In-situ Heating Characterisation Using EBSD

Similar documents
Observation in the GB (Gentle Beam) Capabilities

EBSD Basics EBSD. Marco Cantoni 021/ Centre Interdisciplinaire de Microscopie Electronique CIME. Phosphor Screen. Pole piece.

EBSD Electron BackScatter Diffraction Principle and Applications

3D-EBSD an CrossBeam-Systemen

Introduction to Electron Backscattered Diffraction. TEQIP Workshop HREXRD Feb 1 st to Feb 5 th 2016

AN EBSD STUDY OF THE MICRO STRUCTURAL DEVELOPMENT DURING ANNEALING OF A FOLDED SUPER DUPLEX STAINLESS STEEL SHEET SAMPLE.

Applications of EBSD

Carnegie Mellon MRSEC

MODEL SEM Mill. Two independently adjustable TrueFocus ion sources

NEMI Sn Whisker Modeling Group Part 2:Future Work

In-situ Observation of Microstructure Change in Steel by EBSD

FUSION IN SITU HEATING AND ELECTRICAL. Protochips Quantifiably Better

Electron channelling contrast imaging (ECCI) an amazing tool for observations of crystal lattice defects in bulk samples

Diffraction Contrast Tomography. Unlocking Crystallographic Information from Laboratory X-ray Microscopy. Technical Note

QUANTITATIVE MICROSTRUCTURE ANALYSIS OF DISPERSION STRENGTHENED Al-Al 4 C 3 MATERIAL BY EBSD TECHNIQUE


Thermo Scientific ARL EQUINOX X-ray Diffractometers

Development of bimodal grain structures in microalloyed steels:

Model TEM Mill. Tabletop precision preparation for producing high-quality TEM specimens from a wide variety of materials EXCELLENCE MAGNIFIED

Texture Analysis in MSE

Rapid Imaging of Microstructure using Spatially Resolved Acoustic Spectroscopy

ORIENTATION DETERMINATION BY EBSP IN AN ENVIRONMENTAL SCANNING ELECTRON MICROSCOPE

AN INTRODUCTION TO OIM ANALYSIS

Thermo Scientific ARL EQUINOX 100. X-ray Diffractometers

Crystallographic Textures Measurement

MODEL TEM Mill. Two independently adjustable TrueFocus ion sources

Microstructural characterisation of as-deposited and reheated weld metal High Strength Steel Weld Metals

Stuart I. Wright EDAX-TSL, Draper, Utah

Practical 2P8 Transmission Electron Microscopy

Practical 2P8 Transmission Electron Microscopy

Microstructural Controls on Trace Element Variability in Ore Minerals

Grain Boundary Control for Improved Intergranular Stress Corrosion Cracking Resistance in Austenitic Stainless Steels

MODEL NanoMill TEM Specimen Preparation System. Ultra-low-energy, inert-gas ion source. Concentrated ion beam with scanning capabilities

A Quantitative Evaluation of Microstructure by Electron Back-Scattered Diffraction Pattern Quality Variations

JSM-7800F Field Emission Scanning Electron Microscope

Low kv EBSD using AZtecHKL and NordlysNano: Characterisation of a mollusc shell

Sr and Pb additions. L. Affleck, C. Leach *

Liverpool, UK, L69 3GP

Recrystallization textures in metals and alloys

MICROSTRUCTURE AND TEXTURE

Chapter 8: Strain Hardening and Annealing

Grain Contrast Imaging in UHV SLEEM

Deformation and fracture of an alpha/beta titanium alloy

Empirical constraints of shock features in monazite using shocked zircon inclusions

Application of Scanning Electron Microscope to Dislocation Imaging in Steel

ise J. A. Woollam Ellipsometry Solutions

Evolution of Microstructure and Texture Associated with Ridging in Ferritic Stainless Steels

MiniFlex. Analysis of materials by X-ray diffraction. Benchtop XRD diffractometer

Study of the Initial Stage and an Anisotropic Growth of Oxide Layers Formed on Zircaloy-4

Benchtop XRD diffractometer. MiniFlex. Analysis of materials by X-ray diffraction

MODEL 1061 SEM Mill ION MILLING. Ion milling is used in the physical. sciences to enhance the sample s surface. characteristics. Inert gas, typically

Three stages: Annealing Textures. 1. Recovery 2. Recrystallisation most significant texture changes 3. Grain Growth

Microtexture measurement of copper damascene line with EBSD

MODEL PicoMill TEM specimen preparation system. Achieve ultimate specimen quality free from amorphous and implanted layers

MICROSTRUCTURE CHARACTERIZATION OF GOES AFTER HOT ROLLING AND COLD ROLLING + DECARBURIZATION ANNEALING

Transzmissziós és pásztázó elektronmikroszkópos minták készítése ionsugaras vékonyítással

Quantitative X-ray Microanalysis Of Submicron Carbide Formation In Chromium (III) Oxide Rich Scale

Electron Microscopy Studies of Niobium Thin Films on Copper

MODEL 1051 TEM Mill ION MILLING. Ion milling is used on physical science. specimens to reduce thickness to electron

John de Laeter Centre

Exceptional Technology for Material Science TT DMA. Dynamic Mechanical Analyser

Layer Thickness Analysis of Thin Metal Coatings with. Bruker Nano Analytics, Berlin, Germany Webinar, June 8 th 2017

Development of a Reconstruction Method of Prior Austenite Microstructure Using EBSD Data of Martensite

COMPARISON OF TEXTURE IN COPPER AND ALUMINUM THIN FILMS DETERMINED BY XRD AND EBSD *

ATTACHMENTES FOR EXPLORER DIFFRACTOMETER. Monochromators

ATTACHMENTES FOR APD 2000 PRO POWDER X-RAY DIFFRACTOMETER. Monochromators

Combining Measurement Methods The Benefit of Fast Analytical Instruments

CHAPTER 4: The wetting behaviour and reaction of the diamond-si system

Transmission Kikuchi Diffraction in the Scanning Electron Microscope

Tutorial 2 : Crystalline Solid, Solidification, Crystal Defect and Diffusion

On-axis Transmission Kikuchi Diffraction in the SEM. Performances and Applications

Additive manufacturing

Experimental and theoretical investigation of the microstructural evolution in aluminium alloys during extrusion

CHAPTER FOUR METALLIC SUBSTRATES

In situ SEM observation of electromigration phenomena in fully embedded copper interconnect structures

Finding Grain and Antigrains. Matt Nowell May 2016

In Situ Observation of Dislocation Nucleation and Escape in a Submicron Al Single Crystal

Transmission Kikuchi Diffraction in the Scanning Electron Microscope

Mambo is the perfect tool for viewing EBSD data in pole and inverse pole figures.

Trust but verify: Ensure product quality at all stages of production

The X-MET8000 is great when you need accurate on-site alloy identification and chemistry in metal recycling and scrap yards.

Evolution of Recrystallization Texture in Aluminum Alloy Sheets by Asymmetric-Warm-Rolling

IMP EPD End Point Detector

Electron backscattered diffraction study of poly-si by Ni-mediated crystallization of amorphous silicon using a SiO 2 nanocap

ELECTRON BACKSCATTER DIFFRACTION (EBSD) THE METHOD AND ITS APPLICATIONS IN MATERIALS SCIENCE AND ENGINEERING

Combined EBSD & EDS analysis: Advances in modern materials characterization

Workshop of Electron backscatter diffraction (EBSD) in Scanning Electron Microscope

X-MET8000 Series. Sort scrap metal accurately, fast and maximise profits

Wavelength Dispersive XRF Spectrometer

Workshop of Electron backscatter diffraction (EBSD) in Scanning Electron Microscope

1P1b: Introduction to Microscopy

Evaluation of Solidification Cracking Susceptibility for Austenitic Stainless Steel during Laser Trans-Varestraint Test Using Twodimensional

Microstructural and Textural Evolution by Continuous Cyclic Bending and Annealing in a High Purity Titanium

Mathematical Modelling of an Annealing Furnace for Process Control Applications

The Study of SEM Examination of Crept Ceramic Samples Prepared by Cross Polishing Method

The use of holographic optics in laser additive layer manufacture. Prof John R Tyrer Dept of Mechanical & Manufacturing Engineering

Focused Ion Beam CENTRE INTERDISCIPLINAIRE DE MICROSCOPIE ELECTRONIQUE. Marco Cantoni, EPFL-CIME CIME ASSEMBLEE GENERALE 2007

Microstructure of Friction Stir Welded 6061 Aluminum Alloy

Study on Estimation Methods of Applied Stress using Fractography Analysis

Transcription:

Webinar In-situ Heating Characterisation Using EBSD

Speakers Dr. Ali Gholinia Dr. Neil Othen Dr. Jenny Goulden

Topics Introduction to EBSD Why do in-situ experiments? EBSD equipment requirements for in-situ experiments Application examples In-situ heating stage

In-situ Heating Characterisation Using EBSD Dr. Jenny Goulden Oxford Instruments

Principles of EBSD EBSD: Electron BackScatter Diffraction Automated collection & indexing of electron diffraction (Kikuchi) patterns from samples in the SEM Phosphor Screen General microstructural characterisation technique Pole piece Materials analysed Crystalline materials, e.g. Metals, ceramics, minerals, conductors and insulators Characterising: Local and macro crystallographic texture Grain boundary, grain size Phase distribution Strain distribution Detector (camera)

Why In-situ? In-situ experiments are performed in the SEM chamber Monitor change while experimenting on the sample Typically heating and/or tensile testing Specialised stages are used in conjunction with EBSD Increasingly used to study and understand solid state events: Microstructure development Recrystallisation and recovery Failure analysis Phase transformations and phase relationships Demonstrate importance using an ex-situ experiment

Ex-situ Application Local orientation maps from a Ni200 Alloy As received, Folded, 5, 10, 20 and 90 minutes annealing at 600 o C 200mm Folded 5 minutes 10 minutes 20 minutes 90 minutes Ubhi et-al, Materials Science Forum Vols. 715-716 (2012) pp 770-775

Ex-situ Application A lot of detail can be obtained from ex-situ experiments Limitations as continuity between the starting structure and final structure is lost Ideally observe the changes to a grain over time To observe and record these microstructure changes as they happen offers an additional dimension Increase in application of experiments in the SEM chamber (i.e. Insitu)

Analytical Challenges Analytical requirements for in-situ experiments include: Detector which operates effectively at elevated temperatures Infrared radiation can saturate the detector sensor Monitoring rapid dynamic events as they occur Requires a detection system that can collect, process and visualise EBSD data at suitable speeds Automatically collect data to monitor the microstructural changes Reliably collect maps sequentially as sample and conditions change

Detector Design Infrared radiation interference on the detector CCD: Silicon Background signal from thermal radiation Heater 900 C, 20 kv, 4 na Low signal to noise

Detector Design 2 possible solutions: Infrared filtering before the phosphor screen, typically using an additional (300 nm) Al coating on the phosphor Integrated infrared filter within the detector

Detector Design Background signal, heater temp 900 C, 0 na beam current Phosphor + Al 300nm coating Imperfections in coating Phosphor + Infrared filter

Detector Design Silicon sample, heater temp 900 C, 20 kv, 4 na Phosphor + Al coating Imperfections in coating Exposure time (220 ms) Phosphor + Infrared filter Best signal to noise, Exposure time (130 ms) NordlysMax 2 detector

Monitoring Dynamic Events Requirement to monitor real-time microstructural changes Need to collect EBSD maps in minutes (not hours) Requires a fast EBSD detection system EBSD data collected and indexed at hundreds of patterns a second Example application: phase transformation Austenite to Ferrite in low carbon steel High speed acquisition: each map collected in 6 minutes Captures details of dynamic events during phase transformation

Example: Phase Transformation 945 o C 895 o C 0 mins 895 o C 6 mins 880 o C ferrite austenite

Automation with Flexibility Capability to automatically collect a data sequence to record changes in microstructure Adaptability to change acquisition conditions during the run This can be demonstrated using the following application example: An Al alloy application investigating both deformation and recrystallisation Load applied maps were acquired at regular intervals Load removed, sample heated up to 320 C sequence of maps collected

Al 0.1% Mg - Tensile Strain and Heating GATAN Microtest EH2000 Band Contrast Local mis-orientation IPF Isochronal heating 290, 300 and 320 o C Scattered pole figures (IPF colours)

EBSD Solution The following application examples use: Oxford Instruments NordlysMax 2 fast detector (up to 870 Hz) integrated IR filter Oxford Instruments AZtec platform flexibility ease of Use automation quality data

In-situ Heating Characterisation Using EBSD Dr. Ali Gholinia Manchester University In-situ dynamic heating for Recrystallisation and Phase Transformation studies

Recrystallisation in Bronze and Steel Recrystallisation in Aluminium Phase transformation in Titanium Study of orientations in twin bands during phase transformation in Titanium

Before annealing After annealing Acknowledgements to Sylvia Campbell from MAHLE Engine Systems UK Ltd. for providing the Bronze samples.

IPF-X colour maps Thick black lines: High angle grain boundaries >10 Thin black lines: Low angle grain boundaries >2 Yellow lines: Twin boundaries Bronze Steel

Grains in random colours Thick black lines: High angle grain boundaries >10 Thin black lines: Low angle grain boundaries >2 Yellow lines: Twin boundaries Bronze Steel

Recrystallisation in Aluminium Al-0.1Mg Band Contrast Harvinder Singh Ubhi et al., Materials Science Forum, V.753, (2013), p. 7-10.

Recrystallisation in Aluminium Al-0.1Mg Local misorientation

Recrystallisation in Aluminium Al-0.1Mg IPF-Z colours In-situ heating up to 295 C of deformed Al-0.1Mg alloy

Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) Acknowledgements to Jack Donoghue from University of Manchester for providing the Ti samples.

30 C Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

200 C Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

400 C Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

600 C Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

925 C Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

950 C Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

Green: Ti-alpha (Hexagonal) Red: Ti-beta (Cubic) 20mm

Conclusions In-situ dynamic heating allows the direct investigation of specific grains during recrystallisation and phase transformation. This enables the study of the order of recrystallisation of each grain and link the information to their microstructure. Phase transformation studies benefit from the knowledge of orientations at high temperatures and relating them to low temperatures. This direct link would not be possible in the conventional ex-situ static heating analysis. The free surface during in-situ heating may have some unknown effect on the microstructure development, however comparison of the ex-situ and in-situ microstructures have not shown significant differences.

In-situ Heating Characterisation Using EBSD Dr. Neil Othen Gatan UK

Heating Protection for the SEM The heating stage must offer good thermal isolation, water cooling and heat protection shields for use at high temperatures Precise temperature control. The stage must be responsive, but with a high level of accuracy so transformations can be controlled and observed Stability Minimal drift throughout heating. This can be achieved through a uniform heating platform with minimal thermal gradients and good thermal insulation.

Heating Size of the heating stage To be suitable for techniques such as EBSD a heating stage must be compact so it can be moved and tilted to the correct orientation Imaging At high temperatures, need to consider the limitations of SEM detectors and impact of thermal electrons. A bias voltage applied to the stage can improve imaging by reducing thermal electrons from the specimen Ease of use How quickly can the SEM be returned to normal operation? For multiuser facilities minimal delay in fitting removing the heating stages maximises time running samples

In-situ heating stage Gatan has developed a robust universal heating stage with a novel compact design suitable for: SED and EBSD imaging. Its optimum shape ensures full compatibility with EBSD whilst a choice of user changeable shields ensures protection to the SEM is maintained. The stage enables dynamic EBSD analysis of samples with a high temperature accuracy <0.5 C and stability <0.5 C per hour up to temperatures of 950 C. Suitable for specimens up to several mm 3 in size, a bulk specimens allows easier handling and avoids mis-interpretations due to thin films and surface artefacts.

In-situ heating stage The Gatan model 525 heating stage is specifically designed to suit in-situ market requirements Small, yet powerful, with high tilt compatibility giving optimum EBSD signal Precise controlled heating of specimens up to several mm 3 in size - crucial to observe stable transformations A detachable specimen holder provides quick sample exchange and storage Opportunity to prepare and mount specimens away from the SEM

Model 525 Murano heating stage System comprises:

Model 525 Murano heating stage System comprises: Water-cooled base attached to the SEM stage. Base is designed to suit individual SEMs and is easy to fit/remove. SEM stage can be returned to normal use within minutes. Water cooling with a safety interlock ensures protection for the SEM stage. No water - heating power to stage is stopped.

Model 525 Murano heating stage System comprises: A transferable heating specimen holder The holder fits on to the water cooled base, its dovetail design allows it to be loaded quickly and securely in under 1 minute The removable holder design allows the user to mount their specimen away from the SEM and store it if required for future work Allows airlock loading as a special option

Model 525 Murano heating stage System comprises: Consumable, heated specimen platform Specimen sits on centre platform and is secured using high temperature cement to ensure good thermal contact. The replaceable platform Prevents contamination between specimens. Allows individual specimen storage.

Model 525 Murano heating stage Consumable heated platform and loading jig allow multiple specimens to be prepared and stored.

SE imaging above 600 C PHOTO PENDING EBSD imaging above 600 C A choice of shielding options is available. Shield may be removed below 600 C

A programmable PC based temperature control provides flexibility for a range of experiments. Data logging and time stamping allows EBSD maps to be synchronise. 52

A compact design allows full SEM integration SEM FIB Heating stage EBSD No need for specimen re-mounting, as it is tilted from the 0 tilt loading position. Making it suitable for several analytical and imaging techniques.

Model 525 Murano in-situ heating stage Dynamic testing is possible in-situ in the SEM, with specifically designed heating stages. A more efficient workflow allows a single specimen to be used to study a complete temperature range. Specimens can be prepared, mounted and stored ready for use to allow quick SEM access

Summary EBSD coupled with in-situ dynamic heating is a powerful tool for studying microstructure in the SEM Offers an insight to material behaviour in use Modern analytical equipment makes acquiring this data a reality

Further reading Two in-situ EBSD application notes Tensile / Heating of Al 0.1% Mg Alloy In-situ EBSD Analysis of an Al Alloy www.oxinst.com/insitu

Q&A Dr. Ali Gholinia Dr. Neil Othen Dr. Jenny Goulden