cp0060_02-jan-2012_rm01

Upload: nirman-parashar

Post on 06-Apr-2018

220 views

Category:

Documents


0 download

TRANSCRIPT

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    1/29

    Important Note to students(Applies to all course material related to Tribology)

    This material is only an excerpt of the class room lectures prepared as per the syllabus

    contents.

    It needs to be supplemented with material from text book and other sources.

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    1

    .

    You need to prepare additional notes wherever required.

    Evaluation questions may be expected from material not covered in the slides but discussed

    during the lectures.

    Few Figures/photos/Graphs etc. have been removed because of upload limit.

    To be used for internal circulation only.

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    2/29

    Tribology

    2

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    3/29

    Tribology

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    3

    FrictionWear

    Lubrication

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    4/29

    PEOPLE Leonardo da VinciLeonardo di ser Piero da Vinci (April 15, 1452 May 2, 1519) was an Italian Renaissancepolymath: painter, sculptor, architect, musician, scientist, mathematician, engineer, inventor,

    anatomist, geologist, cartographer, botanist and writer. Leonardo has often been described asthe archetype of the Renaissance Man, a man of "unquenchable curiosity" and "feverishlyinventive imagination.

    Considered to be one of the greatest painters of all time and the most diverselytalented person ever to have lived.

    Amontons' Laws of Friction were first recorded in books during the late 17th century.

    Guillaume Amontons(1663 1705)

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    4

    Charles-Augustin de CoulombCharles-Augustin de Coulomb (14 June 1736 23 August 1806) was a French physicist. He is bestknown for developing Coulomb's law, the definition of the electrostatic force of attraction andrepulsion. The SI unit of charge, the coulomb, was named after him.

    BEAUCHAMP TOWER (1845-1904)Towers Spherical engine was a unique contender in the

    rotary steam engine market

    His experiments led to the revelation of

    pressure development in a fluid film.

    Source : http://www.wikipedia.org/

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    5/29

    Why Tribology ?

    Losses resulting from ignorance of Tribology amountto 4 % of the GDP of every country

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    5

    One third of worlds energy resources in present use

    appear as Friction in one form or other

    A saving of 1% of GDP can be realized by research

    and better tribological practices

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    6/29

    Surface

    Surface Characteristics

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    6

    GeometricCharacteristics

    Physico-ChemicalCharacteristics

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    7/29

    GEOMETRIC CHARACTERISTICS

    ERROR OF FORM

    +

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    7

    WAVINESS

    +

    ROUGHNESS

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    8/29

    GEOMETRIC CHARACTERISTICS

    Error of form : -

    Any deviation from the intended surface profile.

    Caused due to the errors in the manufacturing

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    8

    process.

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    9/29

    GEOMETRIC CHARACTERISTICS

    Waviness :-

    Large waves generated on the surface due to machine toolvibrations

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    9

    Features on the surface other than error of form andwaviness.

    Lay : - The direction of the predominant surface pattern.

    Flaw :- Any defect on the surface (Inclusions, voids,

    porosity, cracks, etc.)

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    10/29

    PHYSICO-CHEMICAL CHARACTERISTICS

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    10

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    11/29

    PHYSICO-CHEMICAL CHARACTERISTICS

    Physisorbed Layer:

    Gases like Oxygen, Argon, Krypton, etc. andwater vapor gets adsorbed to a clean surface

    Thickness of the layer- 0.3 nm

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    11

    Chemisorbed Layer:

    Electron sharing between the chemisorbed species

    and the solid surface-covalent bonds Energy required to remove these bonds are high

    Depends on the purity of the surface

    Layers are monomolecular

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    12/29

    PHYSICO-CHEMICAL CHARACTERISTICS

    Chemically reacted layer:

    Most of the metals react with oxygenForms oxides on the surface

    Interaction continues till a thick layer is formed(10-100 nm)

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    12

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    13/29

    PHYSICO-CHEMICAL CHARACTERISTICS

    Beilby Layer:

    Melting and surface flow during machining ofmolecular layers

    Generally amorphous or microcrystalline

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    13

    ayers ge ar ene ue o e a acen co me a Thickness 1-100 nm

    Heavily deformed layer and Lightly deformed layer:

    Machining makes surfaces highly strained

    Smaller grains due to recrystallisation of the layers

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    14/29

    ROUGHNESS MEASUREMENT

    1. Contact type instruments (stylus measurements):-

    Stylus measurements transform the vertical movements

    of the stylus to corresponding electrical signals.

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    14

    2. Non-contact type of instruments :-

    a. Pneumatic devices

    b. Optical devicesc. Transmission electron microscopy

    d. Reflection electron microscopy

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    15/29

    ROUGHNESS PROFILE

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    15

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    16/29

    ROUGHNESS MEASUREMENT

    Methods

    1. Mean or M-System:- The mean line is taken as thecentroid of the profile. Areas above and below the lineare equal.

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    16

    . -The average heights/depths of five highest peaks andfive lowest valleys is determined.

    3. Method of least squares

    A reference line is fixed in such a way that the squareroot of sum of squares of the vertical deviations fromthis line is minimum

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    17/29

    SCHEMATIC OF A SURFACE PROFILE

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    17

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    18/29

    Extreme value height descriptors

    Rp Distance between the highest asperity and mean line

    Rv Distance between the lowest valley and mean line

    ROUGHNESS PARAMETERS

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    18

    Rt Distance between the highest asperity and lowest

    valley

    Rz Difference between the averages of five highest

    asperities and five lowest valleys.

    Rpm Distance between the average of five highest peaks

    and mean line

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    19/29

    ROUGHNESS PARAMETERS

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    19

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    20/29

    ROUGHNESS PARAMETERS

    1. Mean of a profile

    2. Variance

    Roughness height distribution

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    20

    . an ar ev a on

    4. Skewness

    5. Kurtossis

    Surfaces with same Ra Value

    Bearing Area curve

    Bearing Ratio

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    21/29

    ROUGHNESS HEIGHT DISTRIBUTIONS

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    21

    Non-Gaussian DistributionGaussian Distribution

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    22/29

    ROUGHNESS

    Gaussian distribution:- The Gaussian (normal) distribution washistorically called the law of errors. It was used by Gauss to model errorsin astronomical observations, which is why it is usually referred to as theGaussian distribution. Gaussian probability distribution is perhaps the mostused distribution in all of science.

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    22

    The probability density function for the Gaussian distribution with mean and standard deviation is given by the following formulas.

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    23/29

    ROUGHNESS HEIGHT DISTRIBUTIONS

    Non-Gaussian Distribution

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    23

    Turning, shaping, EDM, Milling,

    Honing, Grinding, Abrasion processes

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    24/29

    BEARING AREA CURVE

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    24

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    25/29

    True area and Geometric area

    Conformal contact

    Contents

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    25

    on con orma con ac

    Elastic Half space

    Hertzian contact

    Friction

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    26/29

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    27/29

    ELASTIC HALF SPACE

    In Non- conformal contacts the pressures at the contact

    spots are very high.

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    27

    as c con ac eory.

    A semi-infinite elastic solid bounded a plane surface.

    Strains are small within the contact region.

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    28/29

    HERTZ CONTACT THEORY(1882)

    Assumptions

    1. Surfaces are smooth, continuous and

    (1857 1894)German physicist

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    28

    2. Strains are small

    3. Each solid is an elastic half-space in the contact region

    4. Surfaces are frictionless

  • 8/2/2019 CP0060_02-Jan-2012_RM01

    29/29

    P

    HERTZ CONTACT THEORY(1882)

    Contact area will be circular

    P.M. Anil Asst. Professor S.G SMBS VIT Universit

    29

    3

    1

    *4

    3

    =

    E

    PRaContact radius = a

    Ball radius = R

    Maximum contact pressure = Po

    =

    20

    2

    3

    a

    PP

    a