno ial Fluid Composi ion
To clea ly iden i y he e ec o model SF composi ion on ic ional beha iou , he addi ional
es s we e pe o med a highe speed conside ing he simple p o ein solu ions o albumin and
γ-globulin as well. The esul s o indi idual ma e ial combina ions a e displayed in Figu es 6–9,
espec i ely. Fo MoM con ac , i can be seen ha he esul s o pu e PBS a e in luenced by he
posi i i y/nega i i y o sliding. Unde nega i e sliding, he le el o ic ion is conside ably highe
(a ound 0.6 a maximum) o PBS compa ed o p o ein solu ion (a ound 0.4). In e ms o indi idual
luids, albumin-con aining lub ican exhibi ed he lowes ic ion, app oxima ely 0.37. Fo he es o
he lub ican s, he e is no clea impac on lub ica ion, while he ic ion is kep be ween 0.4 and 0.43
Figu e 4.
De elopmen o CoF as a unc ion o ime o ou ma e ial combina ions a lowe and highe
mean speed unde nega i e (
a
) and posi i e (
b
) sliding condi ions. Con ac is lub ica ed by model luid
Alb35+Glob70.
An inc ease o p o ein concen a ion o 21 mg/mL led o a e y sligh inc ease o ic ion o
ce amic and me al pai s. In he case o MoP and CoP, he ic ion emained he same o dec eased a
li le bi . Howe e , since he change is negligible, see Figu es 3and 4 s. Figu e 5, i can be concluded
ha he p o ein con en does no play an impo an ole ega ding hese so-called ha d-on-so bea ing
pai s. Finally, ocusing on he pa icula ma e ial combina ions, i can be seen ha he beha iou
co esponds well o he pu e PBS esul s, while he highes ic ion is exhibi ed by MoM, ollowed by
CoC, MoP and CoP (Figu es 2–5). The highes ic ion in he case o me al-me al con ac was epo ed
also by Scholes and Unswo h [
7
]. Ne e heless, i should be no ed ha he esul s do no comple ely
co espond o obse a ions p o ided by V bka e al. [
16
], who de e mined he ic ion coe icien o
a ious implan pai s. In he e e ence, he au ho s measu ed he lowes ic ion when conside ing a
ce amic head sliding agains a ce amic cup. Howe e , i mus be no ed ha di e en expe imen al
condi ions we e employed; in pa icula , BS was employed as he es lub ican , and he expe imen s
we e ealized in di e en geome ical con igu a ions. Mo eo e , as men ioned abo e, he oughness o
ce amic discs used in he p esen s udy was an o de o magni ude highe han is he oughness o eal
ace abula cups, which can also play a signi ican ole.
Ma e ials 2018, 11, x FOR PEER REVIEW 7 o 12
Figu e 4. De elopmen o CoF as a unc ion o ime o ou ma e ial combina ions a lowe and
highe mean speed unde nega i e (a) and posi i e (b) sliding condi ions. Con ac is lub ica ed by
model luid Alb35+Glob70.
An inc ease o p o ein concen a ion o 21 mg/mL led o a e y sligh inc ease o ic ion o
ce amic and me al pai s. In he case o MoP and CoP, he ic ion emained he same o dec eased a
li le bi . Howe e , since he change is negligible, see Figu es 3 and 4 s. Figu e 5, i can be concluded
ha he p o ein con en does no play an impo an ole ega ding hese so-called ha d-on-so
bea ing pai s. Finally, ocusing on he pa icula ma e ial combina ions, i can be seen ha he
beha iou co esponds well o he pu e PBS esul s, while he highes ic ion is exhibi ed by MoM,
ollowed by CoC, MoP and CoP (Figu es 2–5). The highes ic ion in he case o me al-me al con ac
was epo ed also by Scholes and Unswo h [7]. Ne e heless, i should be no ed ha he esul s do
no comple ely co espond o obse a ions p o ided by V bka e al. [16], who de e mined he
ic ion coe icien o a ious implan pai s. In he e e ence, he au ho s measu ed he lowes
ic ion when conside ing a ce amic head sliding agains a ce amic cup. Howe e , i mus be no ed
ha di e en expe imen al condi ions we e employed; in pa icula , BS was employed as he es
lub ican , and he expe imen s we e ealized in di e en geome ical con igu a ions. Mo eo e , as
men ioned abo e, he oughness o ce amic discs used in he p esen s udy was an o de o magni ude
highe han is he oughness o eal ace abula cups, which can also play a signi ican ole.
Figu e 5. De elopmen o CoF as a unc ion o ime o ou ma e ial combina ions a lowe and
highe mean speed unde nega i e (a) and posi i e (b) sliding condi ions. Con ac is lub ica ed by
model luid Alb140+Glob70.
3.2. The E ec o Model Syno ial Fluid Composi ion
To clea ly iden i y he e ec o model SF composi ion on ic ional beha iou , he addi ional
es s we e pe o med a highe speed conside ing he simple p o ein solu ions o albumin and
γ-globulin as well. The esul s o indi idual ma e ial combina ions a e displayed in Figu es 6–9,
espec i ely. Fo MoM con ac , i can be seen ha he esul s o pu e PBS a e in luenced by he
posi i i y/nega i i y o sliding. Unde nega i e sliding, he le el o ic ion is conside ably highe
(a ound 0.6 a maximum) o PBS compa ed o p o ein solu ion (a ound 0.4). In e ms o indi idual
luids, albumin-con aining lub ican exhibi ed he lowes ic ion, app oxima ely 0.37. Fo he es o
he lub ican s, he e is no clea impac on lub ica ion, while he ic ion is kep be ween 0.4 and 0.43
Figu e 5.
De elopmen o CoF as a unc ion o ime o ou ma e ial combina ions a lowe and highe
mean speed unde nega i e (
a
) and posi i e (
b
) sliding condi ions. Con ac is lub ica ed by model luid
Alb140+Glob70.
3.2. The E ec o Model Syno ial Fluid Composi ion
To clea ly iden i y he e ec o model SF composi ion on ic ional beha iou , he addi ional es s
we e pe o med a highe speed conside ing he simple p o ein solu ions o albumin and
γ
-globulin
as well. The esul s o indi idual ma e ial combina ions a e displayed in Figu es 6–9, espec i ely.
Fo MoM con ac , i can be seen ha he esul s o pu e PBS a e in luenced by he posi i i y/nega i i y
o sliding. Unde nega i e sliding, he le el o ic ion is conside ably highe (a ound 0.6 a maximum)
o PBS compa ed o p o ein solu ion (a ound 0.4). In e ms o indi idual luids, albumin-con aining
lub ican exhibi ed he lowes ic ion, app oxima ely 0.37. Fo he es o he lub ican s, he e is
Ma e ials 2018,11, 767 8 o 12
no clea impac on lub ica ion, while he ic ion is kep be ween 0.4 and 0.43 a he end o he es ,
see Figu e 6a. Conside ing he posi i e sliding condi ions, he CoF de elopmen is sligh ly di e en .
The highes ic ion o e he dominan pa o he expe imen was exhibi ed by he solu ion wi h
ela i ely high p o ein con en . Howe e , a e 75 s, he ic ion was s abilized a abou 0.4 wi hou any
u he ime-dependen change. The cou se o ic ion o saline solu ion is linea ly inc easing ( he
same beha iou as unde nega i e sliding), eaching 0.45 a he end. Fo he o he p o ein solu ions,
he beha iou is almos he same, wi h he excep ion o lub ican con aining 70 mg/mL o albumin
and 35 mg/mL o
γ
-globulin, which exhibi s he lowes ic ion. This can be a ibu ed o he ac ion o
he p o ein ilm. I was obse ed in li e a u e ha , conside ing he same model luid as in he case o
he p esen s udy, a me al head o med much hicke p o ein ilm unde posi i e sliding, which can
lead o a dec ease o ic ion be ween he su aces [22].
Ma e ials 2018, 11, x FOR PEER REVIEW 8 o 12
a he end o he es , see Figu e 6a. Conside ing he posi i e sliding condi ions, he CoF
de elopmen is sligh ly di e en . The highes ic ion o e he dominan pa o he expe imen was
exhibi ed by he solu ion wi h ela i ely high p o ein con en . Howe e , a e 75 s, he ic ion was
s abilized a abou 0.4 wi hou any u he ime-dependen change. The cou se o ic ion o saline
solu ion is linea ly inc easing ( he same beha iou as unde nega i e sliding), eaching 0.45 a he
end. Fo he o he p o ein solu ions, he beha iou is almos he same, wi h he excep ion o
lub ican con aining 70 mg/mL o albumin and 35 mg/mL o γ-globulin, which exhibi s he lowes
ic ion. This can be a ibu ed o he ac ion o he p o ein ilm. I was obse ed in li e a u e ha ,
conside ing he same model luid as in he case o he p esen s udy, a me al head o med much
hicke p o ein ilm unde posi i e sliding, which can lead o a dec ease o ic ion be ween he
su aces [22].
Figu e 6. De elopmen o CoF as a unc ion o ime o me al-on-me al pai a highe mean speed
unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
I is appa en ha he MoM combina ion exhibi s an inc easing endency o ic ion, in gene al.
By con as , when he disc is o polye hylene, ic ion is dec easing o cons an , as is shown in Figu e
7. In ha case, he ic ion le el is associa ed wi h he kinema ic condi ions. When he ball o a es
as e han he disc, he lowes ic ion was exhibi ed by PBS, and he lub ican wi h he highe
con en o γ-globulin. The highes ic ion was obse ed o lub ican wi h lowe p o ein
concen a ion (10.5 mg/mL) and he dominan p esence o albumin. The endency was also qui e
uns able in ha case. Ne e heless, i has o be aken in o accoun ha he di e ence be ween
minimum and maximum ic ion is jus 0.05; he e o e, i migh be assumed ha he e ec o he
lub ican is negligible. When he disc was as e , he lowes ic ion was eached, once he lub ican
wi h highe p o ein con en (21 mg/mL) was employed. In addi ion, bo h he simple solu ion
exhibi ed ela i ely low ic ion o a ound 0.11. Wha is in co ela ion wi h p e ious indings is he
ic ion le el o saline solu ion. In a ecen s udy [23], a polye hylene disc conduc ed ecip oca ing
mo ion agains a me al pin (pu e posi i e sliding), while he ic ion was om 0.12 o 0.16, which
co esponds o he p esen esul s, see Figu e 7b.
Figu e 7. De elopmen o CoF as a unc ion o ime o me al-on-polye hylene pai a highe mean
speed unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
Figu e 6.
De elopmen o CoF as a unc ion o ime o me al-on-me al pai a highe mean speed
unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
I is appa en ha he MoM combina ion exhibi s an inc easing endency o ic ion, in gene al.
By con as , when he disc is o polye hylene, ic ion is dec easing o cons an , as is shown in Figu e 7.
In ha case, he ic ion le el is associa ed wi h he kinema ic condi ions. When he ball o a es
as e han he disc, he lowes ic ion was exhibi ed by PBS, and he lub ican wi h he highe
con en o
γ
-globulin. The highes ic ion was obse ed o lub ican wi h lowe p o ein concen a ion
(10.5 mg/mL) and he dominan p esence o albumin. The endency was also qui e uns able in
ha case. Ne e heless, i has o be aken in o accoun ha he di e ence be ween minimum and
maximum ic ion is jus 0.05; he e o e, i migh be assumed ha he e ec o he lub ican is negligible.
When he disc was as e , he lowes ic ion was eached, once he lub ican wi h highe p o ein
con en (21 mg/mL) was employed. In addi ion, bo h he simple solu ion exhibi ed ela i ely low
ic ion o a ound 0.11. Wha is in co ela ion wi h p e ious indings is he ic ion le el o saline
solu ion. In a ecen s udy [
23
], a polye hylene disc conduc ed ecip oca ing mo ion agains a me al
pin (pu e posi i e sliding), while he ic ion was om 0.12 o 0.16, which co esponds o he p esen
esul s, see Figu e 7b.
Ma e ials 2018, 11, x FOR PEER REVIEW 8 o 12
a he end o he es , see Figu e 6a. Conside ing he posi i e sliding condi ions, he CoF
de elopmen is sligh ly di e en . The highes ic ion o e he dominan pa o he expe imen was
exhibi ed by he solu ion wi h ela i ely high p o ein con en . Howe e , a e 75 s, he ic ion was
s abilized a abou 0.4 wi hou any u he ime-dependen change. The cou se o ic ion o saline
solu ion is linea ly inc easing ( he same beha iou as unde nega i e sliding), eaching 0.45 a he
end. Fo he o he p o ein solu ions, he beha iou is almos he same, wi h he excep ion o
lub ican con aining 70 mg/mL o albumin and 35 mg/mL o γ-globulin, which exhibi s he lowes
ic ion. This can be a ibu ed o he ac ion o he p o ein ilm. I was obse ed in li e a u e ha ,
conside ing he same model luid as in he case o he p esen s udy, a me al head o med much
hicke p o ein ilm unde posi i e sliding, which can lead o a dec ease o ic ion be ween he
su aces [22].
Figu e 6. De elopmen o CoF as a unc ion o ime o me al-on-me al pai a highe mean speed
unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
I is appa en ha he MoM combina ion exhibi s an inc easing endency o ic ion, in gene al.
By con as , when he disc is o polye hylene, ic ion is dec easing o cons an , as is shown in Figu e
7. In ha case, he ic ion le el is associa ed wi h he kinema ic condi ions. When he ball o a es
as e han he disc, he lowes ic ion was exhibi ed by PBS, and he lub ican wi h he highe
con en o γ-globulin. The highes ic ion was obse ed o lub ican wi h lowe p o ein
concen a ion (10.5 mg/mL) and he dominan p esence o albumin. The endency was also qui e
uns able in ha case. Ne e heless, i has o be aken in o accoun ha he di e ence be ween
minimum and maximum ic ion is jus 0.05; he e o e, i migh be assumed ha he e ec o he
lub ican is negligible. When he disc was as e , he lowes ic ion was eached, once he lub ican
wi h highe p o ein con en (21 mg/mL) was employed. In addi ion, bo h he simple solu ion
exhibi ed ela i ely low ic ion o a ound 0.11. Wha is in co ela ion wi h p e ious indings is he
ic ion le el o saline solu ion. In a ecen s udy [23], a polye hylene disc conduc ed ecip oca ing
mo ion agains a me al pin (pu e posi i e sliding), while he ic ion was om 0.12 o 0.16, which
co esponds o he p esen esul s, see Figu e 7b.
Figu e 7. De elopmen o CoF as a unc ion o ime o me al-on-polye hylene pai a highe mean
speed unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
Figu e 7.
De elopmen o CoF as a unc ion o ime o me al-on-polye hylene pai a highe mean
speed unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
Ma e ials 2018,11, 767 9 o 12
Conside ing he ce amic-ce amic con ac , he ic ion is inc easing unde nega i e sliding as in he
case o he me al-me al pai . Mo eo e , he e is a good co ela ion o he e ec o p o eins, while adding
he p o eins o he saline solu ion led o a dec ease o ic ion, especially du ing he i s pa o he es ,
see Figu e 8a. The same beha iou can be obse ed e en o posi i e sliding, while he e ec o he
lub ican is mo e subs an ial; anyway, he a iance in ic ion is s ill limi ed. In his pa icula case, he
ic ion is ela i ely s able o all he es luids, as is displayed in Figu e 8b. Simila ic ion wi h ilm
hickness de elopmen can be ound, as men ioned o he me al sliding pai . Using he luo escen
mic oscopy echnique, we e alua ed he cen al ilm hickness in ce amic-on-glass con ac , while i was
ound ha he lub ican laye o alumina ce amic unde posi i e sliding was much hicke compa ed
o nega i e sliding [24].
Ma e ials 2018, 11, x FOR PEER REVIEW 9 o 12
Conside ing he ce amic-ce amic con ac , he ic ion is inc easing unde nega i e sliding as in
he case o he me al-me al pai . Mo eo e , he e is a good co ela ion o he e ec o p o eins, while
adding he p o eins o he saline solu ion led o a dec ease o ic ion, especially du ing he i s pa
o he es , see Figu e 8a. The same beha iou can be obse ed e en o posi i e sliding, while he
e ec o he lub ican is mo e subs an ial; anyway, he a iance in ic ion is s ill limi ed. In his
pa icula case, he ic ion is ela i ely s able o all he es luids, as is displayed in Figu e 8b.
Simila ic ion wi h ilm hickness de elopmen can be ound, as men ioned o he me al sliding
pai . Using he luo escen mic oscopy echnique, we e alua ed he cen al ilm hickness in
ce amic-on-glass con ac , while i was ound ha he lub ican laye o alumina ce amic unde
posi i e sliding was much hicke compa ed o nega i e sliding [24].
Figu e 8. De elopmen o CoF as a unc ion o ime o ce amic-on-ce amic pai a highe mean
speed unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
Finally, he expe imen s we e ealized wi h a ce amic ball and polye hylene disc. The e ec o
he lub ican was again e y limi ed, as o he MoP pai . In pa icula unde posi i e sliding, he
ole o luid is unimpo an , since he di e ence be ween minimum and maximum ic ion is jus
abou 0.04, see Figu e 9b. The e o e, i is no sui able o iden i y which lub ican leads o he lowes
and he highes ic ion, espec i ely. The only no iceable inding is ha in he case o nega i e
sliding, sligh ly highe ic ion (a ound 0.12) was exhibi ed by simple γ-globulin solu ion and by he
solu ion wi h a highe con en o p o ein.
Figu e 9. De elopmen o CoF as a unc ion o ime o ce amic-on-polye hylene pai a highe mean
speed unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
As could be expec ed based on he p e ious indings, he p esen esul s clea ly p o e ha he
mos impo an ac o in luencing he ic ional beha iou o implan s is he ma e ial o he
componen s. Wha is qui e su p ising is he limi ed in luence o model luid composi ion, mainly in
he case o MoP and CoP pai s. Ne e heless, i should be aken in o accoun ha in ha d-on-so
pai s signi ican ly lowe con ac p essu e occu s; he e o e, his may be an explana ion o ela i ely
low sensi i i y o ic ion o es luid. Anyway, since he p e ious obse a ions ocusing on he
assessmen o ilm hickness in hip eplacemen s explo ed whe he he e ec o luid composi ion
Figu e 8.
De elopmen o CoF as a unc ion o ime o ce amic-on-ce amic pai a highe mean speed
unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
Finally, he expe imen s we e ealized wi h a ce amic ball and polye hylene disc. The e ec o
he lub ican was again e y limi ed, as o he MoP pai . In pa icula unde posi i e sliding, he ole
o luid is unimpo an , since he di e ence be ween minimum and maximum ic ion is jus abou
0.04, see Figu e 9b. The e o e, i is no sui able o iden i y which lub ican leads o he lowes and he
highes ic ion, espec i ely. The only no iceable inding is ha in he case o nega i e sliding, sligh ly
highe ic ion (a ound 0.12) was exhibi ed by simple
γ
-globulin solu ion and by he solu ion wi h a
highe con en o p o ein.
Ma e ials 2018, 11, x FOR PEER REVIEW 9 o 12
Conside ing he ce amic-ce amic con ac , he ic ion is inc easing unde nega i e sliding as in
he case o he me al-me al pai . Mo eo e , he e is a good co ela ion o he e ec o p o eins, while
adding he p o eins o he saline solu ion led o a dec ease o ic ion, especially du ing he i s pa
o he es , see Figu e 8a. The same beha iou can be obse ed e en o posi i e sliding, while he
e ec o he lub ican is mo e subs an ial; anyway, he a iance in ic ion is s ill limi ed. In his
pa icula case, he ic ion is ela i ely s able o all he es luids, as is displayed in Figu e 8b.
Simila ic ion wi h ilm hickness de elopmen can be ound, as men ioned o he me al sliding
pai . Using he luo escen mic oscopy echnique, we e alua ed he cen al ilm hickness in
ce amic-on-glass con ac , while i was ound ha he lub ican laye o alumina ce amic unde
posi i e sliding was much hicke compa ed o nega i e sliding [24].
Figu e 8. De elopmen o CoF as a unc ion o ime o ce amic-on-ce amic pai a highe mean
speed unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
Finally, he expe imen s we e ealized wi h a ce amic ball and polye hylene disc. The e ec o
he lub ican was again e y limi ed, as o he MoP pai . In pa icula unde posi i e sliding, he
ole o luid is unimpo an , since he di e ence be ween minimum and maximum ic ion is jus
abou 0.04, see Figu e 9b. The e o e, i is no sui able o iden i y which lub ican leads o he lowes
and he highes ic ion, espec i ely. The only no iceable inding is ha in he case o nega i e
sliding, sligh ly highe ic ion (a ound 0.12) was exhibi ed by simple γ-globulin solu ion and by he
solu ion wi h a highe con en o p o ein.
Figu e 9. De elopmen o CoF as a unc ion o ime o ce amic-on-polye hylene pai a highe mean
speed unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
As could be expec ed based on he p e ious indings, he p esen esul s clea ly p o e ha he
mos impo an ac o in luencing he ic ional beha iou o implan s is he ma e ial o he
componen s. Wha is qui e su p ising is he limi ed in luence o model luid composi ion, mainly in
he case o MoP and CoP pai s. Ne e heless, i should be aken in o accoun ha in ha d-on-so
pai s signi ican ly lowe con ac p essu e occu s; he e o e, his may be an explana ion o ela i ely
low sensi i i y o ic ion o es luid. Anyway, since he p e ious obse a ions ocusing on he
assessmen o ilm hickness in hip eplacemen s explo ed whe he he e ec o luid composi ion
Figu e 9.
De elopmen o CoF as a unc ion o ime o ce amic-on-polye hylene pai a highe mean
speed unde nega i e (a) and posi i e (b) sliding condi ions o a ious model luids.
As could be expec ed based on he p e ious indings, he p esen esul s clea ly p o e ha
he mos impo an ac o in luencing he ic ional beha iou o implan s is he ma e ial o he
componen s. Wha is qui e su p ising is he limi ed in luence o model luid composi ion, mainly in
he case o MoP and CoP pai s. Ne e heless, i should be aken in o accoun ha in ha d-on-so
pai s signi ican ly lowe con ac p essu e occu s; he e o e, his may be an explana ion o ela i ely
low sensi i i y o ic ion o es luid. Anyway, since he p e ious obse a ions ocusing on he
assessmen o ilm hickness in hip eplacemen s explo ed whe he he e ec o luid composi ion