Harmonic Function (time averages) II

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SUMMARY

The discussion focuses on the time average of the product of two harmonic functions, A(t) and B(t), represented by the equations A(t) = |A|cos(ωt + α) and B(t) = |B|cos(ωt + β). The time average is calculated using the integral = (1/2)|A||B|cos(α - β), with the integral of cos(2ωt + α + β) over a complete period resulting in zero. This is confirmed by the property of sine functions, where sin(θ + 2nπ) = sin(θ), leading to the conclusion that the integral of a cosine function over any whole number of periods is zero.

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jeff1evesque
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Statement:
[tex]A(t) = |A|cos(\omega t + \alpha), B(t) = |B|cos(\omega t + \beta)[/tex]

The time average of the product is given by:
[tex]<A(t)B(t)> = \frac{1}{T} \int^{T}_{0}A(t)B(t)dt = \frac{|A||B|}{2T}\int^{T}_{0}cos(2\omega t + \alpha + \beta)dt + \int^{T}_{0}cos(\alpha - \beta)dt] = \frac{1}{2}|A||B|cos(\alpha - \beta)[/tex]Relevant equations:
Note: using trigonometric identities:
[tex]A(t)B(t) = \frac{1}{2} |A||B|[cos(2\omega t + \alpha + \beta) + cos(\alpha - \beta)][/tex]Questions:
How is [tex]\int^{T}_{0}cos(2\omega t + \alpha + \beta)dt = 0?[/tex]
When I worked it out I got [tex]\int^{T}_{0}cos(2\omega t + \alpha + \beta)dt = \frac{1}{(2w)} sin(u) |^{T}_{0} = \frac{1}{2w}sin(2\omega t + \alpha + \beta)^{T}_{0} \neq 0[/tex]Is there a real-world application for taking the product of two harmonic functions (even an application for phasors)??

thanks
 
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jeff1evesque said:
Statement:

Questions:
How is [tex]\int^{T}_{0}cos(2\omega t + \alpha + \beta)dt = 0?[/tex]
When I worked it out I got [tex]\int^{T}_{0}cos(2\omega t + \alpha + \beta)dt = \frac{1}{(2w)} sin(u) |^{T}_{0} = \frac{1}{2w}sin(2\omega t + \alpha + \beta)^{T}_{0} \neq 0[/tex]

HOW is it not zero? By definition, ωT = 2π



[tex]\sin(2 \omega t + \alpha + \beta) |_0^T[/tex]

[tex]= \sin(4 \pi + \alpha + \beta) - \sin(\alpha + \beta) = 0[/tex]


because,

[tex]\sin(\theta + 2n\pi) = \sin(\theta)[/tex]​

The integral of a cosine function over any whole number of periods is zero (that much is obvious just by looking at it).
 

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