5. For the overdamped oscillations, the displacement x(t) is expressed by the following x(t)-e-t [A et + Bet]. The displacement can be expressed in terms of hyperbolic functions as the following: Hint: Use the following relations e = coshy+sinhy e = coshy-sinhy A. x(t) = (cosh Bt-sin ßt) [(A + B) cosh wt- (A-B) sinh wt] B. C. x(t) = (cosh Bt+ sin ßt)[(A + B) cosh at + (A-B) sinhot] x(t) = (cosh ßt -sin ßt) [(A-B) cosh wt+ (A-B) sinh wt] x(t) = (cosh ßt - sin ßt) [(A + B) cosh wt+ (A-B) sinh wt] D.

5. For the overdamped oscillations, the displacement x(t) is expressed by the following x(t)-e-t [A et + Bet]. The displacement can be expressed in terms of hyperbolic functions as the following: Hint: Use the following relations e = coshy+sinhy e = coshy-sinhy A. x(t) = (cosh Bt-sin ßt) [(A + B) cosh wt- (A-B) sinh wt] B. C. x(t) = (cosh Bt+ sin ßt)[(A + B) cosh at + (A-B) sinhot] x(t) = (cosh ßt -sin ßt) [(A-B) cosh wt+ (A-B) sinh wt] x(t) = (cosh ßt - sin ßt) [(A + B) cosh wt+ (A-B) sinh wt] D.

Elements Of Electromagnetics

7th Edition

ISBN:9780190698614

Author:Sadiku, Matthew N. O.

Publisher:Sadiku, Matthew N. O.

ChapterMA: Math Assessment

Section: Chapter Questions

Problem 1.1MA

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