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Non-ambient Diffraction in the Laboratory Environment Energy, Mining and Environment Pamela Whitfield Accuracy in Powder Diffraction IV, NIST, April 2013
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Pamela Whitfield

Feb 11, 2022

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Page 1: Pamela Whitfield

Non-ambient Diffraction in the Laboratory Environment

Energy, Mining and Environment

Pamela Whitfield

Accuracy in Powder Diffraction IV, NIST, April 2013

Page 2: Pamela Whitfield

Overview • Why work in the lab when synchrotron data is better?

• ‘A bird in the hand….’ (i.e. access!)

• Commercial stages • Some example developments • Sample displacement – the old irritant…

• DIY setups • Considerations and ‘mind-set’ • Low temperature capillary – high speed data with mirror optics & PSD • High gas pressure – a special case and big headache?

• Iron ore sintering - high speed data collection using curved PSD

Page 3: Pamela Whitfield

Commercial vendors… • Some developments…

• Tensile test stage

• Dome stages for 2D detectors

• Extremely-low temperature

• Close-cycle coolers → cryogen-free cold stream

• Combined XRD-DSC (Rigaku)

Oxford Cryosystems Phenix

mri BTS-BASIC

Anton-Paar TS 600

Cryo Industries close cycle cooler

Page 4: Pamela Whitfield

Sample displacement – different approaches • Z-stepper motor on HTK1200 oven

• Has to be properly calibrated

Triclinic-hexagonal phase transition of Ca10(AsO4)6F2 apatite in HTK1200 equipped with z-stepper motor

Whitfield et al, J.Appl.Cryst., 40 (2007), p1019

Page 5: Pamela Whitfield

Parallel-beam geometry

•No sample displacement peak shifts

2 Theta (degrees)34.0 34.5 35.0 35.5 36.0

Inte

nsity

(cou

nts)

0

200

400

600

800

1000

1200

1400 -0.6 mm -0.5 mm -0.4 mm -0.3 mm -0.2 mm-0.1 mm0.0 mm0.1 mm 0.2 mm0.3 mm0.4 mm0.5 mm0.6 mm

Al2O3 104 reflection with displacement (twin mirrors)

Lin

(Cou

nts)

0

1000

2000

3000

4000

5000

2-Theta - Scale25.8 26

α → β-quartz transition

shift in α-quartz lattice expansion only

Can have confidence that these shifts are real…

Page 6: Pamela Whitfield

2 (degrees CuK)26.2 26.4 26.6 26.8 27.0

Inte

nsity

Bragg-Brentano (2.3+2.3º Sollers)GM (5+2.3º Sollers) Twin mirror (5+5º Sollers)GM+PSD (2.3+?º Sollers)

• Lower peak resolution

• Choice of Soller slits a factor….

Parallel-beam : the down-side

Comparison of the main quartz reflection from different optics

Page 7: Pamela Whitfield

No-one sells what you want? now the fun starts… • Mind set – it’s a complete system, not just a stage

• Some engineering restrictions • Size • Stage weight (vertical goniometers) • Access to pass-throughs • θ−θ (don’t foul arms!) • Door closure

Example where engineering restrictions complicate things: Bulk (clearance+heat) Heavy – 10kg High pressure line pass-through transducer, thermocouples & heaters

Page 8: Pamela Whitfield

Low temperature capillary work • System specced and built specifically for rapid low T non-

ambient phase studies with large capillaries (before Oxford Cryo Compact was available!)

• Laminar flow along capillary axis minimizes LN2 usage without icing (goniometer heat shield needed)

• Vertical goniometer

• Limited space for nozzle

• Long transfer line not good (if you can get it inside) • Put dewar inside the cabinet?

Heat shield on goniometer head

Page 9: Pamela Whitfield

Look familiar?

Page 10: Pamela Whitfield

NH4NO3 phase transitions • Focussing mirror

optics, cryoflow with linear PSD

• Snapshots, 8° window, 2 second datasets every 2°C

• Continuous temperature ramp (0.1°C/s)

Proof of concept. Phase transitions of NH4NO3

Page 11: Pamela Whitfield

Something more practical…. • Ability to automate complex ramp-soak programs

• 4 minute datasets - shorter than ramp/dwell times

• 48 datasets in ~7 hours

Phase behaviour of the Li-battery electrolyte solvent dimethyl carbonate

Page 12: Pamela Whitfield

Beyond CuKα ...

• Engineering for high pressures often dictates use of higher energies for optimal usage..

• 1st mainstream company to venture down this route….?

• Anton-Paar HPC-900 • 100 bar pressure for H2, etc • Requires MoKα

– Not a simple add-on

Page 13: Pamela Whitfield

DIY under pressure? • Home-designed and built pressure vessels?

• Space for sample stage and ancillary stuff limited

• The elephant in the cupboard

• The pressure codes (ASME in North America)

• Restricts the materials you can use • What conditions you can use them under (max stress, temp) • Design concepts and validation • QC and manufacture Just one of the ASME

pressure codes…

Page 14: Pamela Whitfield

DIY thought process… 300bar, 300°C • 3 years from concept to delivery

• No modifications – have to think of everything 1st time!

Cover retention . Strong enough but removable using 12 tapered pins

Corrosion-resistant C22 Ni superalloy. Adjustable Ta

knife-edge

Heavy-duty! Strong enough at temp with ASME allowables + a bit

Fittings also need to be corrosion-resistant

Page 15: Pamela Whitfield

300bar NRC pressure vessel • Window is the weak-spot

• Swagelok-type seal (regulator comfort!) • Be window material for transmission • Be corrosion protection? • Strength? (structural grade SR200)

• Windows 6¼ mm thick Be • 2µm Ta coating

• Interior flooded with water/steam

• Interior beampath ca. 15 mm

• Penetration is key…..

Ta-coated window. Notches stop window rotating when tightening

Flooded means flooded..

Page 16: Pamela Whitfield

The exception rather than the rule… • In this case AgKα (22 keV) needed for increased

transmission

• Has consequences…. • Getting hold of a tube • 1.5kW versus 3kW (LFF) • Require new PSD optimized for higher energies • Pd β-filter effects even worse

• Difference between no signal and some signal

• Increase in accuracy = ∞

Calculated transmission through the GEN1 pressure stage at

different energies

Page 17: Pamela Whitfield

2Th Degrees292827262524232221201918171615141312111098

Cou

nts

1,500

1,400

1,300

1,200

1,100

1,000

900

800

700

600

500

400

300

200

100

0

-100

Corundum 100.00 %

Can you actually see anything? • Worst case - fully flooded with cold water

• Total beampath • 12.5mm Be, 8µm Ta, 15mm water

View through dummy windows

SRM1976 plate 20 minute scan AgKα 500µm Lynxeye (no monochromator/mirror – budget cut!)

Page 18: Pamela Whitfield

Anything else easy in comparison… • Autoclave conditions ~190°C

• 161psi steam + 100psi CO2

2Th Degrees30292827262524232221201918171615141312111098

Coun

ts

5,500

5,000

4,500

4,000

3,500

3,000

2,500

2,000

1,500

1,000

500

0

Corundum 100.00 %

Page 19: Pamela Whitfield

Iron Ore Sintering - In Situ X-ray Diffraction

Industrial sinter machine

Australian Synchrotron

X-rays Gas inlet

Detector High-temperature chamber

+

Heating Regime 25-1350-25°C pO2 = 5 x 10-3 atm

Page 20: Pamela Whitfield

Introduction – Industrial Context Iron ore sintering = important stage of the steelmaking process

SFCA is the ‘glue’ phase for sinter

Nathan A.S. Webster et al., Metall. Mat. Trans. B, 2012, 43, 1344-1357

SFCA and SFCA-I bonding matrix CaCO3 flux

Iron ore fines < 6.3 mm Fe2O3, FeOOH

C ~1300°C

Fe2O3, Fe3O4

SFCA = Silico-Ferrite of Calcium and Aluminium SFCA = M14O20 , SFCA-I = M20O28 , M = Fe, Ca, Si, Al

Page 21: Pamela Whitfield

Results – Heating, 25-1350°C Fe3O4 + melt

SFCA

Temperature (°C

)

Ca2Fe2-xAlxO5

CaFe2O4

Al(O

H)

3 SiO

2

CaC

O3

Fe2O

3

CFA*

*New phase

SFCA-I

Nathan A.S. Webster et al., Metall. Mat. Trans. B, 2012, 43, 1344-1357

Page 22: Pamela Whitfield

Iron Ore Sinter Studies Laboratory Based in situ Data Collection

• Beamtime hard to get • Waiting time ~ 6 months

• Once phases known from synchrotron experiments – use lab instrumentation

• INEL CPS120 • Incident beam, multilayer

mirror for high intensity

• CoKα Gas inlet

Gas outlet

High temperature chamber to 1500°C

Detector

X-ray optics

Strip heater Lab diffractometer setup

Page 23: Pamela Whitfield

Iron Ore Sinter Studies Laboratory Based in situ Data Collection

• Heating rate • 20°C min-1, 25 600°C • 10°C min-1, 600 1350°C

• Data collection time • 30 sec for 120° 2θ

• Resolution not as good as synchrotron but most information still visible

• Problem • Industry not so interested if

conditions not close to real processing conditions

Page 24: Pamela Whitfield

Actual Industrial Heating Rates? Attempt to Emulate in Laboratory • Heating rate

• 200°C min-1, 25 1350°C

• Data collection time • 6 sec for 120° 2θ

• Major and some minor phases still apparent

Typical industrial time-temperature profile

Tem

pera

ture

(°C)

1200

1000

800

600

400

200

2 64 8 100

Time (mins)

Page 25: Pamela Whitfield

Conclusions • Lab studies still have a role to play

• Easy access and the freedom to ‘play’

• Think holistically! • In-situ stages don’t work in isolation • Source, optics and detector can be changed/tweaked • Integration with diffractometer systems desirable but not vital

• Think beyond CuKα

• High gas pressure is a real pain (or the regulations are) • “abandon hope all ye who pass here!”

Page 26: Pamela Whitfield

Acknowledgements

• Ian Madsen • Iron ore sintering study

• Cryo Industries of America • Customizing one of their cryo systems for my needs…

• Jim Ross (NRC-DFS) and All-Weld • High pressure gas cell

Page 27: Pamela Whitfield

Questions?