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P= pi(t− x/c)pr(tx/c) (29) 22 WAVES DUE TO INITIAL DISTURBANCES 4 and transmitted waves in the branches are p1(t−x/c1) and p2(t−x/c2) At the junction x= 0 we expect the continuity of pressure and fluxes, hence pi(t)pr(t)=p1(t)=p2(t) (210) pi − pr Z = p1 Z1 p2 Z2 (211) Define the reflection coefficient Rto be the amplitude ratio of reflected wave to incident wave, then Rß b { y R t S Z s s d ) x z ë ç Ñ æ ï § æ ¢ Ü q ` o z è × Ô s p K { n Î Î åV g E l E t i I X j P X V P Disc 1 1Directions 2Honky Tonk 3What I Say 4Sanctuary Disc 2 1It's About That Time 2Yersternow 3Funky Tonk 4Sanctuary Disc 3(DVD P ԂQ P ) ̏ i ̓l R X ւ̎g p ͏o ܂ B


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< = >?) (& # @!, ' % A & ) 0 / & # 0 % @ & $) (' $/;How do you find the log decrement and how is it related to the damping ratio?RYTY 2r TXTY r TXTX (28) = 1 n 0 2XTY 2XTX (29) = 2 n XTX XTY (30) We now set this to zero at the optimum, b XTX b XTY = 0 (31) This equation, for the twodimensional vector b, corresponds to our pair of normal or estimating equations for b 0 and b 1 Thus, it, too, is called an estimating equation Solving, we get b= (XTX) 1XTY (32)


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