Time-harmonic functions (Complex Vectors)

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The discussion centers on the time-average of time-harmonic functions, specifically whether the equality holds for a complex vector representation of v(t). It is established that the time-average of sinusoidal functions is zero when integrated over a complete period. The participants clarify that v(t) as defined does not represent a complex vector but rather a combination of cosine and sine functions. The conversation also emphasizes that the integral's result being zero is contingent on the time interval T being an integer multiple of the period. Ultimately, the consensus is that any sinusoidal function averages to zero over a complete cycle.
jeff1evesque
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Statement:
<v(t)> = \frac{1}{T} \int^{T}_{0}v(t)dt = \frac{1}{T} \int^{T}_{0}V_0cos(\omega t + \phi)dt \equiv 0. (#1)Relevant Question:
If we suppose v(t) is a complex vector, is the second equality above still true?Reasoning:
If v(t) is a complex vector, then v(t) = cos(\omega t)\hat{x} + sin(\omega t)\hat{y}.

But we also know (by sum to angle identity), cos(\omega t + \theta) = cos(\omega t)cos(\theta) - sin(\omega t)sin(\theta) \Leftrightarrow V_0cos(\omega t + \theta) = V_0[cos(\omega t)cos(\theta) - sin(\omega t)sin(\theta)= V_0[cos(\omega t)cos(\theta)]

But is the following true:
V_0[cos(\omega t)cos(\theta)] = cos(\omega t)\hat{x} + sin(\omega t)\hat{y} ?
Because in the original equation (#1), if v(t) is a complex vector, I cannot see why v(t) = V_0cos(\omega t + \phi)?thanks,
Jeff
 
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I don't really see how v(t) ( as you have defined it ) is a complex vector in the first place.
 
What I wrote was really,
<br /> v(t) = cos(\omega t)\hat{x} + sin(\omega t)\hat{y} = A\hat{x} + jB\hat{y}<br />

the left equality is really "instantaneous form".
 
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The fact remains that v(t) is not a complex vector. Sure, as we've talked about before, you can express the cosine function or the sine function as phasors if you like. I just don't see what that has to do with anything. Perhaps you could clarify your question? If your question is:

What is \langle \textbf{v}(t) \rangle if \textbf{v}(t) is defined as:

\textbf{v}(t) \equiv \cos(\omega t) \hat{\textbf{x}} + \sin(\omega t) \hat{\textbf{y}}​

Then I think that the answer is:

\langle \textbf{v}(t) \rangle \equiv \frac{1}{T} \left( \hat{\textbf{x}} \int_0^T \cos(\omega t)\, dt + \hat{\textbf{y}} \int_0^T \sin(\omega t)\, dt \right)

= 0\hat{\textbf{x}} + 0\hat{\textbf{y}}​

which kind of makes sense when you think about it, since the vector goes around in a circle and ends up back where it started.
 
I am just curious because in my notes it says "The time-average of any time-harmonic function is always zero." That part makes sense, I think you answered that last time for me. But I don't understand why v(t) = V_0cos(\omega t + \phi)? In previous pages of my notes, we've defined v(t) as both complex vectors, and complex vectors in the instantaneous form (I wrote above).
 
Without seeing your notes, it is difficult for me to comment further. The fact is,

\cos(\omega t) \hat{\textbf{x}} + \sin(\omega t) \hat{\textbf{y}} \neq V_0\cos(\omega t + \phi)​

The thing on the left hand side is a vector and the thing on the right hand side is a scalar. EDIT: As far as I can see, two different things are being talked about and are being referred to as "v(t)."
 
Since cosine and sine can be written as one another- by shifting the phase,

<br /> \frac{1}{T} \int^{T}_{0}v(t)dt = \frac{1}{T} \int^{T}_{0}V_0cos(\omega t + \phi)dt.<br />

Suppose \phi = 90\circ, then it follows

<br /> \frac{1}{T} \int^{T}_{0}v(t)dt = \frac{1}{T} \int^{T}_{0}V_0sin(\omega t)dt = - \frac{\omega V_0cos(\omega t)}{T}|^{T}_{0} \neq 0<br /> \Leftrightarrow T \neq 0

Doesn't that mean that a time-harmonic function is not always zero?

Thanks for reading my posts,JL
 
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\cos(\omega T) = \cos \left(\frac{2 \pi}{T}T\right) = \cos(2 \pi) = 1

\cos(0) = 1

\Rightarrow \cos(\omega T) - \cos(0) = 1 - 1 = 0​

Without doing any math, you can see that the integral of a sinusoidal function over any whole number of periods will be zero, because you will always be adding together an equal amount of "positive area" and "negative area" under the curve.
 
thanks
 
  • #10
jeff1evesque said:
thanks
As I said in the associate thread that I was helping you with, this only applies if T is in integer multiple of the period.
 
  • #11
Hootenanny said:
As I said in the associate thread that I was helping you with, this only applies if T is in integer multiple of the period.

For some reason in this example, I thought v(t) was some complex vector. Instead it shows that any sinusoid for harmonic functions have an time-average of zero, which is exactly what you said.

Thanks,JL
 
  • #12
Hootenanny said:
As I said in the associate thread that I was helping you with, this only applies if T is in integer multiple of the period.

Oh yeah. I assumed T WAS the period. But I guess T is the time interval over which you are averaging. In any case, I already stated as well that the integral would be zero over some whole number of periods, so we both got the disclaimer in there.
 
  • #13
cepheid said:
Oh yeah. I assumed T WAS the period. But I guess T is the time interval over which you are averaging. In any case, I already stated as well that the integral would be zero over some whole number of periods, so we both got the disclaimer in there.
No problem, I just thought that I would clarify since in the OP's previous question he stated that he didn't know what T was and it wasn't defined in his notes.
 

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