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3 giorni fa · The Feynman Lectures on Physics including Feynman's Tips on Physics: The Definitive and Extended Edition (2nd edition, 2005) The Feynman Lectures on Physics is perhaps his most accessible work for anyone with an interest in physics, compiled from lectures to Caltech undergraduates in 1961–1964.
4 giorni fa · Feynman delivered his seminal lecture “Simulating physics with computers” at the Physics of Computation Conference at the MITEndicott House in May of 1981. The content of his lecture was later published by the International Journal of Theoretical Physics in 1982 [ 1 ]. Nowadays, Feynman’s 1982 paper is properly regarded as one of the most ...
21 apr 2024 · Die Feynman-Vorlesungen über Physik (Originaltitel englisch The Feynman Lectures on Physics) sind eine 1964 bei Addison-Wesley erschienene Sammlung von Vorlesungen, die der spätere Nobelpreisträger Richard Feynman von 1961 bis 1963 (mit einer kurzen „Reprise“ 1964) am California Institute of Technology (Caltech) für Studenten ...
2 mag 2024 · In theoretical physics, a Feynman diagram is a pictorial representation of the mathematical expressions describing the behavior and interaction of subatomic particles. The scheme is named after American physicist Richard Feynman, who introduced the diagrams in 1948.
3 mag 2024 · While Six Easy Pieces is probably the best introduction to physics à la Feynman, the free audio of his lectures is there for those who want more. These free recordings are taken from his physics lectures at Caltech, the material from which Six Easy Pieces was pulled.
29 apr 2024 · Feynman Lectures on Computation: Anniversary Edition. 2nd Edition. Edited By Tony Hey. May 18, 2023. The last lecture course that Nobel Prize winner Richard P. Feynman gave to students at Caltech from 1983 to 1986 was not on physics but on computer science.
2 mag 2024 · Quantum mechanics. The path integral formulation is a description in quantum mechanics that generalizes the stationary action principle of classical mechanics. It replaces the classical notion of a single, unique classical trajectory for a system with a sum, or functional integral, over an infinity of quantum-mechanically possible trajectories ...
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