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Obtain L(te-atcosbt)

Short Answer

Expert verified

Answer

The solution is Lte-atcosbt-p+a2-b2φ+a2+b22

Step by step solution

01

Given information

The given function is ft=te-atcosbtand to prove isLteatcosbt

02

Definition of Laplace Transformation

A transformation of a function f(x) into the function g(t) that is useful especially in reducing the solution of an ordinary linear differential equation with constant coefficients to the solution of a polynomial equation.

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

03

Properties used for given function


L29:Le-atgt=Gp+aL12:Ltcosat=p2-a2p2+a22

04

Proof for given function

From L29

Le-aiggt=Gp+a

Since from L11

Le-aiggt=Gp+a

Consider gt=tcosbtand by use of (L29), L e-atgt=Gp+a;Lte-wcosbtcan be calculated by replace pbyp+ain equation as,

Ltcosbt=p2-b2p2+b22Lte-atcosbt=p+a2-b2p+a2+b22

Hence, Lte-atcosbt=p+a2-b2p+a22

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(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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