Are Sin(nt) and Cos(mt) Orthogonal Over the Interval (0, 2π)?

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Homework Help Overview

The discussion revolves around the orthogonality of the functions f(t) = sin(nt) and g(t) = cos(mt) over the interval (0, 2π), with a focus on the implications for Fourier series analysis. Participants explore the integral of the product of these functions and the conditions under which they are considered orthogonal.

Discussion Character

  • Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants attempt to evaluate the integral of sin(nt) cos(mt) and discuss the implications of the result in the context of Fourier series. Questions arise regarding the evaluation of definite integrals and the significance of integer values in the cosine function.

Discussion Status

The discussion is active, with participants clarifying steps in the integration process and addressing potential pitfalls related to special cases where n equals m. Some guidance has been offered regarding the evaluation of terms and the implications of the results, though no consensus has been reached on formal proof details.

Contextual Notes

Participants note the importance of considering cases where n equals m, as this introduces complications in the evaluation of the integral and the resulting expressions. There is an ongoing exploration of the implications of these cases on the overall proof of orthogonality.

CSNabeel
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Homework Statement



Show that provided that m and n are arbitrary integers, the two functions f(t) = sin nt and g(t) = cos mt are orthogonal over the interval (0,2[tex]\pi[/tex]). Explain the significance of this result in Fourier series analysis. Hint: you may find the following trigonometric identity useful 2sin a cos b = sin(a+b) - sin (a-b)


Homework Equations





The Attempt at a Solution



[tex]\int[/tex] f(t) g(t) dt
[tex]\int[/tex] sin nt cos mt dt
[tex]\int[/tex] 0.5( sin(n+m)t - sin(n-m)t)dt
0.5[ [tex]\frac{cos(n+m)t}{n+m}[/tex] - [tex]\frac{cos(n-m)t}{n-m}[/tex] ]

put (0,2[tex]\pi[/tex]) into (n,m) respectively (sorry not good with code thing).

After subistion the final answer end up being

t over 2[tex]\pi[/tex]

this is my working out so far but what should I write about it under Fourier analysis
 
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You don't put (0,2*pi) into (n,m). You set t=2*pi and t=0 into the anti derivative and subtract the results. There's no t in the final answer. What's cos(k*2*pi) where k is an integer?
 
so in that case does it become

[ cos 2*pi*(n+m) / n + m ] - [ cos 2*pi*(n-m) / n - m ]

?
 
CSNabeel said:
so in that case does it become

[ cos 2*pi*(n+m) / n + m ] - [ cos 2*pi*(n-m) / n - m ]

?

It becomes that minus [ cos 0*(n+m) / n + m ] - [ cos 0*(n-m) / n - m ]. Haven't you done definite integrals before?
 
yeah sorry I made a mistake cancelling that because cos 0 = 1 and forget that the denominator where different

so it becomes

[ cos 2*pi*(n+m) / n + m ] - [ cos 2*pi*(n-m) / n - m ] - [1 / n + m] - [ 1 / n - m]

right?
 
I would write that as cos(2*pi*(n+m))/(n+m) - cos(2*pi*(n-m))/(n-m) - [(1/(n+m)-1/(n-m)]. Use enough parentheses and brackets so your meaning is clear. But, yes, I think you mean the right thing. Now what's cos(k*2*pi) where k is an integer?
 
the integral of cos(k*2*pi) is -sin(k*2*pi)/(2*pi)
 
CSNabeel said:
the integral of cos(k*2*pi) is -sin(k*2*pi)/(2*pi)

I'm not asking you what the integral is. I'm asking you what the value of cos(k*2*pi) is where k is an 'integer' - not 'integral'. If k=1, that's cos(2*pi), if k=2, that's cos(4*pi), if k=3 that's cos(6*pi) etc etc. I'm asking you this because (n+m) and (n-m) are integers.
 
oh well in that case cos(k*2*pi) = 1
 
  • #10
CSNabeel said:
oh well in that case cos(k*2*pi) = 1

Right, so what's the value of the integral now that you know what all the terms are?
 
  • #11
I think it's [(1/(n+m)-1/(n-m)] - [(1/(n+m)-1/(n-m)] which I think cancels out?
 
  • #12
CSNabeel said:
I think it's [(1/(n+m)-1/(n-m)] - [(1/(n+m)-1/(n-m)] which I think cancels out?

Yes, it's zero. That means f(t)=sin(nt) and g(t)=cos(mt) are orthogonal over the interval [0,2*pi] since the integral of f(t)*g(t) over that interval is zero. There is a minor technical point. What happens if n=m or n=(-m)? Then your expression has a zero in the denominator. Can you see why that's not really a problem?
 
  • #13
yeah I think so, they still cancel out even though 1/0 tends to infinity
 
  • #14
CSNabeel said:
yeah I think so, they still cancel out even though 1/0 tends to infinity

That's dangerous reasoning. The point is that if e.g. n=m, then sin((n-m)*t)=sin(0*t)=0. The cos((n-m)t)/(n-m) term isn't in the antiderivative. If you are going to be formal about the proof the you might want to make those special cases.
 
  • #15
ahhh I see. Thanks you been really helpful
 

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