In Problems 13to 16, find the Fourier cosine transform of the function in the indicated problem, and write f(x)as the Fourier integral [ use equation (12.15)]. Verify that the cosine integral for f(x)is the same as the exponential integral found previously.

15. Problem 9

Short Answer

Expert verified

The Fourier cosine transform of the function in the problem 9, written in the Fourier integral is:

f(x)=4π01-cos(αa)α2cos(αx)dα

Step by step solution

01

Meaning of Fourier Sine and Cosine Transform

The Fourier sine and cosine transforms are versions of the Fourier transform that don't employ complex numbers or require negative frequency in mathematics.

02

Given parameter

Given the graph of a function

03

Find the Fourier integral

The function of the Fourier cosine transform will be calculated as

g(α)=2π0a2(α-x)cos(αx)dx=22π0a[a0acos(αx)dx-0axcos(αx)dx]=22π[aαsin(αx)|0a-(xαsin(αx)+1α2cos(αx))|0a]=22π[aαsin(αa)-aαsin(αa)+cos(αa)-1α2]

g(α)=22π1-cos(aα)α2

Then the Fourier integral will be

f(x)=4π01-cos(aα)α2cos(αx)dα

04

Find the Fourier cosine of the function

The solution to the problem 9 is:

f(x)=2π-1-cos(αa)α2eiαxdα

As the function in front of the complex exponential is now even, then the integration will only save the cosine part of the complex exponential.

This implies that

f(x)=2π-1-cos(αa)α2cos(αx)dα=4π01-cos(αa)α2cos(αx)dα

It clarifies that the cosine integral is same as the exponential integral.

So, the Fourier cosine transform is:

f(x)=4π01-cos(αa)α2cos(αx)dα

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Most popular questions from this chapter

We have said that Fourier series can represent discontinuous functions although power series cannot. It might occur to you to wonder why we could not substitute the power series for sinnxand cosnx(which converge for all x) into a Fourier series and collect terms to obtain a power series for a discontinuous function. As an example of what happens if we try this, consider the series in Problem 9.5. Show that the coefficients of x, if collected, form a divergent series; similarly, the coefficients of x3form a divergent series, and so on.

Expand the same functions as in Problems 5.1 to 5.11 in Fourier series of complex exponentials einx on the interval (-π,π)and verify in each case that the answer is equivalent to the one found in Section 5.

The diagram shows a “relaxation” oscillator. The chargeqon the capacitor builds up until the neon tube fires and discharges the capacitor (we assume instantaneously). Then the cycle repeats itself over and over.

(a) The charge q on the capacitor satisfies the differential equation

, here R is the Resistance, C is the capacitance and Vis the

Constant d-c voltage, as shown in the diagram. Show that if q=0 when

t=0 then at any later time t (during one cycle, that is, before the neon

Tube fires),

(b) Suppose the neon tube fires at. Sketch q as a function of t for

several cycles.

(b) Expand the periodic q in part (b) in an appropriate Fourier series.

Given f(x)=|x|on (-π,π), expand f(x)in an appropriate Fourier series of period2π.

The velocity of sound in sea water is about 1530m/sec. Write an equation for a sinusoidal sound wave in the ocean, of amplitude 1 and frequency1000hertz .

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