7122013 An Introduction to Rheology Phenomenon Concept Measuring

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中鋼 講稿 7/12/2013 An Introduction to Rheology: Phenomenon, Concept, Measuring, and Case Study Complex

中鋼 講稿 7/12/2013 An Introduction to Rheology: Phenomenon, Concept, Measuring, and Case Study Complex Fluids & Molecular Rheology Lab. , Department of Chemical Engineering

The XVIth International Congress on Rheology u Non-Newtonian Fluid Mechanics u Colloids and Suspensions

The XVIth International Congress on Rheology u Non-Newtonian Fluid Mechanics u Colloids and Suspensions u Advanced Experimental Methods u Emulsions and Foams u Materials Processing u Solids and Granular Materials u Polymer Solutions, Melts and Blends u Industrial Rheology u Biopolymers, Biofluids and Foods u Complex Flows u Constitutive and Computational Modeling u General Rheology u Rheology of Bio-Pharmaceutical Systems u Rheology of Nano- and Natural Composites u Interfacial Rheology, Micro-rheology & Microfluidics u Associative Polymers, Surfactants and Liquid Crystals u Professor Ken Walters Commemorative Symposium

Frequent Q & A o Q: Rheometer = Rheology? A: Unfortunately, the answer is,

Frequent Q & A o Q: Rheometer = Rheology? A: Unfortunately, the answer is, to a large extent, negative! o Q: How to judge the correctness of rheological data and know the physical meanings? A: Mostly, it’s all about theories or the predictions o Q: A practical processing issue can be well characterized by a set of rheological parameters? A: Well, ……………………. . let’s see!

o Rheology is the science of fluids or—more precisely— deformable materials Newton’s law of

o Rheology is the science of fluids or—more precisely— deformable materials Newton’s law of viscosity 牛頓流體 - 水、有機小分子溶劑等 黏度η為定值 非牛頓流體 - 高分子溶液、膠體等 Small molecule ● Macromolecule Deformable 黏度不為定值 (尤其在快速流場下)

非牛頓流體的特徵 o 非牛頓黏度 (Non-Newtonian Viscosity) - Shear Thinning Flow curve for non-Newtonian Fluids 牛頓流體

非牛頓流體的特徵 o 非牛頓黏度 (Non-Newtonian Viscosity) - Shear Thinning Flow curve for non-Newtonian Fluids 牛頓流體 (甘油加水) 非牛頓流體 (高分子溶液)

o 記憶效應 (Memory effects) - Elastic Recoil - Open Syphon Flow

o 記憶效應 (Memory effects) - Elastic Recoil - Open Syphon Flow

Time-dependent effects (搖變性) Thixotropy behavior Anti-thixotropy behavior A decrease (thixotropy) and increase (anti-thixotropy) of

Time-dependent effects (搖變性) Thixotropy behavior Anti-thixotropy behavior A decrease (thixotropy) and increase (anti-thixotropy) of the apparent viscosity with time at a constant rate of shear, followed by a gradual recovery when the motion is stopped The distinction between a thixotropic fluid and a shear thinning fluid: l A thixotropic fluid displays a decrease in viscosity over time at a constant shear rate. l A shear thinning fluid displays decreasing viscosity with increasing shear rate.

o 典型製程之流場強度範圍 Lubrication High-speed coating Rolling Spraying Injection molding Pipe flow Chewing Extrusion Sedimentation

o 典型製程之流場強度範圍 Lubrication High-speed coating Rolling Spraying Injection molding Pipe flow Chewing Extrusion Sedimentation Typical viscosity curve of a polyolefin- PP homopolymer, melt flow rate (230 C/2. 16 Kg) of 8 g/10 minat 230 C with indication of the shear rate regions of different conversion techniques. [Reproduced from M. Gahleitner, “Melt rheology of polyolefins”, Prog. Polym. Sci. , 26, 895 (2001). ]

o Melt instability Sharkskin Melt fracture Photographs of LLDPE melt pass through a capillary

o Melt instability Sharkskin Melt fracture Photographs of LLDPE melt pass through a capillary tube under various shear rates. The shear rates are 37, 112, 750 and 2250 s-1, respectively. [Reproduced from R. H. Moynihan, “The Flow at Polymer and Metal Interfaces”, Ph. D. Thesis, Department of Chemical Engineering, Virginia Tech. , Blackburg, VA, 1990. ] [Retrieved from the video of Non-Newtonian Fluid Mechanics (University of Wales Institute of Non-Newtonian Fluid Mechanics, 2000)]

o Instability for dilute solutions Taylor vortex R 1 R 2 [S. J. Muller,

o Instability for dilute solutions Taylor vortex R 1 R 2 [S. J. Muller, E. S. G. Shaqfeh and R. G. Larson, “Experimental studies of the onset of oscillatory instability in viscoelastic Taylor-Couette flow”, J. Non-Newtonian Fluid Mech. , 46, 315 (1993). ] Flow visualization of the elastic Taylor-Couette instability in Boger fluids. [http: //www. cchem. berkeley. edu/sjmgrp/]

典型均勻流場 q Two standard types of flows, shear and shearfree, are frequently used to

典型均勻流場 q Two standard types of flows, shear and shearfree, are frequently used to characterize polymeric liquids (a) Shear (b) Shearfree Steady simple shear flow Shear rate Streamlines for elongational flow (b=0) Elongation rate

q The Stress Tensor y x Shear Flow Total stress tensor* Stress tensor Hydrostatic

q The Stress Tensor y x Shear Flow Total stress tensor* Stress tensor Hydrostatic pressure forces z Elongational Flow

q 流變夾具種類與適用範圍 (a) Shear Concentrated Regime Homogeneous deformation: * Nonhomogeneous deformation: (b) Elongation Cone-and.

q 流變夾具種類與適用範圍 (a) Shear Concentrated Regime Homogeneous deformation: * Nonhomogeneous deformation: (b) Elongation Cone-and. Plate Parallel Plates Dilute Regime Concentric Cylinder Capillary Moving clamps For Melts & High-Viscosity Solutions *Stress and strain are independent of position throughout the sample

According to the Reptation Theory: Newtonian Zero-shear viscosity, 0 Power law

According to the Reptation Theory: Newtonian Zero-shear viscosity, 0 Power law

Relative Viscosity: Master curves for the viscosity and first normal stress difference coefficient as

Relative Viscosity: Master curves for the viscosity and first normal stress difference coefficient as functions of shear rate for the low-density polyethylene melt shown in previous figure Intrinsic Viscosity: Intrinsic viscosity of dilute polystyrene Solutions, With various solvents, as a function of reduced shear rate β

小振幅反覆式剪切流: 黏性與彈性檢定 Exp b: Small-Amplitude Oscillatory Shear Flow Oscillatory shear strain, shear rate, shear

小振幅反覆式剪切流: 黏性與彈性檢定 Exp b: Small-Amplitude Oscillatory Shear Flow Oscillatory shear strain, shear rate, shear stress, and first normal stress difference in small-amplitude oscillatory shear flow

It is customary to rewrite the above equations to display the in-phase and out-of-phase

It is customary to rewrite the above equations to display the in-phase and out-of-phase parts of the shear stress Storage modulus Loss modulus Storage and loss moduli, G’ and G”, as functions of frequency ω at a reference temperature of T 0=423 K for the low-density polyethylene melt shown in Fig. 3. 3 -1. The solid curves are calculated from the generalized Maxwell model, Eqs. 5. 2 -13 through 15

Molecular Architecture—The Fingerprints Linear Polymer Star Polymer Pom-Pom Polymer polybutadiene Polyisoprene C. C. Hua,

Molecular Architecture—The Fingerprints Linear Polymer Star Polymer Pom-Pom Polymer polybutadiene Polyisoprene C. C. Hua, H. Y. Kuo, J Polym Sci Part B: Polym Phys 38, 248 -261 (2000) S. C. Shie, C. T. Wu, C. C. Hua, Macromolecules 36, 2141 -2148 (2003)

拉伸流黏度量測與特徵 q Shearfree Flow Material Functions

拉伸流黏度量測與特徵 q Shearfree Flow Material Functions

H. Munstedt, J. Rheol. 24, 847 -867 (1980) Hua and Yang , J Polym

H. Munstedt, J. Rheol. 24, 847 -867 (1980) Hua and Yang , J Polym Res 9, 79 -90 (2002)

The Rheology of Colloidal Dispersions

The Rheology of Colloidal Dispersions

Onset of shear thickening : the Péclet number o Fluid drag on the particle

Onset of shear thickening : the Péclet number o Fluid drag on the particle leads to the Stokes-Einstein relationship: o The mean square of the particle’s displacement is Accordingly, the diffusivity sets the characteristic time scale for the particle’s Brownian motion. o A dimensionless number known as Péclet number, Pe

Lubrication hydrodynamics and hydroclusters Pe<<1 p The flow-induced density fluctuations are known as hydroclusters

Lubrication hydrodynamics and hydroclusters Pe<<1 p The flow-induced density fluctuations are known as hydroclusters which lead to an increase in viscosity. p The formation of hydroclusters is reversible, so reducing the shear rate returns the suspensions to a stable fluid Pe~1 Pe>>1 p At (Pe<<1) regime, random collisions among particles make them naturally resistant to flow. p As the shear rate increase (Pe~1), particles become organized in the flow, which lowers their viscosity. p At (Pe>>1) regime, the strong hydrodynamic coupling between particles leads to the formation of hydroclusters (red particles) which cause an increase in viscosity.

Controlling shear thickening fluids: to modify colloidal surface p The addition of a polymer

Controlling shear thickening fluids: to modify colloidal surface p The addition of a polymer “brush” grafted or absorbed onto the particles’ surface can prevent particles from getting close together. p The figure shows that shear thickening is suppressed by imposing a purely repulsive force field. p With the right selection of grafted density, molecular weight, and solvent , the onset of shear thickening moves out of the desired processing regime

Case Study I: 導電金屬漿流變性質的鑑定 1. Steady-state Viscosity 2. First normal stress difference 3. Linear

Case Study I: 導電金屬漿流變性質的鑑定 1. Steady-state Viscosity 2. First normal stress difference 3. Linear viscoelasticity

A C The Viscosity Curves of Steady Shear Flow B D

A C The Viscosity Curves of Steady Shear Flow B D

A C The 1 st Normal Stress Curves of Steady Shear Flow B D

A C The 1 st Normal Stress Curves of Steady Shear Flow B D

Screen Printing Technique Starting position for a screen printer squeegee medium gauze frame gap

Screen Printing Technique Starting position for a screen printer squeegee medium gauze frame gap (‘snap-off’) board holder emulsion mask board 1. The screen is fixed just above the board, and the medium lies in front of the flexible squeegee. 2. The mesh of the screen is pushed down into contact with the board by the squeegee as it moves across the screen, rolling the medium in front of it. The screen printing process medium drawn from open mesh snap-off 3. The squeegee blade first presses the medium into the open apertures of the image, and then removes the excess as it passes across each aperture. 4. The screen then peels away from the printed surface behind the squeegee, leaving the medium that was previously in the mesh aperture deposited on the board beneath http: //www. ami. ac. uk/courses/topics/0222_print/index. html#1

Versatile Optical Rheometry Lens Iris PEM Iris Objective lens Polarier Laser Pinhole Spatial filter

Versatile Optical Rheometry Lens Iris PEM Iris Objective lens Polarier Laser Pinhole Spatial filter & Beam expander Flow-LS (large-angle detection) Couette cell CCD Analyzer Rheology Rheo-SALS Lens Screen with aperture (from PEM) 1 f 2 f Photodiode Rheo-Birefringence Lock-in amplifiers

CASE STUDY II : Combined Rheo-Optical Measurements § Rheo-Optical Studies of Shear-Induced Structures in

CASE STUDY II : Combined Rheo-Optical Measurements § Rheo-Optical Studies of Shear-Induced Structures in Semidilute Polystyrene Solutions [Kume et al. (1997)] 1. Shear-induced structure formation in semidilute solutions of high molecular weight polystyrene was investigated using a wide range of rheo-optical techniques 2. The effects of shear on the semidilute polymer solutions could be classified into some regimes w. r. t. shear rate FIG. A complete picture of the shear-induced phase separation and structure formation from a wide range of techniques on the same polymer solutions

Continued Comparisons with Mechanical Characterizations: Mechanical Notice that the behavior of the shear viscosity

Continued Comparisons with Mechanical Characterizations: Mechanical Notice that the behavior of the shear viscosity is also classified into three regimes

Physics governing the fluid behavior

Physics governing the fluid behavior

Tips and Recommendations of problem solving Ø Identify an analogous model system that had

Tips and Recommendations of problem solving Ø Identify an analogous model system that had been studied earlier Ø Go through literature survey and read carefully and apprehensively Ø Design tactics for collecting preliminary data—experimental or computational Ø Discuss with your supervisor or counselor for the significance of the current data and appropriate next steps. Ø Repeat this procedure until the problem has been resolved to a satisfactory extent.