The Fundamental Principle of Standing Waves: Is it all about phase?

AI Thread Summary
The discussion centers on the nature of standing waves, emphasizing that they result from the superposition of two waves traveling in opposite directions, creating nodes and antinodes. It clarifies that standing waves can form immediately when a wave is reflected at a fixed point, contradicting the notion that they require time to build up. The conversation also touches on the identification of nodes from still images and the relationship between standing waves and harmonics, noting that harmonics are multiples of the fundamental frequency. Additionally, it addresses misconceptions about energy dissipation and phase relationships in standing waves. Overall, the principles of standing waves and their characteristics are affirmed as fundamental in wave mechanics.
  • #51
sophiecentaur said:
Whatever direction the displacement takes place in, you can still get a resultant when two waves coincide. I think your diagrams may be confusing wave fronts with displacement.
You can use pressure (which corresponds to displacement) or speed (average speed, if it's a gas). The pressure max will be at a velocity min, of course. You can still do the sums but it's normal to consider displacement as it's zero at a wall.

Wavefronts are point on a wave that join up all adjacent points.
Displacement is the maximum distance traveled from resting point.
On my diagram, the point between two lines represents the distance between two new waves - ah I see why I got confused!

How then would I draw a displacement graph for a longitudinal wave or does this not exist?
 
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  • #52
Why do I use pressure? not speed or displacement?

You must have done the kinetic theory by now.

Sound is a pressure wave.
Pressure is the average result of the movement of a large number of individual particles, not in any way aligned like in a transverse wave.
So, on average, the pressure ( ie particle concentration) at any location varies periodically. Individual particles may be moving in widely different patterns and speeds. Tracking the actions of any single particle will not lead to a wave.
 
  • #53
I have uploaded a question here about waves and superposition http://www.mediafire.com/file/bg6raawvbv8mbts/A%20loudspeaker%20is%20connected%20to%20a%20signal%20generator1.doc

here are my answers. Could you please check them:

"Questions"

a) Explain why the minima never have a zero value. [2]
b) As the microphone is moved towards the metal plate, the amplitudes at the minima gradually decrease. Suggest why this happens. [2]

"My answers"
a) the reflected wave will have less energy than the wave produced by the speaker. This means the amplitudes of the both waves cannot destroy one another (interfere totally deconstructivl) as the two amplitudes are not of equal magnitude

b) The sound wave produced by the sound emitted from the microphone will have lost energy as it propagates towards the microphone - hence the amplitudes of the waves will be smaller.
The path difference decreases as the microphone moves closer to the metal plate, so the energy level of both waves will be more similar, as will the amplitudes, so the deconstructive interference becomes more obvious.

How do you rate these answers? are they even correct?
 
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  • #54
How do you rate these answers? are they even correct?

You mean apart from the obvious howler in (b) ?
sound emitted from the microphone

(a) The pressure variation in the sound is about an average value. Obviously the pressure can never actually be negative . Can it be zero?

(b) You got the general idea. Obviously the power in the reflected wave can never be greater than the incident. The power emitted by the loudspeaker is spread out through a larger volume as it travels away. This may not be an inverse square law since it depends upon the directionality of the speaker. So yes close to the speaker there is a much bigger disparity between the power of the direct and the reflected waves than close to the reflector.
 
  • #55
sound emitted from the microphone

Ye kinda big mistake!

quickly thinking back to this
Wave 1: ¦¦¦¦¦¦¦¦¦¦
Wave 2: ¦¦¦¦¦¦¦¦¦¦
(ignore the bits in-between each wave front ¦ - the middle bit)

Superimposed wave: ¦ ¦ ¦ ¦ ¦ ¦

Would this diagram be true if I plotted against time on the x-axis.
The space between each wavefront is the wavelength. It should take about double as long to complete a wavelength if we interfere constructively so the time taken along the x-axis between each wavefront should also be double?
 
  • #56
This issue is often rushed over in textbooks.

For a traveling wave you can put either time or distance on the x-axis and draw a graph of some suitable quantity such as displacement or pressure against this.

So your graph describes how the wave varies in time at a fixed position in space

or

how the wave varies in space at a fixed instant in time.

Both graphs actually look pretty similar and are usually represented by a sinusoidal curve for sound mathematical reasons.

When you allow two waves to combine to form a standing wave a graph of your 'varying' property against time shows a straight line parallel to the x axis. The property does not vary with time or the wave is time independant.

A graph plotted against position shows the characteristic node/antinode sequence.

Understanding this goes back to your question about phase.

If we define the phase-difference between two spatial points as

'the time difference when our varying quantity reaches its maximum'

you can see this is zero for a standing wave.
All points in the wave reach their maximum simultaneously, at least between any two nodes.

Most textbooks omit to emphasise that the illustrations they draw for traveling waves plot time on the x axis, but when they illustrate standing waves they are plotting distance. They often place the two graphs in juxtaposition, when they are not really directly comparable.
 
  • #57
If i were to address the issue using words I might then be able to imagine the graph.

What is going on in any constructive interferece is as follows: the amplitude of the two propagating waves combine to form maxima and minima. These new amplitudes, assuming the waves have the same amplitude will be double. This means that if we assume time along the x axis, it should take double as long to complete a stage in the wave than it would do with our propagating wave.
This means that if it took 0.1 second to complete each of our individual propagating waves, the length of time between each wave in our standing wave would be 0.2.

Obviousley there is not really a concept of time with a standing wave as the standing wave remains stationary so if we assume time as the distance between the beginning of one wave and the beginning of the next on both graphs, our standing wave would have a 'distance' of double the propgating wave

How's that as an explanation?
 
  • #58
On a slight tangent:

http://s359.photobucket.com/albums/oo40/jsmith613/?action=view&current=Long.png

I am writing my notes for physics and came across this diagram telling me what the amplitude for a longitudinal wave is. From the equillibrium position to apparently the next point along (see where blue arrow points to and ends). Surley the displacement is the distance between an area of compression and an area of rarefaction divide by 2

OR does amplitude vary continuosley on a longitdinal wave. Is it actually the maximum displacement of each point on a wave from the equillibrium (in the diagram this is the distance between each line on the wave and the nearest equillibrium point)
 
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  • #59
How's that as an explanation?

Puzzling.

This means that if we assume time along the x axis, it should take double as long to complete a stage in the wave than it would do with our propagating wave.
This means that if it took 0.1 second to complete each of our individual propagating waves, the length of time between each wave in our standing wave would be 0.2.

A standing wave has no period - it is time independent.

It does however have a wavelength, equal to twice the distance between adjacent nodes.

What is going on in any constructive interferece is as follows: the amplitude of the two propagating waves combine to form maxima and minima. These new amplitudes, assuming the waves have the same amplitude will be double.

Only if the two waves are in phase and going in the same direction.

came across this diagram

Can you name any real world waves that actually look like this?
What happens in the white space above and below your diagram?
 
  • #60
Studiot said:
Puzzling.

Can you name any real world waves that actually look like this?
What happens in the white space above and below your diagram?

this diagram was in my physics textbook but poorley explained. I don't know exactly what it is on about but know that I ought to know it - the book is officialy endorsed by edexcel

I would presume the what space in between the diagram was between the waves like in a slinkey

ignore the spaces above and below!
 
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  • #61
jsmith613 said:
On a slight tangent:

http://s359.photobucket.com/albums/oo40/jsmith613/?action=view&current=Long.png
Surley the displacement is the distance between an area of compression and an area of rarefaction divide by 2
This is wrong. The distance between compression regions and rarefaction regions is a quarter wavelength, whatever the amplitude (maximum displacement) of a wave.
In a 'real' compression wave, like sound, the actual displacement is a small fraction of a wavelength. A set of equally spaced vertical lines could be used to show the rest positions of small regions of air (/medium) and the displacement from those lines would be hardly visible. As you can plot a variable on any axis you like, you can just as easily show the displacement using an axis at right angles to the direction of propagation - and use whatever scale factor (gain) you want to show the way the displacement varies. So a longitudinal wave can just as easily be represented by a 'wiggly' line. Or it can be shown as varying shades of grey / colour, the darkest representing high pressure and the lightest, low pressure. I think there is a lot of needless confusion about this but XY graphs are usually chosen to represent most relationships between variables because they are easy to plot onto and to read off data.
 
  • #62
waves like in a slinkey

Good comment.

How about the rest?
 
  • #63
Studiot said:
Good comment.

How about the rest?

you mean the other types of waves?
 
  • #64
sophiecentaur said:
This is wrong. The distance between compression regions and rarefaction regions is a quarter wavelength, whatever the amplitude (maximum displacement) of a wave.

if the wavelength of a wave is between two compression / rarefaction regions then logically it is half not a quarter

compression rarefaction compression
(0)---------- (50) --------------(100)

on the bottom (0), (50), (100) i show the percentage of a wave that has passed at each point.

SC your argument is that

compression rarefaction compression rarefaction compression
(0) -------- (25)------- (50) ------- (75)---------- (100)
is that we pass through two complete compression regions (and begin our third) to complete a single wave?

What?? surely this is wrong?

IGNORE the --- this just allows me to place the correct bracket under the correct term
 
  • #65
Originally Posted by Studiot
Good comment.

How about the rest?

you mean the other types of waves?

I mean my other comments in post#59
 
  • #66
Studiot said:
I mean my other comments in post#59

How's that as an explanation?
Puzzling.
How do you mean, puzzling?
Is it wrong or just gramatticaly confusing?

A standing wave has no period - it is time independent.

It does however have a wavelength, equal to twice the distance between adjacent nodes.
when we say wavelength I presume we are accounting for amplitude (y axis) as opposed to what ever appears on the x axis, because we are discounting time!

Only if the two waves are in phase and going in the same direction.
So deconstructive inteference would occur even when waves are 1 degree out of phase.

Can you name any real world waves that actually look like this?
What happens in the white space above and below your diagram?
I believe i tackled this - the real world wave is like a slinky

the white space above and below the diagram should be ignored it has no relevance. We are only interested in the white space in between each wave front
 
  • #67
jsmith613 said:
if the wavelength of a wave is between two compression / rarefaction regions then logically it is half not a quarter

compression rarefaction compression
(0)---------- (50) --------------(100)

on the bottom (0), (50), (100) i show the percentage of a wave that has passed at each point.

SC your argument is that

compression rarefaction compression rarefaction compression
(0) -------- (25)------- (50) ------- (75)---------- (100)
is that we pass through two complete compression regions (and begin our third) to complete a single wave?

What?? surely this is wrong?

IGNORE the --- this just allows me to place the correct bracket under the correct term

Yes -totally correct. I didn't re-read what I'd written. I was, I guess, thinking in terms of potential energy rather than the sign of the pressure difference.
My comment that the wavelength is not related to the amplitude of the compression / displacement / velocity still holds, though. It's only because of the attempt to depict both displacement and displacement on the same axis that any confusion can arise. Who (in any other circumstances) would think of trying to draw a graph on just one dimension when two dimensions are available to display the information? And, if people can't use graphs to aid understanding then they have no chance of getting this process clear in their heads, I fear.

And your comment about defining wavelength by "discounting time". If a train is going past you, you would not say that its speed is altering the distance between the fronts of successive coaches, would you? (Ignore special relativity). You take a snapshot and measure it with a ruler. WaveLENGTH will have the dimension of length, surely, so why bring in the concept of time? The two variables are 'separable', as they say. This just adds confusion to people who are already confused.

There is little point, either, in complaining about naff diagrams in textbooks. You can find one of those in almost every chapter of most schoolbooks! They were sketched by an original author and then messed about with by a graphic designer and then copied into future textbooks without the information being processed by the brains of future authors.
 
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  • #68
"So deconstructive inteference would occur even when waves are 1 degree out of phase.
"
The relative phases of the two waves is different over all distances so, for "one degree out of phase" in one place will mean that you have zero phase difference somewhere else. The resulting interference pattern will just be shifted a bit.
 
  • #69
A =A0 cos(wt-kx)
I wrote this earlier in the thread. It describes a simple harmonic wave perfectly and it beats me why there needs to be any extra arm-waving discussion of the message of that simple equation. 'A' can be any of the variables in a wave and it can be 'in any direction'. If anyone needs answers, then just feed the numbers in and you will get them. Add two (or several) of these together and you will get a value for total A at anywhere in space or time. Modify A, a bit, to take into account spreading or attenuation of waves and you will also get an accurate answer for the resultant.
Just give the Maths a chance.
 
  • #70
The relative phases of the two waves is different over all distances so, for "one degree out of phase" in one place will mean that you have zero phase difference somewhere else. The resulting interference pattern will just be shifted a bit.

Would you like to rethink this?

For simplicity any two waves will add to provide a compound wave.

Special things happen if

1) The waves are of the same frequency or one frequency is a whole number multiple of the other.

2) The waves are going in the same direction. This is how you can double the amplitude by adding waves. You cannot create a standing wave this way. This is also how to obtain constructive /destructive interference.

3) The waves are going in opposite directions. This is how to create a standing wave.

All this has already been discussed in previous posts.
 
  • #71
This has got to be just another misunderstanding. the forward and reflected wave vary in relative phase from in-phase to anti-phase as you look at different points along the standing wave. This is why the resultant amplitudes vary from zero to double value.
I could suggest thinking of two phasors, their relative angles steadily changing (in opposite senses) as you look at points along the 'string'.
If you change the phase of one of the waves - say by using a delay at the reflection, then everything is the same except for the precise places where the anti and in phase conditions apply.

This thread has discussed many scenarios and I have assumed that the main discussion is about the formation of a standing wave when a reflection occurs - i.e. two waves of the same frequency are traveling towards each other. In that situation, my statement must be true, surely? In which way is it not?
Do you object to my use of the term 'interference pattern'?
 
  • #72
sophiecentaur said:
This thread has discussed many scenarios and I have assumed that the main discussion is about the formation of a standing wave when a reflection occurs - i.e. two waves of the same frequency are traveling towards each other. In that situation, my statement must be true, surely? In which way is it not?
Do you object to my use of the term 'interference pattern'?

I think the confusion may be as follows:
- the main topic is about standing waves BUT we have been side-tracked. It may be that the confusion is between two waves that are moving in the same direction and are 1 degree out of phase (and remain this way) v.s waves that are traveling in opposite directions
 
  • #73
Ah yes.
The resultant would be the same in amplitude over all distances 2A Cos(1 degree). A very 'long standing wave'.
 
  • #74
sophiecentaur said:
Ah yes.
The resultant would be the same in amplitude over all distances 2A Cos(1 degree). A very 'long standing wave'.

Now even I am confused!
If we have the standing wave, they would only be 1 degree out of phase at one point..

I was referring to two waves traveling in the same direction and superimposing where the phase difference was 1 degree.
Then would deconstructive interference occur or would it be defined as constructive
 
  • #75
Could you tell the difference by looking?
The con and des terms are only approximate, aren't they? Certainly only useful for arm waving or, sometimes, for finding a minimum / null in interferometry etc.. What is really relevant is the actual value.
If they are from non-coincident sources you would, in fact, be producing a two slits interference pattern.
 
  • #76
sophiecentaur said:
Could you tell the difference by looking?
The con and des terms are only approximate, aren't they? Certainly only useful for arm waving or, sometimes, for finding a minimum / null in interferometry etc.. What is really relevant is the actual value.
If they are from non-coincident sources you would, in fact, be producing a two slits interference pattern.

surely in an ideal situation (such as an exam question - which is one of the things I am working towards) they may ask the basic question
"Wave A and B are 10 degrees out of phase. When they superimpose would we get a constructive or deconsrtuctive interferance pattern. Explain"

In this case would the following answer suffice
"They would interfere constuctivley as the total displacement is greater than that of both individual waves".



Maybe i was confusing myself by using the value 1 degree. It would actually ONLY make sense if deconstructive intferferene took place at 180 degrees out of phase, right?

Reason being that this is the only stage where maximum displacement is less than that of either / both waves individually?
 
  • #77
Any decent Science exam question would really not concern itself with such semantic ideas. If it were to ask you what the value of the resultant was, you should be able to work it out with a simple vector triangle and get full marks. If you were at too low a level of knowledge then an appropriate question wouldn't introduce the phase value.
You seem determined to keep this topic at a 'conversational' level when, as I have remarked twice already, the Maths say it all and, at your level, that's what would count. It really is the only way forward. I have never come across any question on the lines of your proposed one - for a start, what could be the marking scheme?
All one can say, conversationally, is that the maximum is for zero phase difference and the deepest part of a null is when they are in antiphase - but we all knew that even before this thread started.
 
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