messy sentiments about scale issues - Luleå University of .../file/C_Courbon_2013_09_26... ·...

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C. Courbon *, S. Hernandez, J. Hardell and B. Prakash *Ph.D, Post-doctoral Researcher Luleå University of Technology Division of Machine Elements 971 87 Luleå, Sweden +46 725 661731 [email protected] Another insight into our experiments: messy sentiments about scale issues

Transcript of messy sentiments about scale issues - Luleå University of .../file/C_Courbon_2013_09_26... ·...

C. Courbon*, S. Hernandez, J. Hardell and B. Prakash*Ph.D, Post-doctoral Researcher

Luleå University of TechnologyDivision of Machine Elements

971 87 Luleå, Sweden+46 725 661731

[email protected]

Another insight into our experiments:

messy sentiments about scale issues

2/23

Background

One of the future trend in Tribology

Tribological

tests

• Out of the process • Simple config.• Flexible config.• Access to more data

Wear simulation in

a tribosystem

Contact/Wear

mechanisms

Contact/Wear

modelling

• Predict wear of the comp.• Predict surface defects• Opt. contacting geometry• Opt. operating cond.

• Properly model friction • Properly model heat trans. • Model at the right scale• Wear modelling strategy

• Better understanding• Identif. contact conditions • Identif. wear mechanisms •Propose a wear model

Know what we are doing/looking at

3/23

How are we usually investigating friction and wear?

Standard tribological tests

Reciprocating or unidirectional sliding

Open or closed configuration

Extracted data

Average friction coefficient

Specific wear rate

Post-mortem analysis of the samples

Tribological experiments

Open pin-on-disc

Closed pin-on-disc

Reciprocating test

4/23

Under which conditions are we effectively measuring wear?

Possible heterogeneous contact

Sliding on sticking material, oxide layers

Sliding on worn parts (material removed)

Third body always present in the contact

Low contact pressures (< 100 MPa)

Questions:

Where is the contact actually occurring?

What is the real contact area?

What is the actual contact pressure?

Where is wear actually occurring?

Tribological experiments

[Hardell et al., 2008]

[Kondratiuk & Kuhn, 2011]

5/23

Under which conditions are we effectively measuring wear?

Possible heterogeneous contact

Flat-end pin – RT – 75 N [Hernandez et al., 2013]

Many deposits, irregular surface, ploughing…

Local contact phenomena

Sliding direction

Flattened areas

Sliding direction

Pin Disc

6/23

Under which conditions are we effectively measuring wear?

Local contact phenomena

75 N

RT

7/23

Under which conditions are we effectively measuring wear?

Possible heterogeneous contact

Flat-end pin – 300°C – 75 N

Formation of a tribofilm

Local contact phenomena

Sliding direction Sliding direction

Pin Disc

8/23

Under which conditions are we effectively measuring wear?

Local contact phenomena

75 N

300°C

9/23

Under which conditions are we effectively measuring wear?

Local contact phenomena

75 N

300°C

10/23

Local contact phenomena

Let’s try to get “into the contact”…

Ultrasounds as a powerful method

[Kendall & Tabor, 1971][Marshall et al., 2005][Dwyer-Joyce, 2005]

Direct image of what is happening at the interface

Powerful technic to assess film thickness

Can be used to assess contact area, pressure, adhesion, junction growth…

Online and precise wear monitoring

100 N

RT

Time (s)

1rst reflected pulse

2x

11/23

Local contact phenomena

Let’s try to get “into the contact”…

Overview of the set-up

100 N

RT

12/23

Local contact phenomena

Let’s try to get “into the contact”…

Results – Evolution of the “real contact area”

Time (s)

100 N

RT

13/23

Under which conditions are we effectively measuring wear?

Impact of an heterogeneous contact

Increased local contact pressure and flash temperature

Wear only occurring on asperities ⇒ heterogeneous wear profile

Impairing heat transfer & heat generation across the interface

Consequences

T

P

nF

Concentrated loadingson asperities

W

nF

Artificially increased wear rate

nF

Affected heat transferFormation of TCR

14/23

Modelling scale

How should we look at the contact interface?

Different scales can hide different phenomena

Perfect or imperfect contact?

Contact modelling

Body 1

Body 2

Vsl

yMacroscopic scale

Asperity scale

sTS1

S2

1T

2T

Con

stric

tion

area

Roughness scale

S1

S2

Heat flux lines

15/23

Modelling scale

Macroscopic scale

Neglecting the constriction area

Direct separation between surfaces in contact

Introduction of a Thermal Contact Resistance (TCR)

Possible temperature discontinuity

1T

2T

Con

stric

tion

area

Roughness scale

1T

2T

Con

stric

tion

area

Macroscopic scale

sTCR

( ) gϕαϕ ⋅−= 12

gϕαϕ ⋅=1

S1

S2

S1

S2

VslVsl

Contact modelling

16/23

Heat transfer modelling

Macroscopic Thermal Contact Resistance

Connected to the real contact area

Temperature and Pressure dependent

Contact modelling

0

0.5

1

1.5

2

2.5

3

3.5

4

0 100 200 300 400 500

Temperature (°C)

TC

R (K

.mm

²/W)

P = 80 MPa

Uncoated steel - Copper

Source: LIMATB, France

17/23

Modelling scale

Influence on “contact temperature”

Macroscopic model

0.00

20.00

40.00

60.00

80.00

100.00

120.00

140.00

0.00 0.50 1.00 1.50 2.00

Distance along the path (mm)

Tem

pera

ture

(°C

)

No_TCR

Inf_TCR

Contact modelling

S2

S1

Extraction path

µ = 0.2Vslid = 0.1 m/s

25 °C

100 °C

Macroscopic model

S1

S2

18/23

Modelling scale

But… if we look a little bit closer…

The “actual” contact temperature Ts can not be modelled

Heat generation is not occurring at the right place

Conduction

Conduction

Con

stric

tion

( ) gϕα ⋅−1

gϕα ⋅

1T

2T

sT

1ϕ1ϕ

2ϕ 2ϕ

1T

2T

sTCR

1TCR

2TCR

S1

S2

Vsl

( ) gϕα ⋅−1

gϕα ⋅

a b

Contact modelling

19/23

Modelling scale

Modelling a contact interface at a mesoscopic scale [Rogeon et al., 2009]

Application in resistance spot welding

Conduction

Conduction

( ) gϕα ⋅−1

gϕα ⋅

gϕsT

1T

2T

1TCR

2TCR

Vsl

a b

Mesoscopic scale

1T

2T

sT

( )111 eTCReq ,λ

( )222 eTCReq ,λ

1e

2e

Contact modelling

20/23

0.00

20.00

40.00

60.00

80.00

100.00

120.00

140.00

160.00

180.00

200.00

0.00 0.50 1.00 1.50 2.00

Distance along the path (mm)

Tem

pera

ture

(°C

)

No_TCR

Inf_TCR

MESO

Modelling scale

Influence on “contact temperature”

Mesoscopic model Extraction path

µ = 0.2Vslid = 0.1 m/s

25 °C

100 °C

+ 60 %

Eq. conductivity

Contact modelling

Mesoscopic model

S2

S1

S1

S2

21/23

Modelling scale

Influence on contact temperature [Richard et al., 2008]

Similar findings in the literature with DEM

Contact modelling

22/23

Conclusions

Summary

To keep in mind

“Proper” contact conditions in our experiments (controlled)

Measure as much data as possible

To think about the scale that needs to be considered

Importance of the scale

Temperature distribution

Effect on wear and friction

Important if we are looking from a local point of view

Needs and future trends

Let’s try to get “into the contact” !

23/23

Perspectives

24/23

Discussion

Thank you for your attention !Thank you for your attention !

Soon at:

LTDS UMR CNRS/ECL/ENISESaint-Etienne, France

+33 6 86 94 78 [email protected]