Introduction Material transport by atomic motion Diffusion couple:

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Presentation transcript:

Introduction Material transport by atomic motion Diffusion couple: eg., Cu-Ni in close contact; hold at elevated temperature for extended period and cool to room temperature. Chapter 5: Diffusion

Introduction continue… Before After Interdiffusion or impurity diffusion Self diffusion: same type of atoms; no composition change Chapter 5: Diffusion

Diffusion mechanisms Vacancy diffusion Interstitial diffusion Atom from normal lattice position changes position with an adjacent vacancy (vacancy lattice site). So, the atoms and vacancies travel in opposite directions. Both self- diffusion and inter (impurity)-diffusion can occur thus Chapter 5: Diffusion

Diffusion mechanisms continue … Source: William Callister 7th edition, chapter 5, page 112, figure 5.3(a) Chapter 5: Diffusion

Diffusion mechanisms continue … 2) Interstitial Diffusion Atoms move from one interstitial site to another (vacant) interstitial site. Source: William Callister 7th edition, chapter 5, page 112, figure 5.3(b) Chapter 5: Diffusion

Steady state Diffusion J=M/At If J is constant, steady-state diffusion exists. Where, J= rate of mass transfer with time, kg/m2-sec or atoms/m2- sec A= Area across which diffusion is occurring t= elapsed time, sec Chapter 5: Diffusion

Steady state Diffusion continue…. Concentration profile Source: William Callister 7th edition, chapter 5, page 113, figure 5.4 Chapter 5: Diffusion

Steady state Diffusion continue…. C: Concentration of diffusing species, kg/m3 or gm/cm3 x: Position Hydrogen gas across palladium plate Concentration Gradient: Slope at a particular point on the curve =dC/dx Chapter 5: Diffusion

Steady state Diffusion continue…. Fick’s first law of diffusion D = Diffusion coefficient, m2/sec dc/dx = Concentration gradient is the main driving force for diffusion (-) = Concentration gradient decrease Chapter 5: Diffusion

Steady state Diffusion continue…. = - Steady state Diffusion continue…. Problem Carbon diffusing through a plate of iron 5mm 10mm Carbon deficient rich Concentration: 1.2 kg/m3 0.8 kg/m3 Chapter 5: Diffusion

Steady state Diffusion continue…. = - Steady state Diffusion continue…. - Problem continue Diffusion coefficient: 3 x 10-11 m2/sec = 2.4 x 10-9 kg/m2-sec Chapter 5: Diffusion

Non-steady state Diffusion Diffusion flux and concentration gradient vary with time; net accumulation or depletion of diffusing species results ………… Fick’ second law ……… Modified Fick’s second law Chapter 5: Diffusion

Semi-Infinite solid Surface concentration at the other end is constant. eg, Bar of length, l > 10Dt , i.e., none of the diffusing atoms reach the bar end during the time-period of diffusion Assumptions: Co = Concentration before diffusion x = Distance; at surface it is 0. It increases into the solid t = Time; zero(0) at the instant diffusion starts Chapter 5: Diffusion

Semi-Infinite solid continue…. We have, for t=0, C=Co at 0≤x≤ For t>0, C=CS (Constant surface concentration) at x = 0 Also, C= CO at x= This equation shows relationship between concentration, position and time Error function Chapter 5: Diffusion

Semi-Infinite solid continue…. erf Where, CX=Concentration at depth x after time t. erf =erf2 Concentration at distance x, CX is a function of If time (t) and position (x) are known and CO, CS and D are given, CX can be determined Chapter 5: Diffusion

Semi-Infinite solid continue…. If CX=C1 at a specific concentration of solute, =constant Therefore =constant =constant Chapter 5: Diffusion

Semi-Infinite solid continue…. Surface concentration Concentration C at distance x Concentration before diffusion Chapter 5: Diffusion

Problem Carburization of steel using methane (CH4) at 950°C (1750°F) Steel: 0.25 wt% Carbon. Using CH4, carbon at surface is suddenly brought to and maintained at 1.2 wt% carbon. How long will it take to achieve a carbon content of 0.80% carbon at a position 0.5 mm below the surface? Chapter 5: Diffusion

Problem continue… D= 1.6 x 10-11 m2/sec Chapter 5: Diffusion

Problem continue… Chapter 5: Diffusion

Problem The diffusion coefficients for copper in aluminum at 500 and 600 C are 4.8x10-14 and 5.3x10-13 m2/s, respectively. Determine the approximate time at 500 C that will produce the same diffusion result (in terms of concentration of Cu at some specific point in Al) as a 10-h heat treatment at 600°C. To produce the same effect at 500°C, how long will it take? Chapter 5: Diffusion

Problem continue… Dt= constant Chapter 5: Diffusion

Factors in diffusion Temperature Time D increases 5 orders of magnitude with temperature Chapter 5: Diffusion

Factors in diffusion continue… Do = temperature independent pre-exponential (m2/sec) Qd = the activation energy for diffusion (J/mol,cal/mol and ev/atom) R = gas constant, 8.31 J/mol-K or 8.62 eV/atom-K T = absolute temperature (K) Chapter 5: Diffusion

Factors in diffusion continue… Chapter 5: Diffusion

Summary Self Diffusion Inter-Diffusion Steady state J=M/At Fick’s First law Non-steady state Fick’s second law Temperature effect Activation energy Chapter 5: Diffusion