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By using Laplace transforms, solve the following differential equations subject to the given initial conditions.

y''+2y'+10y=-6e-tsin3t,y0=0,y'0=1

Short Answer

Expert verified

The given differential equation's solution is y(t)=te-tcos3t.

Step by step solution

01

Given information from question

The differential equation is y''+2y'+10y=-6e-tsin3t,y0=0,y'0=1.

02

Laplace transform

Application of Laplace transform:

It's used to simplify complicated differential equations by using polynomials. It's used to convert derivatives into numerous domain variables, then utilise the Inverse Laplace transform to convert the polynomials back to the differential equation.

03

Use Laplace transform on both sides of given differential equation

The initial conditions arey0=0,y'0=1.

Consider L35 result of Laplace transform of derivative of y.

L(y)=YL(y')=pY-y0L(y'')=p2Y-p0-y'0Le-atsinbt=p+ap+a2+b2,Rep+a>lmb

Use Laplace on both sides of given differential equation

Ly''+2y'+10y=L-6e-tsin3t

Compare right hand side termL-6e-tsin3twith the general termLe-atsinbt.

a=1b=3

04

Apply linearity property of Laplace transformation

Use linearity property of Laplace transformation as

Ly''+2Ly'+10Ly=-6Le-tsin3tp2Y-py0-y'0+4pY-y0+10y=-63p+12+32p2+2p+10Y=-18p+12+32+1

Consider the equation,

p2+2p+10=p2+2p+1+9=(p+1)2+32

Use this in above equation.

p2+2p+10Y=-18p+12+32+1Y=-18p+12+32p+12+32+1p+12+32y=-18p+12+322+1p+12+32y=p+12+32p+12+322

The term (p+1)2-32p+12+32-2contains variable (p+1) instead of p.

So, use frequency shift theorem to replace p with (p-1). From this replacement, one can use Laplace inverse transformation.

05

Solve further for frequency shift theorem

The frequency shift theorem

yt=L-1Ype-p0ty(t)=L-1Yp+p0

Substitute -1 for p and (p - 1) for p in above equation.

Solve further

e2tyt=L-1Yp-1 ……. (1)

Yp=p+12-32p+12+322

Substitute p-1 for p in above equation.

Yp-1=2p-1+1-32p-1+12+32=p2-32p2-322

Substitute the value in equation (1)

role="math" localid="1659256010718" e2tyt=L-1Yp-1e2tyt=L-1p2-32p2+322=tcos(3t)tcosat=L-1p2-a2p2+a22

Divide both side by.

y(t)=te-tcos3t

Thus, the given differential equation's solution is y(t)=te-tcos3t.

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Most popular questions from this chapter

(a)Consider a light beam travelling downward into the ocean. As the beam progresses, it is partially absorbed and its intensity decreases. The rate at which the intensity is decreasing with depth at any point is proportional to the intensity at that depth. The proportionality constant μis called the linear absorption coefficient. Show that if the intensity at the surface is I0, the intensity at a distance s below the surface is I=I0eμs. The linear absorption coefficient for water is of the order of 10.2ft.1(the exact value depending on the wavelength of the light and the impurities in the water). For this value of μ, find the intensity as a fraction of the surface intensity at a depth of 1 ft, ft,ft,mile. When the intensity of a light beam has been reduced to half its surface intensity (I=12I0), the distance the light has penetrated into the absorbing substance is called the half-value thickness of the substance. Find the half-value thickness in terms of μ. Find the half-value thickness for water for the value of μgiven above.

(b) Note that the differential equation and its solution in this problem are mathematically the same as those in Example 1, although the physical problem and the terminology are different. In discussing radioactive decay, we call λthe decay constant, and we define the half-life T of a radioactive substance as the time when N=12N0(compare half-value thickness). Find the relation between λand T.

By using Laplace transforms, solve the following differential equations subject to the given initial conditions.

y"+16y=8cos4t,y0=0,ψ'0=8

Consider an equation for damped forced vibrations (mechanical or electrical) in which the right-hand side is a sum of several forces or emfs of different frequencies. For example, in (6.32) let the right-hand side be F1eiω1t+F2eiω2t+F3eiω3t,

Write the solution by the principle of superposition. Suppose, for giventhat we adjust the system so that ω=ω1'; show that the principal term in the solution is then the first one. Thus, the system acts as a "filter" to select vibrations of one frequency from a given set (for example, a radio tuned to one station selects principally the vibrations of the frequency of that station).

Using (3.9), find the general solution of each of the following differential equations. Compare a computer solution and, if necessary, reconcile it with yours. Hint: See comments just after (3.9), and Example 1.

2xy+y=2x5/2

In Problem 33 to 38, solve the given differential equations by using the principle of superposition [see the solution of equation (6.29)]. For example, in Problem 33, solve three differential equations with right-hand sides equal to the three different brackets. Note that terms with the same exponential factor are kept together; thus, a polynomial of any degree is kept together in one bracket.

y"-2y'=9xe-x-6x2+4e2x

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