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tibphysic
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1.10.1 The force field acting on a two-dimensional linear oscillator may be described by
F=−ˆxkx − ˆyky.
Compare the work done moving against this force field when going from (1, 1) to (4, 4)
by the following straight-line paths:
(a) (1, 1)→(4, 1)→(4, 4)
(b) (1, 1)→(1, 4)→(4, 4)
(c) (1, 1)→(4, 4) along x = y.
This means evaluating
−
(4,4)
(1,1)
F · dr
along each path.
F=−ˆxkx − ˆyky.
Compare the work done moving against this force field when going from (1, 1) to (4, 4)
by the following straight-line paths:
(a) (1, 1)→(4, 1)→(4, 4)
(b) (1, 1)→(1, 4)→(4, 4)
(c) (1, 1)→(4, 4) along x = y.
This means evaluating
−
(4,4)
(1,1)
F · dr
along each path.