Ernest Orlando Lawrence was an American nuclear physicist and winner of the Nobel Prize in Physics in 1939 for his invention of the cyclotron, being the youngest winner of the Nobel Prize in Physics. He is known for his work on uranium-isotope separation for the Manhattan Project, as well as for founding the Lawrence Berkeley National Laboratory and the Lawrence Livermore National Laboratory.
Lawrence in 1939
Meeting at Berkeley in 1940 concerning the planned 184-inch (4.67 m) cyclotron (seen on the blackboard): Lawrence, Arthur Compton, Vannevar Bush, James B. Conant, Karl T. Compton, and Alfred Lee Loomis
The 60-inch (1.52 m) cyclotron soon after completion in 1939. The key figures in its development and use are shown, standing, left to right: Donald Cooksey, Dale R. Corson, Ernest Lawrence, Robert L. Thornton, John Backus, and Winfield Salisbury. In the background are Luis Alvarez and Edwin McMillan.
University of California Radiation Laboratory staff framed by the magnet for the 60-inch cyclotron, 1938; Nobel prize winners Ernest Lawrence, Edwin McMillan, and Luis Alvarez are shown, in addition to J. Robert Oppenheimer and Robert R. Wilson.
A cyclotron is a type of particle accelerator invented by Ernest Lawrence in 1929–1930 at the University of California, Berkeley, and patented in 1932. A cyclotron accelerates charged particles outwards from the center of a flat cylindrical vacuum chamber along a spiral path. The particles are held to a spiral trajectory by a static magnetic field and accelerated by a rapidly varying electric field. Lawrence was awarded the 1939 Nobel Prize in Physics for this invention.
Lawrence's 60-inch (152 cm) cyclotron, c. 1939, showing the beam of accelerated ions (likely protons or deuterons) exiting the machine and ionizing the surrounding air causing a blue glow
Lawrence's original 4.5-inch (11 cm) cyclotron
The magnet yoke for the 37-inch (94 cm) cyclotron on the grounds of the Lawrence Hall of Science, Berkeley, California
Vacuum chamber of Lawrence 69 cm (27 in) 1932 cyclotron with cover removed, showing the dees. The 13,000 V RF accelerating potential at about 27 MHz is applied to the dees by the two feedlines visible at top right. The beam emerges from the dees and strikes the target in the chamber at bottom.