Katherine Faber

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Katherine Faber
Katherine T. Faber.jpg
Faber at the McCormick School of Engineering at Northwestern University
Born
Katherine Theresa Faber

(1953-06-19) June 19, 1953 (age 70)
Education
Spouse Thomas Felix Rosenbaum
Scientific career
Fields
Institutions
Doctoral advisor Anthony G. Evans

Katherine T. Faber is an American materials scientist and one of the world's foremost experts in ceramic engineering, material strengthening, and ultra-high temperature materials. Faber is the Simon Ramo Professor of Materials Science at the California Institute of Technology (Caltech). [1] She was previously the Walter P. Murphy Professor and department chair of Materials Science and Engineering at the McCormick School of Engineering and Applied Science at Northwestern University. [2]

Contents

Faber is known for her work in the fracture mechanics of brittle materials and energy-related ceramics and composites, including the Faber-Evans model of crack deflection which is named after her. [3] [4] [5] Her research encompasses a broad range of topics, from ceramics for thermal and environmental barrier coatings in power generation components to porous solids for filters and flow in medical applications. Faber is the co-founder and previous co-director of the Center for Scientific Studies in the Arts and also oversees a number of collaborative endeavors, especially with NASA's Jet Propulsion Laboratory.

Biography

Early life and education

Faber was the youngest daughter of an aspiring aeronautical engineer whose education was halted by the Great Depression. [6] As the only one of her siblings who had an interest in the sciences, she was encouraged by her father to pursue an education in engineering. An initial interest in chemistry evolved to an appreciation for ceramic engineering after Faber recognized its potential in solving many engineering problems. Faber eventually obtained her Bachelor of Science in Ceramic Engineering at the New York State College of Ceramics within Alfred University (1975). [2] She completed her Master of Science in Ceramic Science at Penn State University (1978) where she studied phase separation in glasses with Professor Guy Rindone. [2] After graduating with her MS, she worked for a year as a development engineer for The Carborundum Company in Niagara Falls, New York, on the development of silicon carbide for high performance applications such as engines. [7] Following her year in industry, Faber decided to pursue a Ph.D. in Materials Science at the University of California, Berkeley, which she completed in 1982. [2] [8]

Teaching, recognition

Katherine Faber lecturing on mechanical behavior of solids Katherine T. Faber.png
Katherine Faber lecturing on mechanical behavior of solids

From 1982 to 1987, Faber served as Assistant and Associate Professor of Ceramic Engineering at the Ohio State University. [9] She participated in the first class of the Defense Science Study Group, a program which introduces outstanding American science and engineering professors to the United States’ security challenges (1985–1988). [10] From 1988 to 2014, she taught as Associate Professor, Professor, and Walter P. Murphy Professor of Materials Science and Engineering at the McCormick School of Engineering at Northwestern University. During her time at Northwestern, she served as the Associate Dean for Graduate Studies and Research, overseeing more than $25 million in faculty research funds. [11] She went on to complete a 5-year term as department chair of Materials Science and Engineering at Northwestern, where she also served as the Chair of the University Materials Council (2001–2002), a collaborative group composed of directors of a number of materials programs from across the US and Canada. [2] Additionally, from 2005 to 2007 she sat on the Scientific Advisory Committee of the Advanced Photon Source at Argonne National Lab. [2] In 2014, she joined the teaching faculty at Caltech. [1]

From 2006 to 2007, Faber served as the President of the American Ceramic Society, [12] and in 2013 was named a Distinguished Life Member in recognition of her notable contributions to the ceramic and glass profession. [12] In 2014, Faber was elected to the American Academy of Arts and Sciences class of fellows. [9]

Faber at the WiMSE Reception Katherine Faber.jpg
Faber at the WiMSE Reception

She has also been recognized with:

Work

Research

Katherine Faber's research encompasses a diverse range of material science topics, focusing on fracture mechanics, shape memory materials, environmental barrier coatings (EBCs), additive manufacturing, boron nitride composites, and historical ceramics. Her work on shape memory materials investigates the martensitic transformation in zirconia-based ceramics. [14] Utilizing freeze-casting techniques, Faber's research group creates porous zirconia structures exhibiting shape memory behaviors. Through sol-gel synthesis and freeze-casting, she examines stress-induced shape memory and superelastic effects in oligocrystalline zirconia systems, addressing the volume change issue that causes premature cracking in bulk systems. [15]

Distinguished Lecture by Dr. Katherine Faber at UC Davis College of Engineering, Winter 2018 Distinguished Lecture by Dr. Katherine Faber at UC Davis College of Engineering, Winter 2018 (2) (cropped) (cropped).jpg
Distinguished Lecture by Dr. Katherine Faber at UC Davis College of Engineering, Winter 2018

Faber also explores the durability of environmental barrier coatings (EBCs) in high-temperature applications, such as gas turbine engines. [16] EBCs are essential for protecting ceramic matrix composites (CMCs) from degradation in combustion environments. Her research delves into the damage modes, including oxidation of the bond coat layer and the mismatch of thermal expansion coefficients, which lead to cracking and spalling. Faber employs advanced techniques like high-intensity X-rays at the Advanced Photon Source (APS) to measure internal strains, stresses, and damage evolution in EBC systems, aiming to understand the mechanisms and rates of oxidation failure and enhance the lifetime of these coatings. [17]

In collaboration with NASA's Jet Propulsion Laboratory, Faber works on advancing Hall-effect thrusters by developing a composite material that combines hexagonal boron nitride (h-BN) and graphite. [18] The brittle nature of bulk BN poses challenges under dynamic loads, prompting Faber's group to create a layered system where h-BN is grown on graphite through high-temperature carbothermal reduction. This composite material combines the desirable properties of both components, offering thermal emissivity, chemical inertness, and resistance to thermal shock while addressing the issues of oxidation and brittleness in dynamic environments. [19]

Faber's research group also examines historical ceramics, specifically Meissen porcelain, to understand and authenticate Böttger lusterware. [20] Using scientific methods such as X-ray diffraction, scanning electron microscopy, and chemical characterization, her group investigates the composition and manufacturing techniques of lusterware. By reverse-engineering these historical artifacts, her research provides insights into the materials and processes used in early 18th-century Meissen factories, contributing to the historical knowledge and preservation of these significant cultural artifacts. Her research interests also include silicon-based ceramics and ceramic matrix composites; [1] polymer-derived multifunctional ceramics; [12] graphite- and silicon carbide-based cellular ceramics synthesized from natural scaffolds, such as pyrolyzed wood; [12] and cultural heritage science, [9] with emphasis on porcelains and jades. [10]

Crack Deflection Model

Main Article: Faber-Evans model

Katherine Faber at the 2013 ACS Awards Katherine Faber Scientist.jpg
Katherine Faber at the 2013 ACS Awards

Katherine Faber and her PhD advisor, Anthony G. Evans, first introduced a materials of mechanics model designed to predict the enhancement of fracture toughness in ceramics. This is achieved by accounting for crack deflection around second-phase particles prone to microcracking within a matrix. [21] The model considers particle morphology, aspect ratio, spacing, and volume fraction of the second phase. Additionally, it accounts for the decrease in local stress intensity at the crack tip when deflection or bowing of the crack plane occurs.

Faber showed that by utilizing imaging techniques, the actual crack tortuosity can be determined, enabling the direct input of deflection and bowing angles into the model. The subsequent rise in fracture toughness is then contrasted with that of a flat crack in a plain matrix. The degree of toughening hinges on the mismatch strain resulting from thermal contraction incompatibility and the microfracture resistance at the particle/matrix interface. [22] This toughening effect becomes prominent when particles exhibit a narrow size distribution and are suitably sized.

Faber's analysis revealed that fracture toughness, regardless of morphology, is primarily determined by the most severe twisting of the crack front rather than its initial inclination. While the initial tilting of the crack front contributes to significant toughening in the case of disc-shaped particles, the twist component remains the dominant factor in enhancing toughness. [23] Additionally, she showed that the distribution of inter-particle spacing plays a crucial role in the toughening effect of spherical particles. Specifically, the toughness increases when spheres are in close proximity, causing twist angles to approach π/2. These insights by Faber formed the foundation for designing stronger two-phase ceramic materials. The Faber-Evans model is widely used by materials scientists to indicate that materials with approximately equiaxial grains can experience a fracture toughness increase of about twice the grain boundary value due to deflection effects. [24] [25]

Initiatives

Faber is the co-founder and co-director of the Northwestern University–Art Institute of Chicago Center for Scientific Studies in the Arts (NU-ACCESS), a collaboration between Northwestern University and the Art Institute of Chicago in which advanced materials characterization and analytical techniques are used to further conservation science for historical artifacts. [2] NU-ACCESS, the first center of its kind, provides opportunities for scientists and scholars from a variety of institutions to make use of the center's facilities to study their collections. [26]

Personal life

Faber is married to condensed matter physicist, and current president of the California Institute of Technology, Thomas F. Rosenbaum. [27] They began their careers at the California Institute of Technology in 2013 after Rosenbaum transitioned from his previous position as the John T. Wilson Distinguished Service Professor of Physics and university provost of The University of Chicago. [28] Together, they have two sons, Daniel and Michael. Apart from her research, Faber is a patron of the arts and is especially drawn to theater and art museums.

See also

Selected publications

Faber has authored over 150 papers, written three book chapters, and edited a book, Semiconductors and Semimetals: The Mechanical Properties of Semiconductors v. 37. [12] [29] In 2003, She was recognized by the Institute for Scientific Information as a Highly Cited Author in Materials Science. [2]

Related Research Articles

<span class="mw-page-title-main">Ceramic</span> An inorganic, nonmetallic solid prepared by the action of heat

A ceramic is any of the various hard, brittle, heat-resistant, and corrosion-resistant materials made by shaping and then firing an inorganic, nonmetallic material, such as clay, at a high temperature. Common examples are earthenware, porcelain, and brick.

In materials science, a metal matrix composite (MMC) is a composite material with fibers or particles dispersed in a metallic matrix, such as copper, aluminum, or steel. The secondary phase is typically a ceramic or another metal. They are typically classified according to the type of reinforcement: short discontinuous fibers (whiskers), continuous fibers, or particulates. There is some overlap between MMCs and cermets, with the latter typically consisting of less than 20% metal by volume. When at least three materials are present, it is called a hybrid composite. MMCs can have much higher strength-to-weight ratios, stiffness, and ductility than traditional materials, so they are often used in demanding applications. MMCs typically have lower thermal and electrical conductivity and poor resistance to radiation, limiting their use in the very harshest environments.

<span class="mw-page-title-main">Zirconium dioxide</span> Chemical compound

Zirconium dioxide, sometimes known as zirconia, is a white crystalline oxide of zirconium. Its most naturally occurring form, with a monoclinic crystalline structure, is the mineral baddeleyite. A dopant stabilized cubic structured zirconia, cubic zirconia, is synthesized in various colours for use as a gemstone and a diamond simulant.

<span class="mw-page-title-main">Brittleness</span> Liability of breakage from stress without significant plastic deformation

A material is brittle if, when subjected to stress, it fractures with little elastic deformation and without significant plastic deformation. Brittle materials absorb relatively little energy prior to fracture, even those of high strength. Breaking is often accompanied by a sharp snapping sound.

Thermal shock is a phenomenon characterized by a rapid change in temperature that results in a transient mechanical load on an object. The load is caused by the differential expansion of different parts of the object due to the temperature change. This differential expansion can be understood in terms of strain, rather than stress. When the strain exceeds the tensile strength of the material, it can cause cracks to form and eventually lead to structural failure.

In materials science, the sol–gel process is a method for producing solid materials from small molecules. The method is used for the fabrication of metal oxides, especially the oxides of silicon (Si) and titanium (Ti). The process involves conversion of monomers in solution into a colloidal solution (sol) that acts as the precursor for an integrated network of either discrete particles or network polymers. Typical precursors are metal alkoxides. Sol–gel process is used to produce ceramic nanoparticles.

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<span class="mw-page-title-main">Transgranular fracture</span>

Transgranular fracture is a type of fracture that occurs through the crystal grains of a material. In contrast to intergranular fractures, which occur when a fracture follows the grain boundaries, this type of fracture traverses the material's microstructure directly through individual grains. This type of fracture typically results from a combination of high stresses and material defects, such as voids or inclusions, that create a path for crack propagation through the grains. A broad range of ductile or brittle materials, including metals, ceramics, and polymers, can experience transgranular fracture. When examined under scanning electron microscopy, this type of fracture reveals cleavage steps, river patterns, feather markings, dimples, and tongues. The fracture may change directions somewhat when entering a new grain in order to follow the new lattice orientation of that grain but this is a less severe direction change then would be required to follow the grain boundary. This results in a fairly smooth looking fracture with fewer sharp edges than one that follows the grain boundaries. This can be visualized as a jigsaw puzzle cut from a single sheet of wood with the wood grain showing. A transgranular fracture follows the grains in the wood, not the jigsaw edges of the puzzle pieces. This is in contrast to an intergranular fracture which, in this analogy, would follow the jigsaw edges, not the wood grain.

<span class="mw-page-title-main">Fracture toughness</span> Stress intensity factor at which a cracks propagation increases drastically

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<span class="mw-page-title-main">Faber–Evans model</span> Phenomenon in solid-state physics

The Faber–Evans model for crack deflection, is a fracture mechanics-based approach to predict the increase in toughness in two-phase ceramic materials due to crack deflection. The effect is named after Katherine Faber and her mentor, Anthony G. Evans, who introduced the model in 1983. The Faber–Evans model is a principal strategy for tempering brittleness and creating effective ductility.

References

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  10. 1 2 Madsen, Lynnette D. 1963– VerfasserIn. (February 2016). Successful women ceramic and glass scientists and engineers 100 inspirational profiles. John Wiley & Sons. ISBN   978-1-118-73360-8. OCLC   953526292.{{cite book}}: |last= has generic name (help)CS1 maint: numeric names: authors list (link)
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  14. Zeng, Xiaomei; Arai, Noriaki; Faber, Katherine T. (2019). "Robust Cellular Shape-Memory Ceramics via Gradient-Controlled Freeze Casting". Advanced Engineering Materials. 21 (12). doi:10.1002/adem.201900398. ISSN   1438-1656.
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  16. Harder, Bryan J.; Ramìrez-Rico, Joaquin; Almer, Jonathan D.; Lee, Kang N.; Faber, Katherine T. (2011). "Chemical and Mechanical Consequences of Environmental Barrier Coating Exposure to Calcium–Magnesium–Aluminosilicate". Journal of the American Ceramic Society. 94 (s1). doi:10.1111/j.1551-2916.2011.04448.x. ISSN   0002-7820.
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  18. Chari, Celia S.; McEnerney, Bryan W.; Hofer, Richard R.; Wollmershauser, James A.; Gorzkowski, Edward P.; Faber, Katherine T. (2023). "High-temperature carbothermal synthesis and characterization of graphite/h-BN bimaterials". Journal of the American Ceramic Society. 106 (4): 2225–2239. doi:10.1111/jace.18927. ISSN   0002-7820.
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  20. Chari, Celia S.; Taylor, Zane W.; Bezur, Anikó; Xie, Sujing; Faber, Katherine T. (May 3, 2022). "Nanoscale engineering of gold particles in 18th century Böttger lusters and glazes". Proceedings of the National Academy of Sciences. 119 (18): e2120753119. Bibcode:2022PNAS..11920753C. doi: 10.1073/pnas.2120753119 . ISSN   0027-8424. PMC   9170166 . PMID   35446687.
  21. Faber, K. T.; Evans, A. G. (April 1, 1983). "Crack deflection processes—I. Theory". Acta Metallurgica. 31 (4): 565–576. doi:10.1016/0001-6160(83)90046-9. ISSN   0001-6160.
  22. Faber, K. T.; Evans, A. G. (April 1, 1983). "Crack deflection processes—II. Experiment". Acta Metallurgica. 31 (4): 577–584. doi:10.1016/0001-6160(83)90047-0. ISSN   0001-6160.
  23. Faber, K.T.; Evans, Anthony G. (1983). "Intergranular Crack-Deflection Toughening in Silicon Carbide". Journal of the American Ceramic Society. 66 (6): C–94–C-95. doi:10.1111/j.1151-2916.1983.tb10084.x. ISSN   0002-7820.
  24. Liu, Haiyan; Weisskopf, Karl-L.; Petzow, Gunter (1989). "Crack Deflection Process for Hot-Pressed Whisker-Reinforced Ceramic Composites". Journal of the American Ceramic Society. 72 (4): 559–563. doi:10.1111/j.1151-2916.1989.tb06175.x. ISSN   0002-7820.
  25. Carter, David H.; Hurley, George F. (1987). "Crack Deflection as a Toughening Mechanism in SiC-Whisker-Reinforced MoSi2". Journal of the American Ceramic Society. 70 (4): C–79-C-81. doi:10.1111/j.1151-2916.1987.tb04992.x. ISSN   0002-7820.
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  28. https://www.jpl.nasa.gov. "Caltech Announces New President". NASA Jet Propulsion Laboratory (JPL). Retrieved November 5, 2022.{{cite web}}: External link in |last= (help)
  29. Faber, KAtherine T. Molloy, Kevin J. (1992). The mechanical properties of semiconductors. Academic Press. ISBN   978-0-08-086434-1. OCLC   646758339.{{cite book}}: CS1 maint: multiple names: authors list (link)