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Recompute the coupled mass–spring oscillator motion in Problem 1, Exercises 5.6 (page 287), using Laplace transforms.

Short Answer

Expert verified

x(t)=−817cost−917cos203ty(t)=−617cost+617cos203t

Step by step solution

01

Step 1:Given Information

The differential equation of a coupled mass spring oscillator is

{x''+4x−4y=0,x(0)=−1,x'(0)=03y''−6x+11y=0y(0)=0,y'(0)=0

02

Determining the coupled mass–spring oscillator motion

The mechanism in Exercises 5.6 Problem 1 is

{x''+4x−4y=0,x(0)=−1,x'(0)=03y''−6x+11y=0y(0)=0,y'(0)=0

Using the Laplace transform, we can obtain

{L{x"+4x-4y}=0L{3y"-6x+11y}=0

⇒{s2X(s)−sx(0)−x'(0)+4X(s)−4Y(s)=03[s2Y(s)−sy(0)−y'(0)]−6X(s)+11Y(s)=0

⇒{s2X(s)+s+4X(s)−4Y(s)=03s2Y(s)−6X(s)+11Y(s)=0

⇒{(s2+4)X(s)−4Y(s)=−s(3s2+11)Y(s)−6X(s)=0

⇒{X(s)=4s2+1Y(s)−ss2+1(3s2+11)Y(s)−6X(s)=0

We now have

(3s2+11)Y(s)−6(4s2+1Y(s)−ss2+1)=0(3s2+11)Y(s)−24s2+1Y(s)+6ss2+1=0(3s2+11−24s2+1)Y(s)=−6ss2+1(3s2+11)(s2+1)−24s2+1Y(s)=−6ss2+1(3s4+23s2+20)Y(s)=6sY(s)=−6s3s4+23s2+20

We can get partial fractions by using partial fractions.

Y(s)=−6s17(s2+1)+6s17(s2+203)

As a result, if we use the inverse Laplace, we get

y(t)=−617cost+617cos203t

We now have X(s):

(3s2+11)(−6s)3s4+23s2+20−6X(s)=0X(s)=−s(3s2+11)(s2+1)(s2+203)

We can get partial fractions by using partial fractions.

X(s)=−8s17(s2+1)−9s17(s2+203)

As a result, if we use the inverse Laplace, we get

x(t)=−817cost−917cos203t

03

Determining the Result

The solution is obtained as:

x(t)=−817cost−917cos203t

y(t)=−617cost+617cos203t

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