For integral k, verify L5and L6in the Laplace transform table. Hint: From L2you can write: 0e-pte-atdt=1/(p+a). Differentiate this equation repeatedly with respect to p. (See Chapter 4, Section 12, Example 4, page 235.) Also noteL32for theΓfunction results inL5andL6, see Chapter 11, Problem 5.7.

Short Answer

Expert verified

The final value is Ltk=k!pk+1orΓ(k+1)pk+1 for L5.

The final value isLtke-at=k!(p+a)k+1 orΓ(k+1)(p+a)k+1 forL6 .

Step by step solution

01

Given information

The given expressions are 0e-pte-atdt=1(p+a).

02

Differential equation

An equation that contains the variables and the derivatives is called a differential equation.

03

Verify L5 from the Laplace transform table

Laplace transform is an important concept that is helpful to solve a differential equation.

VerifyL5 from the Laplace transform table.

Ltk=0e-pttkdt=0e-sspkdsp=1pk+10e-sskds=Γ(k+1)pk+1

Hence, the final value isLtk=k!pk+1 or Γ(k+1)pk+1.

04

Verify L6 from the Laplace transform table.

Verify L6from the Laplace transform table.

Ltke-at=0e-pttke-atdt

=0e-t(a+p)tkdt=Γ(k+1)(p+a)k+1

Hence, the final value isLtke-at=k!(p+a)k+1orΓ(k+1)(p+a)k+1..

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Most popular questions from this chapter

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

y''-8y'+16y=32t,y0=1,y0'=2

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).

(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.

Find the solutions of (1.2)(putI=dqIdt)and (1.3), if V=V0sinω't( const.).

The speed of a particle on the x axis, x0, 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.

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