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John M. Dawson

John M. Dawson is a physics topic covered in the lgStudy science library. This page brings together a partial reference excerpt, illustrations, worked examples, real-world applications and a short study plan, so you can understand John M. Dawson rather than just read about it. In short: John Myrick Dawson (30 September 1930 in Champaign, Illinois – 17 November 2001 in Los Angeles) was an American computational physicist and the father of plasma-based acceleration techniques. Dawson earned his degrees in physics from the University of Maryland, College Park: a B.S. in 1952 and Ph.D. in 1957.

Key takeaways

  • John M. Dawson belongs to physics; place it in that map before memorising details.
  • Learn the definition first, then one example that makes the definition concrete.
  • Connect John M. Dawson to a quantity you can measure, compute or draw — that is where exam questions come from.
  • Reproduce the core statement of John M. Dawson from memory before moving on to harder problems.

Reference excerpt

John Myrick Dawson (30 September 1930 in Champaign, Illinois – 17 November 2001 in Los Angeles) was an American computational physicist and the father of plasma-based acceleration techniques. Dawson earned his degrees in physics from the University of Maryland, College Park: a B.S. in 1952 and Ph.D. in 1957. His thesis "Distortion of Atoms and Molecules in Dense Media" was prepared under the guidance of Zaka Slawsky. On graduation, John joined the Princeton Plasma Physics Laboratory (a.k.a. Project Matterhorn). Initially a research physicist, he rose to head the theoretical group from 1966 to 1973. He also spent two years (1969–71) at the Naval Research Laboratory in Washington, D.C., where he started a plasma simulation group. He then joined UCLA in 1973 as a professor of physics. He served as director of UCLA's Center for Plasma Physics and Fusion Engineering from 1976 to 1987. He was associate director of the Institute for Plasma and Fusion Research from 1989 to 1991, principal scientist with the institute since 1989 and the institute's interim director. John was a leading figure in the plasma physics community for more than four decades, with his contributions to science spanning all of plasma physics. He performed seminal work on magnetic fusion, inertial confinement fusion, space plasmas, plasma astrophysics, free-electron lasers, and basic plasma physics. He also proposed numerous controlled-fusion concepts. A visionary, he realized as early as the late 1950s the potential impact of simulations as a way to test both theories and large construction projects before they were built. He used simulations in 1959 to answer such fundamental questions as how large can a plasma wave become before breaking. During the late 1970s and 1980s, John was using simulations to test out new ideas such as plasma-based acceleration. By the 1990s, he was realizing his broader vision for simulations in such projects as the Numerical Tokamak. In the late 1970s and 1980s, while at UCLA, John pioneered the field of plasma-based acceleration. He proposed letting particles surf on the plasma-wave wakes left behind by a laser or a particle beam as it moved through plasma. The fields in these wakes can be more than 1000 times higher than in conventional accelerators. A true humanitarian, Dawson believed that science was still the most noble of professions. He believed strongly in the importance of controlled nuclear-fusion research and was particularly proud of his invention of an isotope separation process that was used to detect cancer and, consequently, help save many lives. John had successfully overcome life-threatening illnesses several times. Shortly before his death, he had been in improving health and had enjoyed attending APS's division of plasma physics meeting in Long Beach, California.

Honours and awards Dawson received the James Clerk Maxwell Prize for Plasma Physics in 1977 and the Aneesur Rahman Prize for Computational Physics in 1994; both are the highest honors bestowed by the American Physical Society's plasma physics and computational physics divisions, respectively. He was named California Scientist of the Year by the California Science Center in 1978. The Rahman prize is the highest honor given by the American Physical Society for work in computational physics. He was a member of the National Academy of Sciences, and a recipient of the California Scientist of the Year award, a Fulbright Fellowship, and two UCLA physics teaching awards.

James Clerk Maxwell Prize for Plasma Physics (1977) citation "For his outstanding contributions to plasma physics and controlled fusion as both as innovative theorist and a prolific inventor, whose ideas have provided the basis for several current fusion configurations. He initiated the use of computer simulation as a new and powerful tool for the study of plasmas. He inspired and trained a cadre of younger theorists to continue the development of the field he initiated." Aneesur Rahman Prize (1994) citation "In recognition of his leading role in opening the field of computer simulation of plasmas and for numerous major contributions made using plasma simulation as a complement to analytic theory and experiment. He has led in opening the field of plasma-based accelerators and made major advances in understanding basic nonlinear plasma wave processes, anomalous absorption and transport, advanced plasma-based coherent light sources and space plasma phenomena." In 2007, the American Physical Society renamed its Award for Excellence in Plasma Physics in honor of John Dawson.

Notes

References Tajima, T.; Dawson, J. M. (1979-07-23). "Laser Electron Accelerator". Physical Review Letters. 43 (4): 267–270. doi:10.1103/PhysRevLett.43.267. ISSN 0031-9007. Rosenzweig, J. B.; Cline, D. B.; Cole, B.; Figueroa, H.; Gai, W.; Konecny, R.; Norem, J.; Schoessow, P.; Simpson, J. (1988-07-04). "Experimental Observation of Plasma Wake-Field Acceleration". Physical Review Letters. 61 (1): 98–101. doi:10.1103/PhysRevLett.61.98. ISSN 0031-9007. C. Joshi, "Plasma Accelerators," Scientific American (February 2006), 294, 40-47 Katsouleas, Thomas (2004). "Electrons hang ten on laser wake". Nature. 431 (7008): 515–516. doi:10.1038/431515a. ISSN 0028-0836.

External links JOHN M. DAWSON, PhD Virtual Memorial Garden

Worked examples

Example 1 — a first encounter with John M. Dawson

Start with the simplest possible case. Write down what John M. Dawson claims or describes in one sentence, then invent the smallest concrete situation in which that sentence is true. In physics, the smallest case is usually a single object, a single equation or a single measurement. Check that every symbol or term in your sentence has a meaning in that case.

Example 2 — changing one variable

Take the situation from Example 1 and change exactly one quantity: double it, halve it, or set it to zero. Predict what should happen to John M. Dawson before you calculate. Comparing your prediction with the result is the fastest way to find out whether you understand the idea or only the words.

Example 3 — an exam-style question

Typical questions about John M. Dawson ask you to (a) state it precisely, (b) apply it to given data, and (c) explain a limitation. Practise writing all three answers in under five minutes; the third part is what separates a full-mark answer from an average one.

Applications of John M. Dawson

In research
John M. Dawson appears in physics research whenever the underlying quantities have to be modelled precisely. Papers usually cite it as a starting assumption and then explore where it breaks down.
In technology and industry
Engineering practice reuses John M. Dawson in design rules, simulations and safety margins. Knowing the idea lets you read a specification sheet and understand why the numbers look the way they do.
In the classroom
John M. Dawson is common in secondary-school and first-year university syllabi. It links to neighbouring topics 1930 births, 2001 deaths, 20th-century American physicists, so understanding it makes those chapters shorter.
In everyday life
Look for John M. Dawson outside the textbook — in sport, cooking, traffic, electronics or the sky above you. An example you found yourself is remembered far longer than one you were given.
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How to study John M. Dawson in 20 minutes

  1. Read the reference excerpt below once, without taking notes.
  2. Close the page and write down what John M. Dawson means in your own words.
  3. Compare your version with the excerpt and mark what you missed.
  4. Work through the three examples above with pen and paper.
  5. Explain John M. Dawson out loud to somebody else — or to Teacher Smith in the lgStudy chat.

Frequently asked questions

What is John M. Dawson in simple terms?

John Myrick Dawson (30 September 1930 in Champaign, Illinois – 17 November 2001 in Los Angeles) was an American computational physicist and the father of plasma-based acceleration techniques. Dawson earned his degrees in physics from the University of Maryland, College Park: a B.S. in 1952 and Ph.D…

Why does John M. Dawson matter?

Because it connects several physics ideas at once: it gives you a definition you can apply, a quantity you can calculate, and a way to check whether a result is plausible.

How should I study John M. Dawson?

Read the excerpt, restate it from memory, then work through the examples and applications listed on this page. The five-step study plan above takes about twenty minutes.

What does this page cover?

It gives you a compact reference excerpt plus original lgStudy explanations, examples, applications and study material on John M. Dawson.

Tags

  • 1930 births
  • 2001 deaths
  • 20th-century American physicists
  • Accelerator physicists
  • American computational physicists
  • Fellows of the American Physical Society
  • Members of the United States National Academy of Sciences
  • Princeton University staff
  • University of Maryland, College Park alumni

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