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Now let’s view the same two events from the point of view of another frame, S. As shown below, the S’-frame is moving to the right with speed v relative to the S-frame. In the S-frame, x 0 . ∆ ≠ 2 d The elapsed time is t , where d 2 d 2 2 . Substitute for ∆ = c = ′ +. d , d , and in terms of. ′ ∆. c 2 t 2.
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the laws of physics are invariant to observers in different inertial reference frames; that is, if you and I are conducting observations and experiments and moving relative to one another at constant velocity, the laws of physics governing the outcomes are not affected and the
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Lecture Notes on Modern Physics (Phys.323) (Fall, 2011) Masatsugu Sei Suzuki Department of Physics, State University of New York at Binghamton Binghamton, New York 13902-6000 (Date: January, 25, 2012) taught the Phys.323 (Modern Physics) in Fall 2011.
PHYSICS 342 Modern Physics. Lecture Notes. (These are all handwritten notes scanned as .PDF files.)
inspired new developments and theories in the Þelds of atomic physics, nuclear physics, and condensed-matter physics. In Chapter 3 9 we introduce the special theory of relativity . The theory provides us with a new and deeper view of physical laws. Although the concepts underlying this
Lecture Notes on Modern Physics I taught the Phys.323 (Modern Physics) in Fall 2011. This course is usually taught for students who just have finished the Phys.131 and 132 (Introductory Physics) in the SUNY at Binghamton.
Modern Physics: (relativistic quantum field theory) • established during 1900-1920! • exotic and counter-intuitive! • now common place in all modern technology, e.g.,! GPS, electronics (cell phones, iPods, laptops…), and! throughout science, e.g., physics, chemistry, astronomy,… ! Course overview
