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FrugalCombination3009

Uploaded by FrugalCombination3009

University of Sunderland

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rheology viscometry fluid mechanics material science

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This document discusses the science of deformation and flow, known as rheology. It covers the importance of rheological measurements for characterizing and classifying materials, focusing on viscosity, elasticity, and viscoelasticity. Various testing methods, including viscometry and different rheometers are highlighted.

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ω 20. Rheology[ 유변학」 flow studying) : the sclence of deformatonand flow. Viscometry Testng= Measurement ofa flud' resistanceto flow...

ω 20. Rheology[ 유변학」 flow studying) : the sclence of deformatonand flow. Viscometry Testng= Measurement ofa flud' resistanceto flow s ' of #2. Importance theology Characterisation &classficatcon of materials - Rhelogicalmeasurementsdescribetheflowbehaviour Eerids & semssolids of. - Insigats into viscosity elasticity viscoelastieity , , , understandstractare to - Raw maaterial - Finished Products Quality Control - physical staablity consistency , In ratcty ,patieat compatibiliy ,dg bioawaslababaty Difference contaminatcon poormixg - can indicate , , variabslaty Adhesive of transdermal patches - performance Process optsomisation. - by understanding how matercals behave ander stress &strains. select suitable erpmeut -. ANewton 's experiment shear stress ① FfA (Nmror Pal Forcelarea = = velocity of top layer = Displaceventftime V = xIt [ms> shearstrain[ strain) Bisplacementfheight = γ = × /it Canstless) shearstrasntate= Veloatyof toplayerfHeight γ " = (시 (s") -Defnition of Tarms #3. Viscometry shearstress( O]forsonalforoefarea [N/m iN 6 m= Poa I ) - straasn[r ) :resuttant bythesample neight displacementdausded shear (strarn )ratelry shear : D strain In certaEn tㆍme $ , sthear. a time rate viscosityI n 3: shearstressdiwided byshear Ls units : Pascal second Pas[SI) bisplacanntap.. #4 shear strafn (r) =.. Poise P (CGs) ARemember. u [NntorPas) I Pas #5 Dynamic viscosity lop =. I mPas I /n. EPS = 0 M = β Kinefic √ Cm > Viscosity s √ = /9 - Mormalised valne of viscosity. of flow veloity - =5 v = =0 - 001 ms- #6. Newtonian flow Ostwald U - fube viscometer Laminarflow of IEusdhenderthenfluenceofgrauty. Record fmeto flowfromL toD. k - et Dynamic viscosity : n = = Fnstrumentonstant density x × frme nake. t = X어 × 800 × 100. = ω. 008 Pas Ostwald U tube viscometer -. viscometer ( Nentonian flow) #n ) Falling sphere Dewiceusedtocalcalate theynamicviscostyof afluid bymeasurg the tne rerired for ball to fall a spherical a centatondistancewonder grauity throgh aa tube , filled the fluid whose determined viscosity is to be use stokes'law 'g(o e) -. 」 = s measure time that between tho pass poouts o] Rotational Rheometer(non -efonian flon) o upper mobile plate. s paralkelplate(stanlessstee ,fitancum efo) Cone → plaate. o Lower stat conary plate Expersmertal platesoum settays sizetsysizeomuetuer. , 4 plate , - Femperature of plates #T Factors that affect. viscosity ↑. Temperature (T) → viscosstyd. pressure [ P) P s viscostyp Tameltl P Viscosty ↓ Thixotropc syst. s. > 시간이지남에따라 점도가 감소하는 현상 - shear stress (O ) Nentoniaon - newtonian - systen Newtonian system ? of Viscossty regardless applied constant shear s fluids that have a , stress rasu rate viscossty (n ) = xchange with rate of shean - - Flow behavion = IEnear( shear stressa shear rate) shear stress nr I 임 ! viscosthear σ = δ rate. = ~ constant example of Newtonian flow - wwater - Petrol. - glycero이 - Aydrogen gas Non Nentonian - system ⇒ Fluids whose chagdependg wiscosity onappliedshearstress or strasm rate. shear stress dependent uiscossty I s shean - thunin flowCeag. cream) - s shear-thickeng flow [e g Couc suspensiou) -.. flo) s BnghamflowLe..trothpaste, needs applied pressure g to en dependent viscosity 1 Thsxotrop' flow ( g - c e.. bentonte , ketchup) 1 ) shear thenningflow[ 전단음력받을때 점도가감소하는유동특성 ) - L xtinear exs ketchup 병 압릴 가하면 잘 흐른다 , flowbeginsassoonasshearstress xiineaar isapplked Viscosity ' highat s lowshear raates and vice versa Power law where " eratiou : ① = nr' nst shear solutions [eg gels formation) thennng polymer - of -. shear 2) - thickening flow = psendoplastic flow. The opposite behautour to shear thiuning flow high at high shear rate and Viscoscty. ss oice varsa where usl 'm faw eration : 8 np power = > 감자 전문에게 치면 단달 산살 , → 흐물 ! 3. Binghan flow [ yield stress 넘으면 흐르기 시작하며, Nentonian flow 처럼 흐른다 ) Newtonian flow begaus. when sress reached yceld Oy is - yieldstress behaviour 4 Thixotro. Loixotropy= fIme- dependent shear - thinning behaviour then mixed becomes uiscosity ↓ st Kpacd. a ap , but sets after re application - shear stress ^ AA YTeld stress - No flow untll a cerfain shear stress is applied > shean Raate * Visco elasticity aproducts Many s Materiabs exhibit elastlaty Visco - , and Iike elastic solids theybehavelikeviscousIerids sme process Ia i - e. - an cothers ex ) coucentrated saspensiou s Buring storage st needs , to behave like a solld to prevent sedimentation s Dugapplication t , needsto behave tikea flucd eg. so that it flows a the and bristles of the brush an be eventypanted. Phase angle (8) For Perey elastic Material. -. stress(O] cand strasoaCr )are exacty n phase s ∴ phase anghe = 0. Viscous Matertal For purey 0 s σ and r are 144of a ayce out of phase s Therefore pthase angle = 900 phase angle(8) Measureof. = elastiaty The higher the phase angle the viscous [액체) s , more s The tower the phase caghe,the more eloastla [고체 ) - Parameters En Oscillatiou * Comples Modulus [G * ) - Comples Modulus (Pal e stracutress * LossCviscous Modlus) fndicate likenature Con of uid sample + ,. a " G (Pa) * sin8 * storage (Elastic) Modulus + Indecate solid lce nature of - sample G'(Pa ) λ Coss , phase angle obeys A ynamicViscosty→ , relatedto shear viscossty if sample Cox Merzrule - " ' G n (Pas) = Fredrency At Test modes - rotational nheometershave or rangeof testmodes : - VisEometry (shear) - OsEillaTiou Creep andrecovery - rwet sponge model ' elastic solid [storage modulus) bry = ifadd water (Enelastio, Viscous] Closs oddlus] - Comples viscoelastia behawjour (Complex modolas Soakwithhony- hagher modelas rector suoonof modeli ) Gompler -. * Viscoelastic behavsor = wiscous t elastic - Visousbehawgour = materials that flow - Eoulds lasticbehaviour structemed materials that deform - = reversably - Solid - visco elastia behaviour = structured Kaids which exhibit both viscous & elastec polymer poly gels properties melts, - creams eg. mer ,. * Oscillation lleasurement types - Amplitude sweep , - Frevengsureep. Temperature sreep - - TKme expencent [thixotropic)

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