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Views | Duration | ||
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61. A paper on the orbits in a cyclotron | 386 | 04:18 | |
62. The synchrocyclotron and the betatron | 372 | 02:20 | |
63. The discovery of positrons | 492 | 03:49 | |
64. My interest in the limits of quantum electrodynamics | 567 | 01:32 | |
65. A paper with Arthur Compton on cosmic radiation | 408 | 02:03 | |
66. The Bethe-Heitler Formula | 563 | 00:29 | |
67. Yukawa's meson prediction | 458 | 03:01 | |
68. Being recommended Emil Konopinski | 400 | 02:21 | |
69. My postdoc students at Cornell | 556 | 01:53 | |
70. How the Sun is radiating? | 1 | 528 | 04:16 |
In 1938 Teller and Gamow decided to do astrophysics rather than plain theoretical physics, and I was really not interested in that, and I said I would skip this conference. But Teller persuaded me to come and it turned out to be very interesting. I had known Eddington's theory of the interior of the sun, and I had known that he predicted the temperature at the center of the sun to be 40 million degrees. Well I should probably mention first one thing that preceded that conference, namely Gamow had proposed his graduate student Critchfield to do something about the energy in the sun. And Critchfield found the suggestion by von Weizsäcker in Germany that maybe two protons could get together to form a deuteron with the emission of a positron and a neutrino. But neither [von] Weizsäcker nor Gamow thought much of this process. But Critchfield decided he'd do it anyway, and he started calculating it and it came out pretty well. So then Gamow told him 'Now really you should get together with somebody who really knows about the deuteron, namely Hans Bethe.' And Critchfield showed me... sent me his calculations, which looked quite good and I could somewhat make his calculations of the deuteron a bit more elegant, and so reduced the number of assumptions which he had put in. And so we wrote a paper together, making energy at the center of the sun by this reaction. Now this is quite a miracle because anything involving emission of electrons, positive or negative, is an extremely slow process. Beta decay of nuclei takes seconds or hours or days or years, whereas nuclear processes in general take something like 10-22 seconds, maybe as long as 10-20 seconds. And of course Fermi had explained that by his theory of beta decay and so the interaction, the weak interaction which makes beta decay is really just what it says, exceedingly weak. And so it is rather a miracle that such a weak interaction can give you enough energy to keep the sun radiating all the time.
The late German-American physicist Hans Bethe once described himself as the H-bomb's midwife. He left Nazi Germany in 1933, after which he helped develop the first atomic bomb, won the Nobel Prize in Physics in 1967 for his contribution to the theory of nuclear reactions, advocated tighter controls over nuclear weapons and campaigned vigorously for the peaceful use of nuclear energy.
Title: How the Sun is radiating?
Listeners: Sam Schweber
Silvan Sam Schweber is the Koret Professor of the History of Ideas and Professor of Physics at Brandeis University, and a Faculty Associate in the Department of the History of Science at Harvard University. He is the author of a history of the development of quantum electro mechanics, "QED and the men who made it", and has recently completed a biography of Hans Bethe and the history of nuclear weapons development, "In the Shadow of the Bomb: Oppenheimer, Bethe, and the Moral Responsibility of the Scientist" (Princeton University Press, 2000).
Tags: Edward Teller, George Gamow, Arthur Eddington, Charles Critchfield, Carl von Weizsäcker
Duration: 4 minutes, 16 seconds
Date story recorded: December 1996
Date story went live: 24 January 2008