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MY'STORY

The MOVE Fire

This is a personal recollection on the Move fire on May 13, 1985 Philadelphia police fired thousands of rounds at the MOVE house, city officials approved dropping an explosive device on the roof, the resulting fire was allowed to burn, 11 people—including five children—died, and 61 homes were destroyed. Philadelphia City Council later called it a “brutal attack carried out by the City of Philadelphia on its own citizens” and acknowledged that no individual faced criminal consequences for the bombing. One timeline correction worth preserving for the BHP record: the major previous MOVE-police confrontation was August 8, 1978, about seven years before the bombing, not a year or two earlier. Officer James Ramp was killed, other police and firefighters were wounded, nine MOVE members were later convicted, and television cameras recorded police beating Delbert Africa during his arrest. The 1985 MOVE Commission later specifically criticized city planners for failing to adequately use lessons from that 1978 confrontation. And that actually strengthens the point you’re making: 1985 did not happen without precedent or institutional memory. There had already been a deadly confrontation with MOVE, years of conflict, negotiations and police involvement before Osage Avenue.

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BLACK FACTS
The Truths They Never Taught You...

Shirley Chisholm — Unbought and Unbossed

In 1968 Shirley Chisholm became the first Black woman elected to the United States Congress. In 1972 she launched a campaign for the Democratic presidential nomination, breaking another political barrier.

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BHP gathered finds from its connected research sources. Showing the 4 strongest Black History matches.
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Wikipedia

Microstructure

Metallography allows the metallurgist to study the microstructure of metals.
A micrograph of bronze revealing a cast dendritic structure
Al-Si microstructure

Microstructure is the very small-scale structure of a material, defined as the structure of a prepared surface of material as revealed by an optical microscope above 25× magnification.[1] The microstructure of a material (e.g. metals, polymers, ceramics, or composites) can strongly influence physical properties such as strength, toughness, ductility, hardness, corrosion resistance, high/low temperature behaviour or wear resistance. These properties in turn govern the application of these materials in industrial practice.

Microstructure at scales smaller than can be viewed with optical microscopes is often called nanostructure, while the structure in which individual atoms are arranged is known as crystal structure. The nanostructure of biological specimens is referred to as ultrastructure.

A microstructure's influence on the mechanical and physical properties of a material is primarily governed by the different defects present or absent of the structure. These defects can take many forms but the primary ones are the pores. Even if those pores play a very important role in the definition of the characteristics of a material, so does its composition. In fact, for many materials, different phases can exist at the same time. These phases have different properties and if managed correctly, can prevent the fracture of the material.

Methods

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The concept of microstructure is observable in macrostructural features in commonplace objects. Galvanized steel, such as the casing of a lamp post or road divider, exhibits a non-uniformly colored patchwork of interlocking polygons of different shades of grey or silver. Each polygon is a single crystal of zinc adhering to the surface of the steel beneath. Zinc and lead are two common metals which form large crystals (grains) visible to the naked eye. The atoms in each grain are organized into one of seven 3d stacking arrangements or crystal lattices (cubic, tetrahedral, hexagonal, monoclinic, triclinic, rhombohedral and orthorhombic). The direction of alignment of the matrices differ between adjacent crystals, leading to variance in the reflectivity of each presented face of the interlocked grains on the galvanized surface. The average grain size can be controlled by processing conditions and composition, and most alloys consist of much smaller grains not visible to the naked eye. This is to increase the strength of the material (see Hall-Petch strengthening).

Microstructure characterizations

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Microstructure of a spiral tube originating from the 12th-13th century cemetery from Kukruse, Estonia. Copper alloy wire containing tin and lead. The spiral was mounted in plastic and ground. Tint etched with the Klemm's II reagent. Photographed with optical microscope under 200x magnification.

To quantify microstructural features, both morphological and material property must be characterized. Image processing is a robust technique for determination of morphological features such as volume fraction,[2] inclusion morphology,[3] void and crystal orientations. To acquire micrographs, optical as well as electron microscopy are commonly used. To determine material property, Nanoindentation is a robust technique for determination of properties in micron and submicron level for which conventional testing are not feasible. Conventional mechanical testing such as tensile testing or dynamic mechanical analysis (DMA) can only return macroscopic properties without any indication of microstructural properties. However, nanoindentation can be used for determination of local microstructural properties of homogeneous as well as heterogeneous materials.[4] Then, these properties can be used to produce various other stochastic models.[5][6][7]

Microstructure generation

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Microstructure generation is also known as stochastic microstructure reconstruction.[8][9] Computer-simulated microstructures are generated to replicate the microstructural features of actual microstructures. Such microstructures are referred to as synthetic microstructures. Synthetic microstructures are used to investigate what microstructural feature is important for a given property. To ensure statistical equivalence between generated and actual microstructures, microstructures are modified after generation to match the statistics of an actual microstructure. Such procedure enables generation of theoretically infinite number of computer simulated microstructures that are statistically the same (have the same statistics) but stochastically different (have different configurations).[3][10]

A computer simulated microstructure of composite materials[3]

Influence of pores and composition

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A pore in a microstructure, unless desired, is a disadvantage for the properties. In fact, in nearly all of the materials, a pore will be the starting point for the rupture of the material. It is the initiation point for the cracks. Furthermore, a pore is usually quite hard to get rid of. Those techniques described later involve a high temperature process. However, even those processes can sometimes make the pore even bigger. Pores with large coordination number (surrounded by many particles) tend to grow during the thermal process. This is caused by the thermal energy being converted to a driving force for the growth of the particles which will induce the growth of the pore as the high coordination number prohibits the growth towards the pore. For many materials, it can be seen from their phase diagram that multiple phases can exist at the same time. Those different phases might exhibit different crystal structure, thus exhibiting different mechanical properties.[11] Furthermore, these different phases also exhibit a different microstructure (grain size, orientation).[12] This can also improve some mechanical properties as crack deflection can occur, thus pushing the ultimate breakdown further as it creates a more tortuous crack path in the coarser microstructure.[13]

Improvement techniques

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In some cases, simply changing the way the material is processed can influence the microstructure. An example is the titanium alloy TiAl6V4.[14] Its microstructure and mechanical properties are enhanced using SLM (selective laser melting) which is a 3D printing technique using powder and melting the particles together using high powered laser.[15] Other conventional techniques for improving the microstructure are thermal processes.[16] Those processes rely in the principle that an increase in temperature will induce the reduction or annihilation of pores.[17] Hot isostatic pressing (HIP) is a manufacturing process, used to reduce the porosity of metals and increase the density of many ceramic materials. This improves the material's mechanical properties and workability.[18] The HIP process exposes the desired material to an isostatic gas pressure as well as high temperature in a sealed vessel (high pressure). The gas used during this process is mostly Argon. The gas needs to be chemically inert so that no reaction occurs between it and the sample. The pressure is achieved by simply applying heat to the hermetically sealed vessel. However, some systems also associate gas pumping to the process to achieve the required pressure level. The pressure applied on the materials is equal and comes from all directions (hence the term "isostatic").[19] When castings are treated with HIP, the simultaneous application of heat and pressure eliminates internal voids and microporosity through a combination of plastic deformation, creep, and diffusion bonding; this process improves fatigue resistance of the component.[20]

See also

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  • Abnormal grain growth – Phenomenon of certain material grains growing faster than others
  • Crystallite – Small crystal which forms under certain conditions
  • Fractography – Study of the fracture surfaces of materials
  • Grain boundary – Interface between crystallites in a polycrystalline material
  • Metallurgy – Field of science that studies the physical and chemical behavior of metals
  • Micrograph – Process for producing pictures with a microscope

References

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  1. ^ "Metallography and Microstructures". ASM Metals Handbook. Vol. 9 (9th ed.). Metals Park, Ohio: American Society for Metals. 1985. p. 12.
  2. ^ Sanei, Seyed Hamid Reza; Fertig, Ray S. (2015). "Uncorrelated volume element for stochastic modeling of microstructures based on local fiber volume fraction variation". Composites Science and Technology. 117: 191–198. doi:10.1016/j.compscitech.2015.06.010.
  3. ^ a b c Sanei, Seyed Hamid Reza; Barsotti, Ercole J.; Leonhardt, David; Fertig, Ray S. (2017). "Characterization, synthetic generation, and statistical equivalence of composite microstructures". Journal of Composite Materials. 51 (13): 1817–1829. Bibcode:2017JCoMa..51.1817S. doi:10.1177/0021998316662133. S2CID 138768783.
  4. ^ Fu, Jinlong; Xiao, Dunhui; Li, Dongfeng; Thomas, Hywel R.; Li, Chenfeng (2022). "Stochastic reconstruction of 3D microstructures from 2D cross-sectional images using machine learning-based characterization". Computer Methods in Applied Mechanics and Engineering. 390 114532. doi:10.1016/j.cma.2021.114532.
  5. ^ Tahmasebi, Pejman (2018-02-20). "Accurate modeling and evaluation of microstructures in complex materials". Physical Review E. 97 (2) 023307. Bibcode:2018PhRvE..97b3307T. doi:10.1103/PhysRevE.97.023307. PMID 29548238.
  6. ^ Tahmasebi, Pejman (2018). "Nanoscale and multiresolution models for shale samples". Fuel. 217: 218–225. Bibcode:2018Fuel..217..218T. doi:10.1016/j.fuel.2017.12.107.
  7. ^ Tahmasebi, Pejman; Sahimi, Muhammad (2018-06-29). "A stochastic multiscale algorithm for modeling complex granular materials". Granular Matter. 20 (3). doi:10.1007/s10035-018-0816-z. ISSN 1434-5021. S2CID 85549903.
  8. ^ Fu, Jinlong; Tan, Wei; Dunhui, Xiao; Xiaoying, Zhuang (2025). "Computational Intelligence in Stochastic Reconstruction of Porous Microstructures for Image-Based Poro/Micro-Mechanical Modeling". Archives of Computational Methods in Engineering. doi:10.1007/s11831-025-10313-9. PMC 12884968.
  9. ^ Fu, Jinlong; Cui, Shaoqing; Cen, Song; Li, Chenfeng (2021). "Statistical characterization and reconstruction of heterogeneous microstructures using deep neural network". Computer Methods in Applied Mechanics and Engineering. 373 113516. doi:10.1016/j.cma.2020.113516.
  10. ^ Tahmasebi, Pejman (2018-02-20). "Accurate modeling and evaluation of microstructures in complex materials". Physical Review E. 97 (2) 023307. Bibcode:2018PhRvE..97b3307T. doi:10.1103/physreve.97.023307. ISSN 2470-0045. PMID 29548238.
  11. ^ Oberwinkler, B., Modeling the fatigue crack growth behavior of Ti-6Al-4V by considering grain size and stress ratio. Materials Science and Engineering: A 2011, 528 (18), 5983-5992.
  12. ^ Sieniawski, J.; Ziaja, W.; Kubiak, K.; Motyka, M., Microstructure and mechanical properties of high strength two-phase titanium alloys. Titanium Alloys-Advances in Properties Control 2013, 69–80.
  13. ^ Nalla, R.; Boyce, B.; Campbell, J.; Peters, J.; Ritchie, R., Influence of microstructure on high-cycle fatigue of Ti-6Al-4V: bimodal vs. lamellar structures. Metallurgical and Materials Transactions A 2002, 33 (13), 899–918.
  14. ^ Henriques, V. A. R.; Campos, P. P. d.; Cairo, C. A. A.; Bressiani, J. C., Production of titanium alloys for advanced aerospace systems by powder metallurgy. Materials Research 2005, 8 (4), 443–446.
  15. ^ Kruth, J.-P.; Mercelis, P.; Van Vaerenbergh, J.; Froyen, L.; Rombouts, M., Binding mechanisms in selective laser sintering and selective laser melting. Rapid prototyping journal 2005, 11 (1), 26–36.
  16. ^ Murr, L.; Quinones, S.; Gaytan, S.; Lopez, M.; Rodela, A.; Martinez, E.; Hernandez, D.; Martinez, E.; Medina, F.; Wicker, R., Microstructure and mechanical behavior of Ti–6Al–4V produced by rapid-layer manufacturing, for biomedical applications. Journal of the mechanical behavior of biomedical materials 2009, 2 (1), 20–32.
  17. ^ Kasperovich, G.; Hausmann, J., Improvement of fatigue resistance and ductility of TiAl6V4 processed by selective laser melting. Journal of Materials Processing Technology 2015, 220, 202–214.
  18. ^ Lin, C. Y.; Wirtz, T.; LaMarca, F.; Hollister, S. J., Structural and mechanical evaluations of a topology optimized titanium interbody fusion cage fabricated by selective laser melting process. Journal of Biomedical Materials Research Part A 2007, 83 (2), 272–279.
  19. ^ Leuders, S.; Thöne, M.; Riemer, A.; Niendorf, T.; Tröster, T.; Richard, H.; Maier, H., On the mechanical behaviour of titanium alloy TiAl6V4 manufactured by selective laser melting: Fatigue resistance and crack growth performance. International Journal of Fatigue 2013, 48, 300–307.
  20. ^ Larker, H. T.; Larker, R., Hot isostatic pressing. Materials Science and Technology 1991.
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Wikipedia

Microstructure

Microstructure is the very small-scale structure of a material, defined as the structure of a prepared surface of material as revealed by an optical microscope above 25× magnification. The microstructure of a material (e.g. metals, polymers, ceramics, or composites) can strongly influence physical properties such as strength, toughness, ductility, hardness, corrosion resistance, high/low temperature behaviour or wear resistance. These properties in turn govern the application of these materials in industrial practice. Microstructure at scales smaller than can be viewed with optical microscopes is often called nanostructure, while the structure in which individual atoms are arranged is known as crystal structure. The nanostructure of biological specimens is referred to as ultrastructure. A microstructure's influence on the mechanical and physical properties of a material is primarily governed by the different defects present or absent of the structure. These defects can take many forms but the primary ones are the pores. Even if those pores play a very important role in the definition of the characteristics of a material, so does its composition. In fact, for many materials, different phases can exist at the same time. These phases have different properties and if managed correctly, can prevent the fracture of the material.

MORE →
Wikipedia

Max Planck Institute of Microstructure Physics

The Max Planck Institute of Microstructure Physics in Halle (Saale) is a research institute in Germany focused on novel materials with useful functionalities. Active research topics includes spintronics, neuromorphic systems, superconductivity, nano-photonics, topological metals and insulators, 2D materials etc. It was founded in 1992 by Hellmut Fischmeister and is a follow-up to the German Academy of Sciences Institute of Solid State Physics and Electron Microscopy. The institute moved into new buildings from 1997 till 1999. It is one of 84 institutes in the Max Planck Society (Max-Planck-Gesellschaft). The institute has three main departments: Prof. Dr. Stuart Parkin: Nano-systems from Ions, Spins and Electrons (NISE) Dr. Wesley David Sacher: Nano-photonics, Integration and Neural Technology (NINT) Prof. Dr. Xinliang Feng: Synthetic Materials and Functional Devices (SMFD) Former departments include the following: The Theory Department, headed by Prof. Eberhard Gross, mainly carries out theoretical research on the electronic, magnetic, optical, and electrical properties of micro- and nanostructured solid-state systems'. The Experimental Department 1, headed by Prof. Jürgen Kirschner, mainly deals with the magnetic properties of dimensionally reduced systems and their dependence on electronic structure, crystalline structure and morphology. The Experimental Department 2, headed by Prof. Ulrich Gösele, is focussed on the scientific understanding, design and fabrication of new materials for information, communication, engineering as well as bio-technological applications. The Experimental Department 3, headed by Prof. Johannes Heydenreich, is focused on analytical methods using high-resolution electronic microscopy.

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Wikipedia

Market microstructure

Market microstructure is a branch of finance concerned with the details of how exchange occurs in markets. While the theory of market microstructure applies to the exchange of real or financial assets, more evidence is available on the microstructure in the financial field due to the availability of transactions data from them. The major thrust of market microstructure research examines the ways in which the working processes of a market affect determinants of transaction costs, prices, quotes, volume, and trading behavior. In the twenty-first century, innovations have allowed an expansion into the study of the impact of market microstructure on the incidence of market abuse, such as insider trading, market manipulation and broker-client conflict.

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Wikipedia

Microstructures in 3D printing

The use of microstructures in 3D printing, where the thickness of each strut scale of tens of microns ranges from 0.2mm to 0.5mm, has the capabilities necessary to change the physical properties of objects (metamaterials) such as: elasticity, resistance, and hardness. In other words, these capabilities allow physical objects to become lighter or more flexible. The pattern has to adhere to geometric constraints (shape regulations), and thickness constraints (minimum thickness control), or can be enforced using optimization methods (microstructure shape and topological optimization). Innovations in this field are being discovered in addition to 3D printers being built and researched with the intent to specialize in building structures needing altered physical properties.

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TOPIC OF THE DAY

Greenwood / Black Wall Street

Before the 1921 destruction of Tulsa’s Greenwood District, Black residents had created a remarkable center of business and community life. The district included stores, professional offices, entertainment venues and homes owned by Black citizens. Understanding Greenwood means learning what was built—not only what was burned.

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TRIVIA QUESTION OF THE DAY

What prosperous Tulsa district became widely known as “Black Wall Street”?

The Greenwood District.