How does a standing wave form?

In summary, standing waves form when two waves of the same frequency and wavelength travel in opposite directions and superpose on each other. However, the waves do not always add up to zero at all points due to the fact that the phases of the two waves must be in anti-phase for complete cancellation. The reflected wave is not always a complete mirror opposite of the incoming wave, which is why standing wave patterns can have non-zero displacement at certain points. This is due to impedance mismatches and the reflection causing resonances in the system.
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phantomvommand
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A short explanation on how standing waves form would be appreciated
I understand how waves undergo superposition. However, for a standing wave, the reflected wave is a mirror opposite of the incoming wave. By the superposition principle, won’t the 2 waves add up to 0, at all points?
 
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Take, for instance, ##f(x,t) = \sin{(kx - \omega t)}## and ##g(x,t) = \sin{(kx + \omega t)}##; by a trig identity then$$h(x,t) := f(x,t) + g(x,t) = 2 \sin{(kx)} \cos{(\omega t)}$$which is a standing wave, and definitely not everywhere zero! It's because the incident and reflected waves generally don't meet in anti-phase, apart from the times when the wave-crests meet the boundary [for the above example you can take the boundary, or mirror, to be ##x=0##].

Try plotting some oppositely traveling waves on https://www.desmos.com/calculator to build intuition :smile:
 
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When two waves of the same frequency and wavelength travel in opposite directions, something cancels. It’s not the waves themselves (that’s destructive interference) it’s the direction of travel hence the name “standing wave” as opposed to “traveling wave”.
 
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There are instants when the superpositioned waves are zero (namely when [itex] t [/itex] is such that @etotheipi 's [itex] \cos(\omega t)=0 [/itex]), but apart from those instants, only the "nodes" (the [itex] x [/itex]'s where [itex] \sin(kx)=0 [/itex]) of the standing wave are forever zero--the superpositioned waves for other locations have a nonzero displacement.
 
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  • #5
kuruman said:
It’s not the waves themselves (that’s destructive interference)
Why distinguish between the situations. If the resultant amplitude is less than the mean of one wave then you have destructive interference. The standing wave pattern is stationary in just the same way that a (stationary / standing) interference pattern forms on a screen. Precisely the same phenomenon.
Many standing wave patterns do not have perfect zeros, of course.
 
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phantomvommand said:
However, for a standing wave, the reflected wave is a mirror opposite of the incoming wave.
I don't know what you mean by a mirror opposite. There are instants when the reflected wave is identical in shape to the incoming wave. In those cases you get constructive interference. There are other instants where they are out of phase and you get destructive interference.
 
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  • #7
phantomvommand said:
Summary:: A short explanation on how standing waves form would be appreciated

I understand how waves undergo superposition. However, for a standing wave, the reflected wave is a mirror opposite of the incoming wave. By the superposition principle, won’t the 2 waves add up to 0, at all points?
That rather depends on the mirror!

In some cases, yes this is precisely what happens and it is called a 'perfectly matched load'.

In others, there is a mismatch between the incoming wave and the 'load'.

That's why in RF engineering, for example, if one wants to be rid of standing waves (which one very much usually does want) then the transmission line and the load it goes into have to be configured in such a way that their impedances are conjugate.

In mechanical examples, such as a plucked string on a guitar, the mechanical wave of the string has a low 'mechanical' impedance and the bridge it is attached to is very high, hence the reflected wave. (If the bridge was made of a sponge then it'd be more a matched load and the energy absorbed.) This impedance mismatch creates the reflection but it is imperfect and some small component of the energy in that wave is dissipated into the bridge, the remainder goes back into the string. That wave resonates on the string, and the small component of the energy that goes into the bridge (defined by the 'Q' of the system) then stimulates modes in the guitar body which radiates the noise.
 
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  • #8
phantomvommand said:
Summary:: A short explanation on how standing waves form would be appreciated

By the superposition principle, won’t the 2 waves add up to 0, at all points?
To get cancellation, the waves have to be of the same amplitude and exactly in anti phase. The phase of the forward wave, viewed at one point, will constantly be progressing. The phase of the reflected wave will also be constantly progressing. It's only if the path from the wave, via the mirror and back, is exactly a whole number of wavelengths that the phases of the two waves are in anti phase to give a node. (Both in phase for an antinode) at nowhere else will this happen and you will get a non-zero resultant of the complex addition of the two waves. If you assume a rigid fixing at the 'mirror' or a short circuit if it's a electrical wave then the reflected signal will be in anti phase at the point of reflection and if you have a free end or an open circuit at the reflection point, the reflected wave will be in phase and the positions of nodes and antinodes in the standing wave will swap.
 
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  • #9
Exactly the same thing is going on with the 2D interference pattern for just two sources. There are regions of highs and lows, which are stationary. If the two sources are far apart (a couple of wavelengths, say, the pattern won't just be the familiar 'rays', spreading out from Young's slits but there will be a 'chequered' pattern on top of the 'rays' so in any given direction it goes from maxes to mins between the sources.
This Wiki image has various combinations of spacings to produce a range of patterns. The line between the sources shows a simple standing wave.
1621185281042.png
 

1. How does a standing wave form?

A standing wave is formed when two waves with the same frequency and amplitude travel in opposite directions and interfere with each other. This results in certain points along the wave where the amplitude is always zero, known as nodes, and points where the amplitude is at its maximum, known as antinodes. The interference between the waves causes the energy to be trapped in a specific area, creating the standing wave pattern.

2. What factors affect the formation of a standing wave?

The formation of a standing wave is affected by the frequency and amplitude of the two interfering waves, as well as the medium through which the waves are traveling. The length and boundary conditions of the medium can also impact the formation of standing waves.

3. Can standing waves form in any type of medium?

Yes, standing waves can form in any type of medium, as long as there is a source of two waves with the same frequency and amplitude traveling in opposite directions. This includes solids, liquids, and gases.

4. What are some real-life examples of standing waves?

Standing waves can be observed in a variety of natural and man-made systems. Some examples include musical instruments such as stringed instruments, organ pipes, and drums, as well as seismic waves in the Earth's crust, and electromagnetic waves in transmission lines.

5. How are standing waves used in practical applications?

Standing waves have many practical applications, including in musical instruments, where they create specific harmonics and tones, and in communication systems, where they are used to transmit and receive signals. They are also used in medical imaging techniques such as ultrasound and in industrial processes such as ultrasonic cleaning.

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