Classical Dynamics of Particles and Systems
Classical Dynamics of Particles and Systems
5th Edition
ISBN: 9780534408961
Author: Stephen T. Thornton, Jerry B. Marion
Publisher: Cengage Learning
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Chapter 1, Problem 1.20P

Show that

  1. (a) i , j ε i j k δ i j = 0
  2. (b) i , k ε i j k ε l j k = 2 δ i l
  3. (c) i , j , k ε i j k ε l j k = 6
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Why is (j + k) = i?I see that i x i = 0, that makes sense. But I thought that j x k = i? not j + k.
solve for letter b, options are: a. 1.93 N/C and 6.43 x 10^-9 T b. 1.54 N/C and 5.13 x 10^-9 T c. 1.09 N/C and 3.63 x 10^-9 T d. 2.18 N/C and 7.25 x 10^-9 T
Show that the power law relationship P(Q) = kQr, for Q > 0 and r # 0, has an inverse that is also a power law, Q(P) = mP s, where m = k - l/r and s = 1/ r.

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Classical Dynamics of Particles and Systems

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Length contraction: the real explanation; Author: Fermilab;https://www.youtube.com/watch?v=-Poz_95_0RA;License: Standard YouTube License, CC-BY