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Use L34 and L2 to find the inverse transform of G(p)H(p)whenand G(p)=1/(p+a)andH(p)=1/(p+b); your result should be L7 .

Short Answer

Expert verified

The inverse transforms of is GpHpis1b-ae-at-e-bτ.

Step by step solution

01

Given information.

The given expressions are andGpHpis1p+aandHpis1p+b .

02

Inverse transform.

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{f}(s)=F(s)

where L is the Laplace transform.

03

Find the inverse transform of G(p)H(p). .

Calculate Laplace inverse.

L-1GpHp=g*h=0tgt-τhτdτ

Calculate Laplace inverse of Gp.

role="math" localid="1659264162995" L-1Gp=L-11p+agt=e-atgt-τ=e-at-τ

Calculate Laplace inverse of H(p).

L-1Hp=L-11p+bht=e-btht-τ=e-bτ

Calculate Laplace inverse of G(p)H(p) .

L-11p+a1p+b=1b-ae-at-e-bτ

Thus, the Laplace inverse of is GpHpis1b-ae-at-e-bτ..

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Most popular questions from this chapter

Find the shape of a mirror which has the property that rays from a point 0 on the axis are reflected into a parallel beam. Hint: Take the point 0 at the origin. Show from the figure that tanθ=2yx. Use the formula for tanθ2to express this in terms of tanθ=dydxand solve the resulting differential equation. (Hint: See Problem 16.)

The momentum pof an electron at speednear the speedof light increases according to the formula p=mv1-v2c2, whereis a constant (mass of the electron). If an electron is subject to a constant force F, Newton’s second law describing its motion is localid="1659249453669" dpdx=ddxmv1-v2c2=F.

Find v(t)and show that vcas t. Find the distance travelled by the electron in timeif it starts from rest.

Solve the following sets of equations by the Laplace transform method

.y'+2z=1y0=02y-zz'=2tz0=1

In Problems 13 to 15, find a solution (or solutions) of the differential equation not obtainable by specializing the constant in your solution of the original problem. Hint: See Example 3.

13. Problem 2

(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.

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