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Unformatted text preview: ) , where F 1 ( t ) is the driving force from part (a). Then, by superposition, we can write the solution as x 1 ( t )x 1 ( t ) , where x 1 ( t ) is the solution of part (a). (c) From the solution to (b), take the limit and such that = a = constant, and show that the resulting x ( t ) agrees with M&T Eqn. 3.105 with t = 0 ....
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This note was uploaded on 10/06/2011 for the course PHYS 325 taught by Professor Staff during the Spring '08 term at University of Illinois, Urbana Champaign.
 Spring '08
 Staff
 Physics, mechanics

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