Title: W A T K I N S - J O H N S O N C O M P A N Y Semiconductor Equipment Group
1Engineering 45
PhaseDiagrams (1)
Bruce Mayer, PE Registered Electrical
Mechanical EngineerBMayer_at_ChabotCollege.edu
2Learning Goals Phase Diagrams
- When Two Elements Are Combined, Determine the
Resulting MicroStructural Equilibrium State - For Example
- Specify
- a composition (e.g., wtCu - wtNi), and
- a temperature (T)
- a pressure (P)
- almost ALWAYS assume ROOM Pressure
- Determine Structure
3Learning Goals.2 Phase Dia.
- Cont Determine Structure
- HOW MANY phases Result
- The COMPOSITION of each phase
- Relative QUANTITY of each phase
4Definitions Phase Systems
- Component ? Pure Constituent of a Compound
- Typcially an ATOM, but can also be a Molecular
Unit - Solvent/Solute
- Solvent ? Majority Component in a Mixture
- Solute ? Minority Component in a Mixture
- System ? Possible Alloys Formed by Specific
Components (e.g. C-Fe Sys)
5The Solid Solubility Limit
- Solubility Limit ? Max Concentration of Solute
that will actually DISSOLVE in a Solvent to form
a SOLUTION
- Example Water-Sugar
- Add Sugar (Solute) to Water (Solvent)
- Initially ALL the Sugar Dissolves
- But after a Certain Amount, SOLID Sugar Starts to
Collect on the bottom of the Vessel
6The Solid Solubility Limit cont.
- Sol-Sol Quantitative Example
- At What wt Sugar does the Sugar NO Longer
Dissolve for - 20 C
- 80 C
- For 20 C
75
63
Sugar
- Cast Right from 20C
- Find Solid Sugar in Vessel at C0 63 wt
- For 80C, Again Cast Rt
- Find Solid Sugar in Vessel at C0 75 wt
- INcreased Temp INcreases Sol-Sol Limit
7Components Phases
- Components ? The elements or compounds which are
mixed initially (e.g., Al and Cu) - Phases ? The PHYSICALLY and CHEMICALLY DISTINCT
material regions that result from mixing
(e.g., a and b below)
8Effect of T Composition (C0)
- Changing T can change No. of phases path A to B.
- Changing C0 can change No. of phases path B to D
9Phase Equilibria
- Consider the Cu-Ni Alloy System
Crystal Structure electroneg r (nm)
Ni FCC 1.9 0.1246
Cu FCC 1.8 0.1278
- Both have the same crystal structure (FCC) and
have similar electronegativities and atomic radii
(c.f. Hume Rothery rules) suggesting high
mutual solubility. - Copper and Nickel are, in fact, totally miscible
in all Proportions
10Phase Diagrams
- Describes Phase Formation as a Function of T, C0,
P - This Course Considers
- binary systems 2 components
- independent variables T C0 (P 1atm in all
Cases)
11Phase Dia.s Phase No.s Types
- Rule-1 Given T C0 (for P 1 atm) then Find
- NUMBER TYPES of Phases Present
- Examples
- Pt-A (1100C, 60wt-)
- 1 Phase ? a the FCC Solid Solution
- Pt-B (1250,35)
- 2 Phases ? La
12Phase Dia.s Phase Composition
- Rule-2 Given T C0 (for P 1 atm) then Find
- The COMPOSITION (wt or at) for EACH Phase
- Example C0 35 wt Ni
- At TA
- Only Liquid
- CL CO 35 wt Ni
13Phase Dia.s Phase Comp. cont.
- Example C0 35 wt Ni
- At TD
- Only Solid (a-FCC)
- Ca C0 35 wt Ni
- At TB
- BOTH a and L
- Ca Csolidus
- 43 wt Ni
- CL Cliquidus
- 32 wt Ni
- Note the Use of the IsoThermal Tie Line at TB
to Find CL Ca
14Phase Dia.s Phase Wt Fractions
- Rule-3 Given T C0 (for P 1 atm) then Find
- The AMOUNT of EACH Phase in Wt-Fraction
- Example C0 35 wt Ni
- At TA
- Only Liquid
- WL 1.00 Wa 0.00 (wt Fracs)
- At TD
- Only Solid
- WL 0.00 Wa 1.00 (Fracs)
15Phase Dia.s Wt Fractions cont.
- Example C0 35 wt Ni
- At TB
- BOTH a and L
- Calc Wa,B WL,B Using the INVERSE LEVER RULE
16Lever Rule Proof
- Conservation of mass (Ni)
- Combine These Two Equations for WL Wa
- A Geometric Interpretation
Balance massXdist at Tip-Pt
17Cooling Cu-Ni Binary Phase-Sys
- Phase Diagram for Cu-Ni System ?
- System Characteristics
- BINARY ? 2 components Cu Ni
- ISOMORPHOUS ? Complete Solubility of one
Component in Another - At least One Solid Phase-Field Extends from 0 to
100 wt Ni
18Ex Cu-Ni Binary Cooling
- Consider 35 wt Ni Cooled 1300 C ? Rm-Temp
- Pt-A
- 1.00 Liquid
- 35 wt Ni
- Pt-B on Liquidus
- Tiny Amount of solid-a in Liq. Suspension
- Liq ? 35 wt Ni
- a ? 46 wt Ni
19Ex Cu-Ni Binary Cooling cont.
- Pt-C in 2-Ph Region
- (43-35)/(43-32) 0.727 Liquid
- Liq ? 32 wt Ni
- a ? 43 wt Ni
- Pt-D on Solidus
- Small Liq Pockets in Solid Suspension
- Liq ? 24 wt Ni
- a ? 36 wt Ni
- Pt E
- 1.00 a, _at_ C0
20NonEquilibrium Cooling
- Phases Diagrams are Constructed Under the
Assumption of ThermoDynamic Equilibrium - i.e., All Phases have Formed Sufficiently Slowly
to allow for HOMOGENOUS (same) Concentrations
WITHIN ALL Phases - In the Previous Example The Solid STARTS at 46
wt-Ni (pt-B) and ENDS at 35 wt-Ni (Pt-E) - Thus Solid particles that WERE 46Ni Had to CHANGE
to 35Ni by SOLID STATE DIFFUSION - But Solid-State Diffusion Proceeds Slowly
- Rapid Cooling Can result in NonUniform Comp.
21NonEquil Cool ? Cored Structure
- Ca Changes Composition Upon Cooling
- First a to solidify has Ca 46 wtNi
- Last a to solidify has Ca 35 wtNi
- Fast Cool Rate ? Cored structure
- Slow Cool Rate ? Equil. Structure
22Mech Props ? Cu-Ni System
- Recall Solid-Solution Strengthening
23WhiteBoard PPT Work
- Problems 9.5,6
- The Affect of PRESSURE on Phase Diagrams
- Water Ice, Has at Least TEN, yes 10, Distinct
Structural Phases - Phases form in Response to the PRESSURE Above
The Ice
24Ice is Nice Problem 9.5
- Given Ice-I at -15C 10atm ? Find MELTING and
SUBLIMATION PRESSURES
- Note Typo in Book
- Temperature needs to be 15 C for this to work
Starting Point
25Ice is Nice P9.5a Melt Temp
- At -15C Cast UPward to the Solid-LIQUID Phase
Boundary
- Find that Ice-I, when held at -15C, MELTS at
about 1000 atm (15000 psi, 100 Mpa)
1000
26Ice is Nice P9.5b Sublime Temp
- At -15C Cast DOWNward to the Solid-VAPOR Phase
Boundary
- Find that Ice-I, when held at -15C, VAPORIZES at
about 0.003 atm (0.0002 psi, 20 Pa)
0.003
27Ice is Nice P9.6 ? P 0.1 Atm
- At 0.1 Atm Cast RIGHTward to intercept the
Sol-Liq and Liq-Vap Phase-Boundaries
- Ice-I MELTS at ?2 C
- Water BOILS at ?75 C
- i.e., the VAPOR PRESSURE of Water at 75 C
is?10 of Atm
2.0
75