Material of the Day – Metallic Clays Methylcellulose Binder Atomized Metallic Powders MAT_SCI 201/301 | S23 | 1 Lecture W5-2 Diffusion in Crystalline Solids and Polymers Pr. Jonathan Emery ANNOUNCEMENTS | April. 27th, 2023 Lecture Topic - Diffusion (Plug-in examples in supplemental video lecture.) Logistics - P-set W6/Quiz W6. Exams returned after class. Rewrites due May 4th. Morfli: Videos now embedded into Morfli Reading Morfli Ch. 7 MAT_SCI 201-301 | F21 MAT_SCI 201/301 S23• 2 Outline: Diffusion in Materials • Diffusion • Motivation and Basics • Brownian Motion to Random Walk • Discovering Fick’s Laws • Analysis with Fick’s Laws (2nd Law Analysis in Supplemental Video) • Diffusion Mechanisms • The Diffusion Coefficient and Structure/Temperature • Polymer Structure • Polymers and their applications • Polymer synthesis • Polymers and their characteristics • • • • Size [Video lecture] Shape Structure/Configuration Crystallinity MAT_SCI 201/301 | S23 | 3 Steady-state Diffusion – Across Plate The slope is the concentration gradient: MAT_SCI 201/301 | S23 | 4 Steady-state Diffusion • Flux independent of time: (if in steady-state, J does not change with time) • Flux is proportional to concentration gradient • The two are related by a diffusion constant (𝐷𝐷): (a material property, units m2/s) C1 Fick’s first law of diffusion If the slope is linear: C2 The concentration gradient is called the driving force for diffusion. Why negative? Ensures flux is positive when describing mass transfer from high to low concentration. MAT_SCI 201/301 | S23 | 5 Example: Chemical Protective Clothing (CPC) Methylene chloride is a common ingredient in paint removers. Besides being an irritant, it also may be absorbed through the skin. When using this paint remover, protective gloves should be worn. 1 2 If butyl rubber gloves (0.04 cm thick) are used, what is the diffusive flux of methylene chloride through the glove? Assume steady-state diffusion. Data: • Diffusion coefficient of methyl chloride in butyl rubber is: • Surface concentrations are: MAT_SCI 201/301 | S23 | 6 Example: Chemical Protective Clothing (CPC) Fick’s 1st Law Linear concentration profile. LD50 dose = 1.25 g/kg MAT_SCI 201/301 | S23 | 7 Non-Steady-State Diffusion • In most practical case non-steady-state diffusion is occurring: 1. 2. Flux and concentration gradient change with time at a position in the material Implies net accumulation or depletion of diffusing species. • The concentration of diffusing species changes with both time and position C = C (x,t) • In this case Fick’s Second Law is used: (Assumes D is independent of composition. This is a powerful approximation, but it is not always a good assumption.) • Second order partial differential equations (PDE) requires boundary conditions for physical solution. Known as a governing equation, because it governs the behavior of the system. MAT_SCI 201/301 | S23 | 8 Non-Steady-State Diffusion: Testing a Solution • There are only some mathematical functions that satisfies Fick’s Second Law. How can we test them? • How to test whether a proposed concentration profile C(x, t) satisfies Fick’s Second Law? • Example: Nope. Not a function that can describe diffusion. You are not solving differential equations. You are testing solutions. MAT_SCI 201/301 | S23 | 9 Example: • Cu Diffusion into a Semi-infinite Bulk of Al from a Constant Surface Concentration Copper diffuses into a long bar of Al and the surface concentration is held constant. Surface concentration: Cs of Cu atoms → bar pre-existing conc., C0 of copper atoms CS C(x,t) C0 x Boundary conditions (BCs) (at t = 0, constant concentration in bar) (constant surface concentration at all time) (semi-infinite solid) MAT_SCI 201/301 | S23 | 10 A Solution to the PDE • C(x,t) for a constant surface concentration into a semi-infinite solid can be expressed as: • C(x,t) is the concentration at point x at time t. erf(z) is the error function: • You do not need to solve this PDE, but you should be able to use/evaluate solutions I provide. After some time (at t = t1) MAT_SCI 201/301 | S23 | 11 A Solution to the PDE (VL) • C(x,t) for a constant surface concentration into a semi-infinite solid can be expressed as: • C(x,t) is the concentration at point x at time t. erf(z) is the error function: • I will tabulate erf values for you. You don’t have to evaluate it to get values. MAT_SCI 201/301 | S23 | 12 Example: Non-steady State Diffusion (VL) • An FCC iron-carbon alloy initially containing 0.20 wt% C is carburized at an elevated temperature in an atmosphere that provides a constant surface carbon concentration at 1.0 wt%. • If after 49.5 h the concentration of carbon is 0.35 wt% at a position 4.0 mm below the surface, determine the diffusion coefficient of the material. • Use • Boundary conditions 1.) Find D MAT_SCI 201/301 | S23 | 13 Example: Non-steady State Diffusion (VL) MAT_SCI 201/301 | S23 | 14 Outline: Diffusion in Materials • Diffusion • Motivation and Basics • Brownian Motion to Random Walk • Diffusion Mechanisms • Discovering Fick’s Laws • Analysis with Fick’s Laws • The Diffusion Coefficient and Structure/Temperature MAT_SCI 201/301 | S23 | 15 Diffusion in Solids • What’s odd about the picture below? How is diffusion proceeding? • How could those silver and orange atoms possibly exchange positions? Initially (at t = t0) After some time (at t = t1) MAT_SCI 201/301 | S23 | 16 Diffusion Mechanism #1: Vacancy-mediated Diffusion • • • Atoms “exchange” with vacancies, hopping into a vacant lattice position Vacancy-mediated diffusion is the mechanism for the motion of substitutional impurities and self-diffusion. Rate of diffusion depends on: • Number of vacancies present • Activation energy to “hop” • The energy in the system • What do these three independent variables suggest? General form – Arrhenius equation MAT_SCI 201/301 | S23 | 17 Diffusion Mechanism #2: Interstitial-mediated Diffusion • • • Diffusion proceeds through interstitial sites (triangular, tetragonal, octahedral…) Preferential pathways have minimum distortion from point A to point B. Generally faster or slower than vacancy diffusion? Why? Position of interstitial atom before diffusion (an atomic jump) Position of interstitial atom after diffusion (an atomic jump) MAT_SCI 201/301 | S23 | 18 The Diffusion Coefficient But wait – what is the diffusion coefficient, exactly? But… D0? → number that ties together material-dependent properties: e.g., lattice vibrational frequencies, entropic contributions, jump distance… It is a measured (or calculated), tabulated material property. Deeper investigation into the mature of D0 in upper-level MSE courses. MAT_SCI 201/301 | S23 | 19 Diffusion and Temperature • D has an exponential dependence on 1/T • Plotting the natural log of the diffusion coefficient vs. 1/T presents the data linearly: How to read this graph? MAT_SCI 201/301 | S23 | 21 Example: Diffusion Coefficient at Temperature What is the diffusion D coefficient of Cu in Si at 350 °C if: D(300 °C) is 7.8 x 10-11 m2/s and Qd = 41.5 kJ/mol? transform data MAT_SCI 201/301 | S23 | 22 Example: Diffusion Coefficient at Temperature What is the diffusion D coefficient of Cu in Si at 350 °C if: D (300 °C) is 7.8 x 10-11 m2/s and Qd = 41.5 kJ/mol? Sanity check → larger diffusion coefficient at higher temp… good. MAT_SCI 201/301 | S23 | 23 Factors Affecting the Diffusion Coefficient • Mechanism: in general, DInt. > DSub. • Temperature • Higher temperature, faster diffusion • Diffusion species: smaller → faster Crystal structure: more “open” (small APF) → faster Polymer structure more “open” (looser chain packing) → faster (more permeable) Bonding: stronger → slower (higher Qd) • Lattice imperfections: “short circuit” diffusion • • • • Much faster along dislocations, (grain boundaries), and external surfaces. MAT_SCI 201/301 | S23 | 24 Summary • Mass can be transported through solids by diffusion. • There are two diffusion atomistic mechanisms* that dominate in metallic and ceramic crystals – interstitial and vacancy (aka substitutional-mediated) diffusion. • Fick’s first law is a differential equation that describes time-independent diffusion flux across an (typically thin) interface. • Fick’s second law is a differential equation that describes time-dependent diffusion and is the case in most practical diffusion situations. • Diffusion can be influences by numerous factors – host lattice, density, diffusing species, bond type, temperature, etc. *Neglecting so-called short-circuit paths. MAT_SCI 201/301 | S23 | 27 Outline: Diffusion in Materials • Diffusion • Motivation and Basics • Brownian Motion to Random Walk • Discovering Fick’s Laws • Analysis with Fick’s Laws (2nd Law Analysis in Supplemental Video) • Diffusion Mechanisms • The Diffusion Coefficient and Structure/Temperature • Polymer Structure • Polymers and their applications • Polymer synthesis • Polymers and their characteristics • • • • Size [Video lecture] Shape Structure/Configuration Crystallinity MAT_SCI 201/301 | S23 | 30 Module Outcomes • Recognize the features within polymer structure hierarchy (chemistry, size, shape, architecture) and compare simple properties (melting temperature, strength, density) of polymers with varying structures. • Compute important values for polymer structures such as molecular weight, end-to-end distance, dispersity, etc, • Explain the roles of primary and secondary bonding in polymeric structures. • Discuss how polymers occupy space due to their intermolecular bonding, size, and conformation. • Understand how simple random walk models can lead to polymer conformation and conjecture about limitations and extensions of the model. • Differentiate between various types of polymer synthesis (chain-growth/step growth) and evaluate the affects these differences may have on polymer structure, namely molecular weight and dispersity. • Correlate polymer architecture with post-consumer processability (recycling). *Practice this. MAT_SCI 201/301 | S23 | 31 Structure in Polymers Chemistry Conformation Size Architecture H H H H H H C C C C C C H H H H H H Polyethylene (PE) H H H H H H C C C C C C H Cl H Cl H Cl Poly(vinyl chloride) (PVC) MAT_SCI 201/301 | S23 | 32 Polymers: Name That Polymer! MAT_SCI 201/301 | S23 | 33 Polymers: Natural The structure of wheat protein and response to hydration and shear. MAT_SCI 201/301 | S23 | 34 Ancient Human Uses of Polymers • Natural polymers used by ancient peoples: • Wood, Rubber, Wool • Cotton, Silk, Leather • Oldest known uses • Skins for clothing • Textiles (felts, woven cloth) • Wooden structures and weapons • Rubber ball *Pretty subjective. MAT_SCI 201/301 | S23 | 35 Polymers since ~1940 • Many plastics, rubbers, fibers used today are synthetic polymers… • Since WWII, synthetic polymers have revolutionized industry: • Cheap to produce • Highly tunable properties • Often superior to natural materials • Displaced metals and wood in many applications • Lower cost and superior/good enough properties • Environmental concerns… • Recycling • Resource usage and conservation • Sustainability • Toxicity MAT_SCI 201/301 | S23 | 36 What is a Polymer? Poly mer many repeat unit repeat unit repeat unit H H H H H H C C C C C C H H H H H H H H H H H H C C C C C C H Cl H Cl H Cl Polyethylene (PE) Adapted from Fig. 14.2, Callister & Rethwisch 8e. repeat unit H C H Poly(vinyl chloride) (PVC) H H C C CH3 H H H C C CH3 H H C CH3 Polypropylene (PP) MAT_SCI 201/301 | S23 | 37 Polymer Composition Most polymers are hydrocarbons* • Made up of H and C Strong covalent intramolecular bonds 4 valence e- per C atom 1 valence e- per H atom Weaker hydrogen and secondary intermolecular bonds Polymers therefore have relatively low melting/boiling points [or mer (C2H4)] *Others: polysiloxanes (silicones), polyphosphates (biological processes), S-based, B-based… n MAT_SCI 201/301 | S23 | 38 Physical Properties and Chain Length MAT_SCI 201/301 | S23 | 39 Bulk or Commodity Synthetic Polymers “Vinyl” “Teflon” “Styrofoam” Do not memorize repeat units. MAT_SCI 201/301 | S23 | 40 Bulk or Commodity Synthetic Polymers (cont’d) “Acrylic” “Phenolics” “Nylon” “Polyester” Do not memorize repeat units. MAT_SCI 201/301 | S23 | 41 Unsaturated Hydrocarbons • Each carbon not bonded to 4 other atoms • Other atoms or groups can bond to the original molecule • Double & triple bonds somewhat chemically unstable → can form new bonds. • Double bond found in ethylene or ethene (C2H4) • • 4-bonds, but only 3 atoms bound to C atoms Triple bond found in acetylene or ethyne (C2H2) Strength (dissociation energy) and chemical stability is not the same: https://pubs.acs.org/doi/full/10.1021/acs.jpca.6b03631 MAT_SCI 201/301 | S23 | 42 Polymerization and Polymer Chemistry • Chain-growth/addition polymerization • Monomer unit daisy-chained one at a time to form linear macromolecule • 3 stages: initiation, propagation, and termination: • Ethylene (monomer) reacted to form polyethylene Initiation Free Radical Monomer (ethylene) Propagation • Chain forms via sequential addition of monomer units • Active site (unpaired e-) transfers in each reaction step. Radicals for polyethylene: TiCl3 complexes. Watch it happen. MAT_SCI 201/301 | S23 | 43 Polymerization and Polymer Chemistry • Step-growth/Condensation polymerization Intermolecular reactions involving >1 monomer species giving off a low MW condensate (e.g., HCl) • Example: Nylon 6,10 • in Sebacoyl chloride cyclohexane in 6-diaminohexane water + Note – there is a distinction between step-growth and condensation reactions, but the vast majority of step-growth produce condensate. MAT_SCI 201/301 | S23 | 44 Let’s Make Some Nylon (Back-up Video Below) See nylon being pulled from solution: MAT_SCI 201/301 | S23 | 45 Exercise 8.1.1 MAT_SCI 201/301 | S23 | 46 Molecular Conformation of Polymers • Conformation is the shape of the polymer chain • Implies the shape that results due to the rotation about bonds. • Chain bending and twisting are possible by rotation of carbon atoms around their chain single bonds • It is not necessary to break the chain bonds to alter the molecular shape Adapted from Fig. 14.5, Callister & Rethwisch 8e. MAT_SCI 201/301 | S23 | 47 Chain End-to-End Distance, r • Rotation about bond: • Results in bending, coiling, or kinking of chain • Chain can entangle with itself or other chains. • Affects mechanical properties (elasticity and strength) • How to model the conformation of a polymer chain? • Why not random walk? • (Consider limitations in homework) • l = length between bonded atoms in chain • n = number of bonds in the molecule r << total chain length For polymer chains of typical lengths Derivation MAT_SCI 201/301 | S23 | 48 Polymer Molecule Classification [VL] (Architecture) Be able to identify/explain tfhe structural classifications above. MAT_SCI 201/301 | S23 | 51 Size - Molecular Weight [VL] • • Molecular weight, M: Mass of a mole of chains. MW can be extremely large. Low M Not all chains in a polymer are the same length! — i.e., there is a distribution of molecular weights High M • MW can be defined in several ways: • �𝑛𝑛 ) Number averaged, (𝑀𝑀 • Bin the chains into a set of ranges and determine the number fraction in each range • �𝑤𝑤 ) Weight averaged, (𝑀𝑀 • Based on total weight fraction of molecules within a given range. • Degree of polymerization, DP • Number of monomers per polymer chain MAT_SCI 201/301 | S23 | 52 Molecular Weight Distribution [VL] �𝑛𝑛 : number-average molecular weight: 𝑀𝑀 �𝑤𝑤 : weight-average molecular weight 𝑀𝑀 Break up molecular distribution into ranges: Mi = mean molecular weight in range i xi = number fraction of chains in size range i wi = weight fraction of chains in size range i Adapted from Fig. 14.4, Callister & Rethwisch 8e. MAT_SCI 201/301 | S23 | 53 Molecular Weight Distribution [VL] Number Fraction Weight Fraction Weight fraction is always* higher than number faction → Shifted towards large molecular weight molecules Adapted from Fig. 14.3, Callister & Rethwisch 8e. *There is one case this is not true… can you think of it? MAT_SCI 201/301 | S23 | 54 Determine the Average Mass of the Class [VL] • What is the average weight of the students in this class? • (a) Based on the number fraction of students in each mass range? • (b) Based on the weight fraction of students in each mass range? MAT_SCI 201/301 | S23 | 55 Determine the Average Mass of The Class: Solution [VL] Sort the students into weight ranges. 1. 1. • 40 lb ranges gives the following table: total number total weight MAT_SCI 201/301 | S23 | 56 Determine the Average Mass of The Class: Solution [VL] 1. Calculate the number fraction and weight fraction of students in each range : For example: for the 81-120 lb range MAT_SCI 201/301 | S23 | 57 Determine the Average Mass of Class, Solution [VL] MAT_SCI 201/301 | S23 | 58 �𝑛𝑛 vs 𝑀𝑀 �𝑤𝑤 [VL] The Use of 𝑀𝑀 • Number-average molecular weight is used when a property or interaction is dependent on number distribution. • Thermodynamic properties depending on number of molecules in a system. • Colligative properties (often in solution): • Vapor pressure • Glass transition temperature • Important for processing • Weight-average molecular weight is used when a property or interaction is dependent on the weight distribution. • Mechanical properties depend more highly on the number of large molecules • Tensile strength • Rigidity • Characterization: • Visible light scattering • X-ray scattering MAT_SCI 201/301 | S23 | 59 Degree of Polymerization (DP), Dispersity (Đ) • • DP is the average number of repeat units (monomers) per chain Dispersity Đ is a measure of the heterogeniety of the chains in the polymer H H H H H H H H H H H H H C C (C C ) C C C C C C C C H H H H H H H H H H H H H Where m = molecular weight of the repeat unit. Example, MAT_SCI 201/301 | S23 | 60 Why Do We Care About Polymer Size Distribution? • Molecular weight influences a broad spectrum of materials properties • Mechanical performance generally improves with molecular weight • Long chains interweave with each other → more interactions, higher thermal stability • Large molecular weights influences melt temperature and viscosity (higher) • Large molecular weights can increase entanglement, increasing tensile strength. MAT_SCI 201/301 | S23 | 61 Exercise 8.1.2 MAT_SCI 201/301 | S23 | 62 Exercise 8.1.2 MAT_SCI 201/301 | S23 | 63 Polymers: Chemistry, Size, Architecture, Conformation Size Chemistry H H H H H H C C C C C C H H H H H H Polyethylene (PE) H H H H H H C C C C C C H Cl H Cl H Cl Poly(vinyl chloride) (PVC) Shape/Conformation Architecture Adapted from Figs. 14.4, 14.6 Callister & Rethwisch 9e. MAT_SCI 201/301 | S23 | 64 Polymer Architectures • Linear • Repeat units joined end-to-end • Long flexible chains (“spaghetti”) • Extensive Van der Waals and hydrogen bonding between chains • Examples: HDPE, PVC, PS, Nylon, fluorocarbons • secondary bonding Linear Branched • Side-branch chains connected to main chain • Chain-packing efficiency reduced • Thermodynamically unavoidable (processing) • Lower density • Often weaker interchain interactions • Examples: LDPE Branched MAT_SCI 201/301 | S23 | 65 Molecular Structures • Cross-linked • Adjacent chains joined by covalent bonds • Occurs during synthesis • Non-reversible processing • Examples: Rubbers (via vulcanization using sulfur) • Cross-Linked Network • Monomers forming 3 or more covalent bonds • Form 3-D networks • Examples: Epoxies, polyurethanes, phenol-formaldehyde Network MAT_SCI 201/301 | S23 | 66 Molecular Structures for Polymers • Generalized chain configurations and strength Increased Strength secondary Branched bonding Linear Cross-Linked Network • Thermoset Polymers • Thermoplastic Polymers • Covalent bonds between chains or • Secondary bonds between chains formation of network polymers *Branched and linear may be interchanged, depending on specifics. and network may be interchanged, depending on specifics. *Cross-linked MAT_SCI 201/301 | S23 | 67 Polymer types • Thermoplastics • Thermosets • Linear polymers with 2 links/mer • Branched with flexible chains • Weak secondary bonds between chains • Strong bonds within chains • • • They can be softened (and melted) repeatedly by raising the temperature • Relatively soft • Can be recycled • Examples: PE, PVC *This isn’t strictly true, but it is true in practice. However, clever people are making developments. Crosslinked with 3 links/mer or network polymers • Rigid character to strong, immovable covalent bonds After a thermoset is formed, it cannot* be reshaped or remelted • Difficult to recycle* • Examples: vulcanized rubber, epoxies, polyester resins MAT_SCI 201/301 | S23 | 68 Exercise 8.1.3 MAT_SCI 201/301 | S23 | 69 Exercise 8.3.1 MAT_SCI 201/301 | S23 | 70 Summary • Most polymeric materials are composed of large molecular chains with some size distribution. • Molecular: • Chemistry • Size (molecular weight/degree of polymerization) • Shape (conformation), • Architecture (linear…network) • Crystallinity • Polymers are highly engineerable materials – a key principle of this engineering is influencing the interchain interaction. MAT_SCI 201/301 | S23 | 73