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Show that in (5.2 ) the average values ofsinmxsinnx and of cosmxcosnx,mnare zero (over a period), by using the complex exponential forms for the sines and cosines as in (5.2).

Short Answer

Expert verified

The function is -ππ(sinmx)sin(nx)dx=-ππ(cosmx)cosnxdx=0formn12form=n.

Step by step solution

01

Given

The given expressions are sin(mx)sin(nx) and cos(mx)cos(nx),mn.

02

Definition of Integral

The definite integral of a real-valued function f(x)with respect to a real variable xon an interval [a, b] is expressed as abf(x)dx=F(b)-F(a).

Here, = Integration symbol, a= Lower limit, b= Upper limit, f(x) Integral and dx Integrating agent

Thus, abf(x)dxis read as the definite integral of f(x]with respect to dx from a to b.

03

Integrate the Cosines

Apply integral on cosines.

12π-ππ(cosmx)cosnxdx=12π-ππeimx+e-imx2einx+e-inx2dx=18π-ππeimx+e-imxeinx+e-inxdx=18π-ππeix(m+n)+eix(m-n)+eix(n-m)+e-ix(m+n)dx=14πeix(m+n)i(m+n)+eix(m-n)i(m-n)+eix(n-m)i(n-m)-e-ix(m+n)i(m+n)-ππ

Calculate further as shown below.

12π-ππ(cosmx)cosnxdx=18πeix(m+n)i(m+n)-e-ix(m+n)i(m+n)+eix(m-n)i(m-n)+eix(n-m)i(n-m)-ππ=14πsin{x(m+n)}m+n+sin{x(m-n)}m-n-ππ=12πsin{π(m+n)}m+n+sin{π(m-n)}m-n

For mn, where mNand nN, the above result is equal to zero.

For m=n, first term =0.

12π-ππ(cosmx)cosnxdx=12πsin{π(m-n)}m-n

Take the limit limmn012πsinπm-nm-n.

We know that limx0sinxx=1.

limmn012πsin{π(m-n)}m-n=π2π=12

04

Integrate the sines

Apply integral on sines.

12π-ππ(sinmx)sin(nx)dx=12π-ππeimx-e-imx2einx-e-inx2dx=18π-ππeimx-e-imxeinx-e-inxdx=18π-ππeix(m+n)-eix(m-n)-eix(n-m)+e-ix(m+n)dx=14πeix(m+n)i(m+n)-eix(m-n)i(m-n)-eix(n-m)i(n-m)-e-ix(m+n)i(m+n)-ππ

Calculate further as follows:

12π-ππ(sinmx)sin(nx)dx=18πeix(m+n)i(m+n)-e-ix(m+n)i(m+n)-eix(m-n)i(m-n)-eix(n-m)i(m-n)-ππ=14πsin{x(m+n)}m+n-sin{x(m-n)}m-n-ππ=12πsin{π(m-n)}m-n-sin{π(m+n)}m+n

For mn, where mN and nN, the above result is equal to zero.

For m=n, second term =0.

12π-ππ(sinmx)sin(nx)dx=12πsin{π(m-n)}m-n

Take the limit limm-n012πsin{π(m-n)}m-n.

We know thatlimx0sinxx=1.

limm-n012πsin{π(m-n)}m-n=π2π=12

Hence, -ππ(sinmx)sin(nx)dx=-ππ(cosmx)cosnxdx=0,formn12form=n.

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Most popular questions from this chapter

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

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.

A general form of Parseval’s theorem says that if two functions are expanded in Fourier series

f(x)=12a0+1ancosnx+1bnsinnxg(x)=12a'0+1a'ncosnx+1b'nsinnx

then the average value off(x)g(x)=14a0a'0+121ana'n+1bnb'n.Prove this.

Find the average value of the function on the given interval. Use equation (4.8) if it applies. If an average value is zero, you may be able to decide this from a quick sketch which shows you that the areas above and below the xaxis are the same.

cosxon(0,3π)

Use Parseval’s theorem and the results of the indicated problems to find the sum of the series in Probllems 5 to 9. The series n=11n4 ,using problem 9.9.

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