Function describing a moving waveform

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fog37
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Hello Forum,
  • I am first wondering about the possibility to factor a function ##f(x,t)## into a product of two functions, i.e. ##g(x) p(t)##. Is there any general rule that tells us if this decomposition is possible based on the characteristics of the function ##f(x,t)##?
  • If a function ##f(x,t)## is to represent a traveling wave, the same waveform ##f(x,t_0)## at time ##t_0## must be translated along the x-axis at later times ##t##: $$f(x-vt)$$
The function ##f(x,t)## and ##f(x-vt)## are the same waveforms, just translated in space by a factor ##vt##.

  • A standing wave is a wave that does not move or travel. For real-valued functions, the function describing a standing wave ca be factored: $$f(x,t)=g(x)p(t)$$ This means that the spatial function ##g(x)## is not translated but just modulated by the temporal function ##p(t)##. However, if the function ##g(t)## is not periodic, I think the product ##f(x,t)=g(x)p(t)## does not represent a standing wave but a traveling wave! Is that correct? could anyone provide further insight into this?
Thanks!
 
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Sorry fresh_42, I am not sure what you exactly mean. So, let's say we have function $$f(x,t)= [sin(x)] [e^{3t}]$$

where ##g(x)=sin(x)## and ##p(t)=e^{3t}##. What do you exactly suggest doing at this point?
 
fog37 said:
Sorry fresh_42, I am not sure what you exactly mean. So, let's say we have function $$f(x,t)= [sin(x)] [e^{3t}]$$

where ##g(x)=sin(x)## and ##p(t)=e^{3t}##. What do you exactly suggest doing at this point?
This is a wave with an increasing amplitude, not a moving wave. I thought, a wave is ##f(x)=A(x)\cdot \sin(\omega x)## if you want to have a variable amplitude. Now just make the position time dependent, ##x=x(t)##, e.g. ##x=v \cdot t## which in this case with a constant velocity is the same as considering the variable as time flow.
 
Actually, the function I gave seems to not be a moving wave: the spatial structure is a sine wave and the amplitude at each point, as you mention, increases exponentially with time. I don't see any oscillatory behavior or translational behavior.

A function like ##f(x,t)= sin(x) cos(t)## is instead a standing wave: the wave does not move but the amplitude at each point oscillates harmonically in time since ##cos(t)## is periodic.

I am still wondering if, given an arbitrary spatial function ##g(x)##, we can multiply it by a temporal function ##p(t)## and obtain a traveling wave ##f(x,t)=g(x) p(t)##...