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IMAC-U course 6 th semester Tribology 4. Friction-1 Assoc. Prof. Takeshi YAMAGUCHI [email protected]

Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

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Page 1: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

IMAC-U course 6th semester

Tribology 4. Friction-1

Assoc. Prof. Takeshi YAMAGUCHI [email protected]

Page 2: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Static and kinetic friction coefficient

m=F/W

W Normal load

Tangential force

P

Friction force F

Time

Fric

tio

n f

orc

e

( ) ( )

Static friction coefficient : Fs/W at slip initiation Kinetic friction coefficient : Fs/W at during sliding

Page 3: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Amonton-Coulomb Law for sliding friction

(1) Friction force is proportional to normal load.

(2) Friction force is independent of apparent contact area.

(3) Friction force is independent of sliding velocity.

(4) Static friction force is larger than kinetic friction force.

F

2F

F Fr

icti

on

forc

e Static friction force

kinetic friction force

Sliding velocity

Page 4: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Normal load, N

Fric

tio

n c

oef

fici

ent

Fric

tio

n c

oef

fici

ent

Apparent contact area, mm2

Wood/steel Dry condition Normal load: 0.3 N

Friction coefficient is independent of normal load, sliding velocity, and contact area.

(3.1)

Amonton-Coulomb Law for sliding friction

Page 5: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Fric

tio

n c

oef

fici

ent

Fric

tio

n c

oef

fici

ent

Sliding velocity, mm/s Contact time, s

Steel/Indium

Steel/Lead

Steel/steel Dry sliding

Amonton-Coulomb Law for sliding friction

There are lots of cases where the Amonton-Coulomb friction law is not established.

Page 6: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

F = Fa + Fp (Fh)

Adhesion at real contact area

Ploughing due to penetration by hard

asperities

strain

Stress

Hysteresis energy loss

Elastic hysteresis loss

Friction mechanism

(3.2)

Page 7: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Adhesion friction theory

Friction force

橋本巨著,基礎から学ぶトライボロジー,森北出版(株),(2006)

Normal load Traction force

Friction force:Force to shear adhesion in the real contact area

ro

n

i

n

i

rioi AsAsFF

1 1

so: maximum shear strength Ar:real contact area W: normal load p0: plastic flow pressure

0p

s

W

As

W

F oro m

(3.3)

(3.4)

Page 8: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Hard ball Hard ball Hard ball

Hard Hard Soft

Soft film

Asmall Alarge Amedium

slarge ssmall ssmall

Effect of soft film on hard substrate

>

Page 9: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Modified Adhesion friction theory W

A0 = Wp0

FT

W

A > Wp0

More significant plastic flow occurs when the tangential force is applied. → Junction Growth

222

0 spp

Condition for plastic deformation when the normal pressure and shear pressure are applied.

22

2

0

A

F

A

Wp T

A

(3.5)

(3.6)

(3.7)

Page 10: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Effect of surface roughness on friction coefficient W

P F

32

W

P F

Rough Smooth Fr

icti

on

co

effi

cie

nt

Page 11: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

F : 摩擦力 r : 材料表面における突起半径 W : 垂直荷重 h : 食込み深さ A : 投影面積 m : 摩擦係数 p0 : 塑性流動圧力 V : 垂直方向 n : 突起総数 2q : 突起の角度 H : 進行方向

q

r

h

F

W Conical asperity

r

q

r

AH h

A conical asperity is penetrated into the surface and moves in the right direction

2

2rnAv

Av

q

m

cotr

h

W

F

nrhppAF

pr

nAvpW

H

22

2

00

0

2

0

nrhAH

Ploughing friction

Soft

Hard

(3.8)

(3.9)

(3.10)

Page 12: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Hysteresis friction

strain

Stre

ss

Hysteresis energy loss F

W

Viscoelastic material

Hard asperity

Loading unloading

s

S-S curve for viscoelastic materials under compression

( ) > ( )

Hysteresis friction is caused by the energy dissipation due to cyclic deformation (loading and unloading) for viscoelastic materials such as rubbers.

Page 13: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Method to reduce friction and wear

Hydrodynamic lubrication

Hydrostatic lubrication

Solid lubricants (powder form)

Solid lubricating film Self lubricating materials

Rolling type guide Magnetic force

Boundary lubrication by adsorbed molecular films

How to reduce adhesion in the contact area is key to reduce friction.

Page 14: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Stick slip phenomena

Slip

Stick

Fric

tio

n f

orc

e F

, N

Time t, s

Fs

Fk

F

v

x k

m

Mechanical mode of friction vibration Friction force as a function of time when stick-slip occurs

0 kxxm)v(xm m (3.11)

0

0

dv

d)v(

dv

d)v(

mm

mm

( )

( )

Page 15: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Characteristics

Practical applications of RB ceramics

RB ceramics

Carriage

Guide rail

RB ceramics

Carriage

Guide rail

Guide rail:Stainless steel

Slider:RB ceramics

Guide rail:Stainless steel

Slider:RB ceramics

Dry-type linear sliding bearings using RB ceramics

A dry-type linear sliding bearing using RB ceramics was developed collaborated with Japanese company

and has been in practical use since 2001.

Overview Structure

Oil free Maintenance free Noise free Capability to be used at high velocity over 1m/s Capability to be used in water

Pamphlet of newly developed dry linear sliding bearing

Page 16: Tribology - Tohoku University Official English WebsiteNormal load, N t t Apparent contact area, mm2 Wood/steel Dry condition Normal load: 0.3 N Friction coefficient is independent

Type of Bearings

Dry linear sliding bearing

using RB ceramics

Grease-lubricated linear

rolling bearing

Sliding velocity 680mm/s 500mm/s

Maximum noise level 40.5dB 69.4dB

Sound pressure ratio 3% 100%

Noise level data

RB ceramics

Carriage

Guide rail

RB ceramics

Carriage

Guide rail

Guide rail:Stainless steel

Slider:RB ceramics

Guide rail:Stainless steel

Slider:RB ceramics

RBセラミックスガイドの静粛性 Quietness Suppression of stick-slip motion by using RB ceramics