Laplace transform to solve the initial-value problem y"+4y=sin(t)U(t-2*pi), y(0)=1, y'(0)=0? (2024)

Question:

Laplace transform to solve the initial-value problem y"+4y=sin(t)U(t-2*pi), y(0)=1, y'(0)=0?

2013-05-19 03:17:43 UTC

Laplace transform to solve the initial-value problem y"+4y=sin(t)U(t-2*pi), y(0)=1, y'(0)=0?

Three answers:

You have:

y" + 4y = sin(t)*u(t - 2*π), with y(0)=1, y'(0)=0

If F(s) is the Laplace transform of f(t), then the "time-shift" property of the Laplace transform says that the Laplace transform of f(t - a)*u(t-a) = exp(-a*s)*F(s).

Your differential equation has the nono-hom*ogeneous term, sin(t)*u(t-2*π), which is not quite in the format we need to apply the time-shift property. Note, however, that sin(t) = sin(t + n*π), where n = 0, ±1, ±2, ±3...., so we can rewrite your differential equation as :

y" + 4y = sin(t - 2*π)*u(t - 2*π)

Now take the Laplace transform (using a table of transforms), letting Y(s) be the transform of y(t):

(s^2)*Y(s) - s*y(0) - y'(0) + 4*Y(s) = exp(-2π*s)*(1/(s^2 + 1))

Plug in the initial values: and simplify:

Y(s)*(s^2 + 4) - s = exp(-2π*s)*(1/(s^2 + 1))

Y(s) = exp(-2π*s)*(1/(s^2 + 4))*(1/(s^2 + 1)) + s/(s^2 + 4)

Y(s) = (1/3)*exp(-2π*s)*[1/(s^2 + 1) - 1/(s^2 + 4)] + s/(s^2 + 4)

Now take the inverse transform, again using the time-shift property:

y(t) = (1/3)*u(t - 2π)*[sin(t) - (1/2)*sin(2t)] + (1/2)*cos(2t)

Ian H

2013-05-19 09:49:16 UTC

Only partial help, but it might get you started.

Solving the left side is equivalent to finding the complementary function

L[y''(t) + 4y(t)] = s^2 Y - sy(0) - y'(0) + 4Y

substituting y(0) = 1 anf y'(0) = 0 and IF RHS was zero, (it is not), you would have

(s^2 + 4)Y - s = 0

Y = s/(s^2 = 4) ==> y(t) = cos(2t)

But of course the situation you actually have is

(s^2 + 4)Y - s = L[u(t - 2pi)*sin(t)]

~~~~~~~~~~~~~~~~~~~~~~~~

That means we need to find the LT of a product of a function and Heaviside or step function

A table of transforms quotes that

L[u(t)*f(t - 2pi)] = e^(-cs)*L[f(t)] = e^(-cs)*F(s) so we can say that

L[u(t)*sin(t - 2pi)] = e^(-2pi*s)*L[sin(t)] = e^(-2pi*s)*/(s^2 + 1)

but we want L[u(t - 2pi)*sin(t)] which just seems to need shifting.

~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~

In this page from "Paul's online notes" he starts by explaining that in order to take the transform of a function that involves a Heaviside we’ve got to make sure the function has been properly shifted.

I suggest you take over here and follow his examples through to see the shifting idea.

http://tutorial.math.lamar.edu/Classes/DE/IVPWithStepFunction.aspx

There is another helpful page here about Unit Step Functions and Laplace Transforms

http://www.sinclair.edu/centers/mathlab/pub/findyourcourse/worksheets/DiffEq/TheUnitStepFunction.pdf

Regards - Ian

woolum

2016-12-02 06:44:32 UTC

So: Flying automobiles, in yet another century. we are on the verge of understanding of gasoline this century, and it takes plenty greater potential to push something around mutually as conserving interior the air, than to push something around mutually because it sits on the floor. as quickly as we run out of gasoline, and detect a renewable selection for it, we are going to probable be waiting to handle the demands of flying automobiles that inhabitants improve will necessitate. "Visiphone"s are already in use right this moment. There are some 56k modem based ones (which suck, and particularly appear as if a slideshow). people use webcams and microphones to speak on broadband each and every of the time. the component this is retaining this 'technologies' back is that the communications infrastructure isn't there. telephone companies are (for now) required to lend others the use of their telephone lines, and so no one needs to construct technologies for telephony, whilst the internet can render it ineffective. Holograms. the priority with holograms is this is suited created with a laser, yet that the laser desires a medium to eliminate darkness from. this is why you notice the greater "reasonable" sci fi video clips with holograms projected on a layer of foggy air. it is not precisely hi-fi. And for modern-day verbal substitute purposes, this is solid adequate that we are able to make certain a photo of a individual, with out with the ability to communicate to the back of their head or see their baldspot. Moon, we don't opt to goto, this is uninteresting. Mars, the holiday time quandary (of a million/2 a decade) is as a results of nicely-known propulsion. there is an ion engine that in simple terms got here out, in spite of the incontrovertible fact that it's going to purely cut back flight time by making use of a few million/4, or possibly a 300 and sixty 5 days. nevertheless no longer a visit to the back backyard. or maybe then, the means for those fuels remains generally derived ultimately from fossil fuels (the two in production of the engine, or of the liquid hydrogen/oxygen combination, or for the potential saved interior the ion engine). And we are approximately to expire of that quickly. relatively, do no longer carry your breath for something neat, yet i'd pass your hands that we don't all turn waterworld type after the oil runs out.

This content was originally posted on Y! Answers, a Q&A website that shut down in 2021.

Laplace transform to solve the initial-value problem y"+4y=sin(t)U(t-2*pi), y(0)=1, y'(0)=0? (2024)
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