Alan Needleman

Last updated
Alan Needleman
Alma mater Harvard University
Awards
Academic career
Institutions
Doctoral advisor John W. Hutchinson
Doctoral studentsNicolas Triantafyllidis

Alan Needleman (born September 2, 1944) is a professor of materials science & engineering at Texas A&M University. [1] Prior to 2009, he was Florence Pirce Grant University Professor of Mechanics of Solids and Structures at Brown University in Providence, Rhode Island.

Contents

Early life and education

Needleman received his B.S. from the University of Pennsylvania in 1966, an M.S. and Ph.D. from Harvard University in 1967 and 1970 [2] respectively, advised by John W. Hutchinson.

Research and career

He was an instructor and assistant professor in the Department of Applied Mathematics at the Massachusetts Institute of Technology from 1970 to 1975. He was a professor of engineering at Brown University starting in 1975, and served as the dean of the Engineering Department from 1988 to 1991. He was the chair of the Applied Mechanics Division.

Needleman's main research interests are in the computational modeling of deformation and fracture processes in structural materials, in particular metals. A general objective is to provide quantitative relations between the measurable (and hopefully controllable) features of the materials' micro-scale structure and its macroscopic mechanical behavior. Ongoing research projects involve studies of ductile fracture and ductile-brittle transitions; crack growth in heterogeneous microstructures with particular emphasis on the role of interfaces; nonlocal and discrete dislocation plasticity; fatigue crack growth; and fast fracture in brittle solids.

Professor Needleman often collaborates with Viggo Tvergaard, John Hutchinson, Subra Suresh, and Erik van der Giessen among others in both materials science and mechanics.

Awards and honors

Needleman is a member of the National Academy of Engineering, a fellow of the American Society of Mechanical Engineers, a fellow of the American Academy of Mechanics, an honorary member of MECAMAT (Groupe Français de Mecanique des Matériaux) and a foreign member of the Danish Center for Applied Mathematics and Mechanics. He has been recognized by Institute for Scientific Information (ISI) Science Citation Index as a highly cited author both in engineering and in materials science. In 1994, his work on 3D modeling of metallic fracture was a finalist in the Science Category for the Computerworld-Smithsonian Award. In 2006 he was the recipient of both the William Prager Medal and the Drucker Medal and received an Honorary Doctorate from Technical University of Denmark (DTU). He is also the recipient of Timoshenko Medal in 2011.

Selected publications

Related Research Articles

<span class="mw-page-title-main">Ductility</span> Degree to which a material under stress irreversibly deforms before failure

Ductility is a mechanical property commonly described as a material's amenability to drawing. In materials science, ductility is defined by the degree to which a material can sustain plastic deformation under tensile stress before failure. Ductility is an important consideration in engineering and manufacturing. It defines a material's suitability for certain manufacturing operations and its capacity to absorb mechanical overload. Some metals that are generally described as ductile include gold and copper, while platinum is the most ductile of all metals in pure form. However, not all metals experience ductile failure as some can be characterized with brittle failure like cast iron. Polymers generally can be viewed as ductile materials as they typically allow for plastic deformation.

<span class="mw-page-title-main">Fracture</span> Split of materials or structures under stress

Fracture is the separation of an object or material into two or more pieces under the action of stress. The fracture of a solid usually occurs due to the development of certain displacement discontinuity surfaces within the solid. If a displacement develops perpendicular to the surface, it is called a normal tensile crack or simply a crack; if a displacement develops tangentially, it is called a shear crack, slip band or dislocation.

<span class="mw-page-title-main">Fracture mechanics</span> Study of propagation of cracks in materials

Fracture mechanics is the field of mechanics concerned with the study of the propagation of cracks in materials. It uses methods of analytical solid mechanics to calculate the driving force on a crack and those of experimental solid mechanics to characterize the material's resistance to fracture.

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

In materials science, fracture toughness is the critical stress intensity factor of a sharp crack where propagation of the crack suddenly becomes rapid and unlimited. A component's thickness affects the constraint conditions at the tip of a crack with thin components having plane stress conditions and thick components having plane strain conditions. Plane strain conditions give the lowest fracture toughness value which is a material property. The critical value of stress intensity factor in mode I loading measured under plane strain conditions is known as the plane strain fracture toughness, denoted . When a test fails to meet the thickness and other test requirements that are in place to ensure plane strain conditions, the fracture toughness value produced is given the designation . Fracture toughness is a quantitative way of expressing a material's resistance to crack propagation and standard values for a given material are generally available.

Liquid metal embrittlement is a phenomenon of practical importance, where certain ductile metals experience drastic loss in tensile ductility or undergo brittle fracture when exposed to specific liquid metals. Generally, a tensile stress, either externally applied or internally present, is needed to induce embrittlement. Exceptions to this rule have been observed, as in the case of aluminium in the presence of liquid gallium. This phenomenon has been studied since the beginning of the 20th century. Many of its phenomenological characteristics are known and several mechanisms have been proposed to explain it. The practical significance of liquid metal embrittlement is revealed by the observation that several steels experience ductility losses and cracking during hot-dip galvanizing or during subsequent fabrication. Cracking can occur catastrophically and very high crack growth rates have been measured.

The J-integral represents a way to calculate the strain energy release rate, or work (energy) per unit fracture surface area, in a material. The theoretical concept of J-integral was developed in 1967 by G. P. Cherepanov and independently in 1968 by James R. Rice, who showed that an energetic contour path integral was independent of the path around a crack.

John W. Hutchinson is the Abbott and James Lawrence Research Professor of Engineering in the School of Engineering and Applied Sciences at Harvard University. He works in the field of solid mechanics concerned with a broad range of problems in structures and engineering materials.

George Rankin Irwin was an American scientist in the field of fracture mechanics and strength of materials. He was internationally known for his study of fracture of materials.

<span class="mw-page-title-main">Shear band</span>

A shear band is a narrow zone of intense shearing strain, usually of plastic nature, developing during severe deformation of ductile materials. As an example, a soil specimen is shown in Fig. 1, after an axialsymmetric compression test. Initially the sample was cylindrical in shape and, since symmetry was tried to be preserved during the test, the cylindrical shape was maintained for a while during the test and the deformation was homogeneous, but at extreme loading two X-shaped shear bands had formed and the subsequent deformation was strongly localized.

<span class="mw-page-title-main">Zdeněk P. Bažant</span>

Zdeněk Pavel Bažant is McCormick School Professor and Walter P. Murphy Professor of Civil Engineering and Materials Science in the Department of Civil and Environmental Engineering at Northwestern University's Robert R. McCormick School of Engineering and Applied Science.

Material failure theory is an interdisciplinary field of materials science and solid mechanics which attempts to predict the conditions under which solid materials fail under the action of external loads. The failure of a material is usually classified into brittle failure (fracture) or ductile failure (yield). Depending on the conditions most materials can fail in a brittle or ductile manner or both. However, for most practical situations, a material may be classified as either brittle or ductile.

James Robert Rice is an American engineer, scientist, geophysicist, and Mallinckrodt Professor of Engineering Sciences and Geophysics at the Harvard John A. Paulson School of Engineering and Applied Sciences,.

In materials modeled by linear elastic fracture mechanics (LEFM), crack extension occurs when the applied energy release rate exceeds , where is the material's resistance to crack extension.

Ramarathnam Narasimhan is an Indian materials engineer and a professor at the Department of Mechanical Engineering of the Indian Institute of Science. He is known for his pioneering researches on fracture mechanics and is an elected fellow of the Indian Academy of Sciences, Indian National Science Academy and the Indian National Academy of Engineering. The Council of Scientific and Industrial Research, the apex agency of the Government of India for scientific research, awarded him the Shanti Swarup Bhatnagar Prize for Science and Technology, one of the highest Indian science awards for his contributions to Engineering Sciences in 1999.

In materials science, toughening refers to the process of making a material more resistant to the propagation of cracks. When a crack propagates, the associated irreversible work in different materials classes is different. Thus, the most effective toughening mechanisms differ among different materials classes. The crack tip plasticity is important in toughening of metals and long-chain polymers. Ceramics have limited crack tip plasticity and primarily rely on different toughening mechanisms.

<span class="mw-page-title-main">Robert O. Ritchie</span> American professor of engineering

Robert Oliver Ritchie is the H.T. and Jessie Chua Distinguished Professor of Engineering at the University of California, Berkeley and Senior Faculty Scientist at the Lawrence Berkeley National Laboratory.

<span class="mw-page-title-main">Striation (fatigue)</span>

Striations are marks produced on the fracture surface that show the incremental growth of a fatigue crack. A striation marks the position of the crack tip at the time it was made. The term striation generally refers to ductile striations which are rounded bands on the fracture surface separated by depressions or fissures and can have the same appearance on both sides of the mating surfaces of the fatigue crack. Although some research has suggested that many loading cycles are required to form a single striation, it is now generally thought that each striation is the result of a single loading cycle.

<span class="mw-page-title-main">Katherine Faber</span> Professor of Materials Science

Katherine T. Faber is an American materials scientist and one of the world's foremost experts in material strengthening, ceramic engineering, and mechanical behavior. Faber is the Simon Ramo Professor of Materials Science at the California Institute of Technology (Caltech). Currently, Faber is the faculty representative for the Materials Science option at Caltech. She is also an adjunct professor of Materials Science and Engineering at the McCormick School of Engineering and Applied Science at Northwestern University.

Jean-Baptiste Leblond, born on 21 May 1957 in Boulogne-Billancourt, is a materials scientist, member of the Mechanical Modelling Laboratory of the Pierre-et-Marie-Curie University (MISES) and professor at the same university.

<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

  1. "Professor Needleman's web page". Archived from the original on September 2, 2006. Retrieved January 31, 2021.
  2. "ALAN NEEDLEMAN; Class of 2012-13". hias.tamu.edu. Retrieved January 31, 2021.