Upload
laura-carpenter
View
76
Download
0
Embed Size (px)
Citation preview
0 10 20 30 40 50 60 70 800
20
40
60
80
100
120
140
160
2θ (degrees)
Inte
nsity
IntroductionThe microstructure analysis of thermoelectric oxides like Ca3Co4O9 is fundamental to the research of thermoelectric power generation devices. These devices provide a means of utilizing waste heat to make power; thus, improving the sustainability of energy. Analysis techniques for studying the p-type semiconductor Ca3Co4O9 were explored in this study. Also, β-FeO(OH) was investigated which is useful in magnetic recording media.
Experiment
Synthesis of Iron Powder: • FeCl3 + Urea + H2O • Solution placed in high preactor• Particles centrifuged after
removed from preactor
Determination of appropriate XRD and SEM parameters for analysis:• Adjust XRD scan speed, lens size, and
angle increment• Adjust SEM preparation method,
voltage applied, detector mode, and working distance
0 10 20 30 40 50 60 70 800
50
100
150
200
250
300
350
2θ (degrees)
Inte
nsity
ObjectiveDetermine appropriate XRD settings to get well-defined peaks for Ca3Co4O9 pellet sample and β-FeO(OH) powder sample. Determine appropriate SEM settings to get clear SEM images for β-FeO(OH).
Scan Angles: 5°-62°Increment: 0.05Scan Speed: 16 sec/stepMode: 1DAbsorber: 1
Scan Angles: 5°-80° Increment: 0.05°Scan Speed: 8 sec/stepMode: 0DAbsorber: 1
Scan Angles: 5°-80° Increment: 0.05°Scan Speed: 38 sec/stepMode: 1DAbsorber: 1Lens: 0.2 mm
SEM Images for β-FeO(OH)
Preparation: particles dispersed on double sided copper tape attached to sample mount
Preparation: particles mounted on silicon wafer and coated with platinum
XRD Results for β-FeO(OH)
Scan Angles: 10°-80° Increment: 0.05°Scan Speed: 13 sec/stepMode: 1DAbsorber: 1Lens: 0.1 mm
10µm
Conclusions
1 µm
XRD • Ca3Co4O9 pellets require a scanspeed of 16 sec/step for distinguishable peaks• β-FeO(OH) powder requires a scanspeed of 38 sec/step • Powders require a higher scan speed than pellets• A larger lens size produces higher peaksSEM• β-FeO(OH) powder must be attached to a silicon wafer and coated with a conductive
coating to get clear images• β-FeO(OH) particles were roughly 500 nm with a narrow particle size distribution and
a needle-like shape
XRD Results for Ca3Co4O9
References[1] Michitaka OHTAKI, Recent aspects of oxide thermoelectric materials for power generation from mid-to-high temperature heat source, Journal of the Ceramic Society of Japan, 119 (11), 770-775.[2] Jeffrey W. Fergus, Oxide materials for high temperature thermoelectric energy conversion, Journal of the European Ceramic Society, 32 (2012) 525-540.[3] http://www.sciencedirect.com/science/article/pii/S0010938X03000787[4] http://www.easyfairs.com/de/events_216/labotec-suisse2012_24924/labotec-suisse-2012_24925/visitors_24926/ausstellerkatalog_24937/stand/337587/[5] http://serc.carleton.edu/research_education/geochemsheets/techniques/XRD.html[6] http://www.nanocenter.umd.edu/new_facilities/NispLab.php
[1]
[4]
Acknowledgements• I want to thank Xueyan Song and Maria Alejandra Torres Arango for their assistance as
well as the WVU Shared Facilities for their assistance and access to the XRD and SEM.• This research was sponsored by NSF Divisions of Materials Research and Chemistry
(DMR-1004431).
0 10 20 30 40 50 600
200
400
600
800
1000
1200
1400
2θ (degrees)
Inte
nsity
(002
)
(003
) (004
)
(005
)
(006
)
(001
)
(202
)
0 10 20 30 40 50 60 70 800
200400600800
10001200140016001800
2θ (degrees)
Inte
nsity
(110
)
(200
)
(310
)
(211
)
(521
)
(411
)
(420
)
SEMHydrothermal Reactor
Thermoelectric Unicouple Ca3Co4O9 crystal structure β-FeO(OH) crystal structure
XRD
[2] [3]
[5] [6]
Laura E. Carpenter, Xueyan Song, and Maria Alejandra Torres ArangoDepartment of Mechanical and Aerospace Engineering, West Virginia University, Morgantown, WV 26506-6045
Microstructure Analysis of Ca3Co4O9 and β-FeO(OH) using XRD and SEM