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Use the convolution integral to find the inverse transforms of:

p(p2-1)2=pp2-1.pp2-1

Short Answer

Expert verified

The inverse transform of given equation is tsinht2.

Step by step solution

01

 Step 1: Given information.

The equation iscp(p2-1)2=pp2-1.pp2-1 .

02

Inverse transform and Convolution theorem.

The piecewise-continuous and exponentially-restricted real function f(t) is the inverse Laplace transform of a function F(s), and it has the property:

L{f}(s)=L{ft}(s)=F(s)

where L is the Laplace transform.

As per Convolution theorem, if we have two functions, taking their convolution and then Laplace is the same as taking the Laplace first (of the two functions separately) and then multiplying the two Laplace Transforms.

03

Find the inverse transform of cp(p2-1)2=pp2-1.pp2-1 .

Consider the equation.

cp(p2-1)2=pp2-1.pp2-1

As per the convolution theorem.

role="math" localid="1659268906381" L-1pp2-1.pp2-1=∫0g1g2dx=∫0tg1xg2t-xdx=∫0tcoshxsinht-xdx=∫0tcoshxsinhcoshx-coshtsinxdx

Further solve,

role="math" localid="1659269317585" L-1pp2-1.pp2-1=sinht∫0tcoshx2dx-cosht∫0tcoshxsinhxdx=sinht∫0tcoshx2dx-cosht2∫0tcoshxsinhxdx=sinht∫0tcoshx2dx-cosht∫0tcoshxsinhxdx=tsinht2+sinht2.sinh2t2-cosht2.cosh2t2+12cosht2

Further solve,

role="math" localid="1659269600381" L-1pp2-1.pp2-1=tsinht2+14cosh2t-tcosht4=tsinht2-cosht4+cosht4=tsinht2

Thus, the inverse transform of given equation is =tsinht2.

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Most popular questions from this chapter

The speed of a particle on the x axis, x≥0, is always numerically equal to the square root of its displacement x. If x=0when t=0, find x as a function of t. Show that the given conditions are satisfied if the particle remains at the origin for any arbitrary length of time t0and then moves away; find x for t>t0for this case.

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

Find the position x of a particle at time t if its acceleration isd2xdt2=AtÓ¬sin.

(a) Show that D(eaxy)=eax(D+a)y,D2(eaxy)=eax(D+a)2y, and so on; that is, for any positive integral n, Dn(eaxy)=eax(D+a)ny.

Thus, show that ifis any polynomial in the operator D, then L(D)(eaxy)=eaxL(D+a)y.

This is called the exponential shift.

(b) Use to show that (D-1)3(exy)=exD3y,(D2+D-6)(e-3xy)=e-3x(D2-5D)y..

(c) Replace Dby D-a, to obtain eaxP(D)y=P(D-a)eaxy

This is called the inverse exponential shift.

(d) Using (c), we can change a differential equation whose right-hand side is an exponential times a

polynomial, to one whose right-hand side is just a polynomial. For example, consider

(D2-D-6)y=10×e2x; multiplying both sides by e-3xand using (c), we get

e-3x(D2-D-6)y=[D+32-D+3-6"]"ye-3x=(D2+5D)ye-3x=10x

Show that a solution of (D2+5D)u=10xis u=x2-25x; then or use this method to solve Problems 23 to 26.

(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.

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