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Old April 30th, 2009, 09:21 AM
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Default Orthogonality of sin functions?

Hey, I'm looking through a solution to a problem and I'm not sure how this line went to the next.


Apologies for the writing. (Not my solution :P).

The reason it gave is (orthogonality of sin functions) which I don't understand.

Dn is a constant btw.

Thanks a lot.

Mark.
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Old April 30th, 2009, 09:37 AM
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Quote:
Originally Posted by MarkH747 View Post
Hey, I'm looking through a solution to a problem and I'm not sure how this line went to the next.


Apologies for the writing. (Not my solution :P).

The reason it gave is (orthogonality of sin functions) which I don't understand.

Dn is a constant btw.

Thanks a lot.

Mark.
It should be noted that \sum_{n=1}^{\infty}D_n \sin\!\left(n\pi x\right) is a Fourier Sine Series, where the coefficient is D_n=\frac{2}{L}\int_0^L f\!\left(x\right)\sin\!\left(n\pi x\right)\,dx. From what I see, 0<L<1 and f\!\left(x\right)=x(2-x), so it turns out that D_n=2\int_0^1x\left(2-x\right)\sin\!\left(n\pi x\right)\,dx

Does that make sense?
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Old April 30th, 2009, 09:46 AM
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The "orthogonality of sine functions" refers to the fact that \int_0^{2\pi} sin(nx)sin(mx)dx= 0 as long as m\ne n. You can prove that by using the trig identity sin(nx)sin(mx)= (1/2)[cos((n+m)x+ cos((n-m)x)].

The term "orthogonality" comes from thinking of integrable functions, periodic on [0, 2\pi] as a vector space having {sin x, cos x, sin 2x, cos 2x, ...} as "basis" and inner product <f, g>= \int_0^{2\pi} f(x)g(x)dx.
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Old April 30th, 2009, 11:48 AM
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Thanks a lot. Makes a bit more sense now.
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