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CONTACT ANGLES ARVIND TOMAR Sr-08471
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Contact angle
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FACTORS AFFECTING CONTACT ANGLE
SURFACE TENSION SURFACE ENERGY OF SOLID SURFACES INTERACTION FORCES BETWEEN LIQUID MOLECULES SURFACE ROUGHNESS TEMERATURE OF LIQUID
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SURFACE TENSION
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SURFACE TENSION IS A CONTRACTIVE TENDENCY OF SURFACE OF A LIQUID
THIS ALLOWS IT TO RESIST AN EXTERNAL FORCE DUE TO SURFACE TENSION A LIQUID ACQUIRE MINIMUM SURFACE AREA DUE TO SURFACE TENSION LIQUID SURFACE BAHAVES AS A STRECHED SKIN SURFACE TENSION IS CAUSED BECAUSE OF MOLECULER ATTRACTION FORCES IN GENERAL DISSOLVED CONTAMINATION IN WATER REDUCES SURFACE TENSION, HENCE ALSO THE CONTACT ANGLE
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DUE TO SURFACE TENSION A NEEDLE CAN FLOAT ON A LIQUID
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SURFACE TENSION =FORCE/LENGTH
=WORK DONE /AREA TO SEPRATE TWO LIQUID SURFACES WE HAVE TO DO WORK THIS PER UNIT AREA WORK IS CALLED SURFACE TENSION THIS WORK INCREASES POTENTIAL ENERGY OF LIQUID
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AS SURFACE TENSION REDUCES, DROPLETS TENDS TO SPREADS AND CONTACT ANGLE DECREASES
GREATER THE PORTION OF POLAR GROUPS,HIGHER THE ATTRACTIVE FORCES,HIGHER SURFACE TENSION AND HIGH WILL BE THE CONTACT ANGLE EX. WATER HAS HIGHER CONTACT ANGLE AS COMPARED TO OILS
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SURFACES BENDS TO BALANCE FORCES
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YOUNG-LAPLACE EQUATION
ΔP=σ[1/Rx +1/Ry]
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HIGHER THE SURFACE TENSION HIGHER WILL BE CONTACT ANGLE
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SURFACE ENERGY HIGHER THE SURFACE ENERGY LOWER WILL BE CONTACT ANGLE
HIGH SURFACE ENERGY OVERCOMES SURFACE TENSION AND LIQUID DROPLET SPREADS OVER SURFACE HIGHER THE SURFACE ENERGY HIGHER THE ADHESION SURFACE IS ALWAYS AT HIGHER ENERGY AS COMPARED TO BULK
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DEPENDENCE OF CONTACT ANGLE ON SURFACE ENERGY AND SURFACE TENSION
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SURFACE ENERGY DEPENDS ON CHEMICAL COMPOSITION AT SURFACE
POLAR GROUPS CAUSES HIGH SURFACE ENERGY CLEAN METALIC SURFACES HAVE HIGH SURFACE ENERGY BONDING BETWEEN HYDROCARBON MOLECULES IS LESS POLYETHYNES HAVE LESS SURFACE ENERGY AND HIGHER CONTACT ANGLE
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FOR UNPOLISHED SURFACE THERE ARE SO MANY POLAR GROUP(EX
FOR UNPOLISHED SURFACE THERE ARE SO MANY POLAR GROUP(EX. O-H) SO HAD HIGHER ENERGY SURFACE ENERGY OF SURFACE CAN BE REDUCED BY POLISHING WAX
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WATER PROOF FABRICS FLOURINATED FABRICS, WHICH ARTIFICIALLY MAKE A SURFACE LOW ENERGY ONE THUS MORE CONTACT ANGLE AND SURFACE IS NON-WETTING BY FORMING OXYGEN CONTAINING COMPOUNDS AT SURFACE A LOW ENERGY SURFACE CAN BE CONVERTED INTO A HIGH ENERGY ONE THIS CAN BE ACHEIVED BY EXPOSURE TO UV-RADIATION,CORONA/PLASMA DISHCHARGE, ACID TREATMENT etc.
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NON-WETTING FABRIC
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INTERACTION FORCES BETWEEN LIQUID MOLECULES
CONTACT ANGLE (IN DEGREES) DEGREE OF WETTING SOLID-LIQUID INTERACTION LIQUID-LIQUID INTERACTION θ=0 PERFECT WETTING VERY STRONG VERY WEAK 0<θ<90 HIGH WETTING STRONG WEAK 90≤θ<180 LOW WETTING θ=180 PERFECTLY NON-WETTING
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SURFACE ROUGHNESS WITH INCREASING SURFACE ROUGHNESS CONTACT ANGLE DECREASES FOR HYDRO-PHILIC SURFACE WITH INCREASING SURFACE ROUGHNESS CONTACT ANGLE INCREASES FOR HYDRO- PHOBIC SURFACE
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TEMPERATURE WITH INCREASING OF TEMPERATURE SURFACE TENSION DECREASES AS INTERMOLECULER FORCE DECREASES THUS WITH INCREASING OF TEMPERATURE CONTACT ANGLE DECREASES
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BALANCE OF FORCES
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γsl +γlg*cosθc =γsg YOUNG'S EQUATION
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TWO DIFFRENT LIQUIDS
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METHODS FOR MEASURING CONTACT ANGLE
THE STATIC SESSILE DROP METHOD THE DYNAMIC SESSILE DROP METHOD DYNAMIC WILHELMY METHOD POWDER CONTACT ANGLE METHOD
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Young-dupre equation γ(1+cosθc)= ∆Wsl Here,
∆Wsl=solid-liquid adhesion energy per unit area
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CALCULATION FOR CONTACT ANGLE
θc=arcCOS[rAcosθA+rRcosθR/rA+rR] Where, CALCULATION FOR CONTACT ANGLE
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ΘA= advancing angle ΘR= receding angle ADVANCING ANGLE:- largest contact angle possible without increasing solid-liquid interfacial area by adding volume dynamically RECEDING ANGLE:- if in above case you start removing volume then smaalest possible angle is called receding angle
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Calculation of Θa and Θr on a tilted plane
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Hysteresis angle H=Θa-Θr
Hysteresis angle for an ideal solid surface is zero i.e. Θa=Θr With increasing roughness H increases With increasing roughness Θa increases and Θr decreases Increased liquid penetration leads to increased hysteresis
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THANK YOU
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