How Do Different Equations Affect the Initial Direction of a Traveling Wave?

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The discussion focuses on how different wave equations influence the initial direction of a traveling wave. It highlights that the equations y=A sin(kx - ωt) and y=A sin(-kx - ωt) represent waves traveling to the right and left, respectively, with their initial vertical movements varying based on the amplitude's sign. Participants debate the implications of these equations on the wave's behavior at the origin, particularly how to determine whether the wave moves upwards or downwards at t=0. The conversation emphasizes that the amplitude's sign and the wave's phase shift are crucial in understanding the wave's initial direction. Ultimately, the direction of movement can be assessed by evaluating the derivative of the wave function at the origin.
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Homework Statement
This is not homework

I want to ask about equation of traveling wave. I read in my book the derivation of equation of traveling wave. The explanation starts from equation ##y=A \sin (kx)## then change into ##y=A \sin (kx - \omega t)## as the wave moves to the right. If the wave moves to the left, the term inside the sin would be ##(kx + \omega t)##
Relevant Equations
##y=A \sin (kx + \omega t)##

##y=A \sin (-kx - \omega t)##
But in the notes from teacher, the equation is ##y=A \sin (kx - \omega t)## for wave traveling to the right and ##y=A \sin (-kx - \omega t)## for wave traveling to the left

When I transform the equation of the wave traveling to the left using trigonometry:
$$y=A \sin (-kx - \omega t)$$
$$y=-A \sin (kx + \omega t)$$

The issue is in the practice question, there is question asking the initial direction of movement of the wave, will it move upwards or downwards. Equation ##y=A \sin (kx + \omega t)## states that the wave initially moves upwards but ##y=-A \sin (kx + \omega t)## states the wave moves downwards initially. It means that the answer to the question will differ, depends on which equation I use.

In this youtube video,
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There is another equation for wave traveling to the right, which is ##y=A \sin (\omega t - kx)## which is equal to ##y=-A \sin (kx - \omega t)##. This means that the initial vertical movement for wave traveling to the right will differ from two previous equations.

How to address the difference? Thanks
 
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A traveling sine wave should always look “identical”, just shifted in time and space. The value of the amplitude is irrelevant.
Look at sin(f(x,t)). It is “identical” for f(x,t)=constant.
For kx=±constant+ωt, as t increases, x increases⇒right going
For kx=±constant-ωt, as t increases, x decreases⇒left going
 
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songoku said:
The issue is in the practice question, there is question asking the initial direction of movement of the wave, will it move upwards or downwards.
How exactly does the question specify the wave? If it only tells you which way it is moving as a whole in respect of left/right you cannot tell whether it is moving up or down at the origin at t=0.
caz said:
A traveling sine wave should always look “identical”, just shifted in time and space. The value of the amplitude is irrelevant.
Look at sin(f(x,t)). It is “identical” for f(x,t)=constant.
For kx=±constant+ωt, as t increases, x increases⇒right going
For kx=±constant-ωt, as t increases, x decreases⇒left going
I don't think that's what you meant. If f(x,t)=constant then sin(f(x,t)) is a horizontal line. And kx=±constant+ωt doesn't work either, since those are necessarily independent variables.
How about, given sin(kx+ωt),
ω/k <0 moves right,
ω/k>0 moves left
ω/k=0 is static?

But none of that relates the question being asked in post #1.
 
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haruspex said:
How exactly does the question specify the wave? If it only tells you which way it is moving as a whole in respect of left/right you cannot tell whether it is moving up or down at the origin at t=0.

I don't think that's what you meant. If f(x,t)=constant then sin(f(x,t)) is a horizontal line. And kx=±constant+ωt doesn't work either, since those are necessarily independent variables.
How about, given sin(kx+ωt),
ω/k <0 moves right,
ω/k>0 moves left
ω/k=0 is static?

But none of that relates the question being asked in post #1.
I guess that I didn’t explain it clearly. Take a feature at time t0; there is an x0 associated with it. We now have an f(x0,t0) for that feature. At a later time, t1, the feature is at x1 at which point you can use the equations that I wrote to determine x1 and the direction of travel.
 
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caz said:
I guess that I didn’t explain it clearly. Take a feature at t0; there is an x0 associated with it. We now have an f(x0,t0) for that feature. At a later time, t1 the feature is at x1 at which point you can use the equations that I wrote to determine x1 amd the direction of travel.
So you did not intend specifically a sine function, you meant it to be general.
If f(x,t) is a traveling wave of some arbitrary shape described by y=g(x) and its horizontal motion is given by h(t) then f=g(x-h(t)).
 
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Ok, let me try to clean my comments up while sitting at a computer. Hopefully, third time is a charm. My apologies.

We have f(kx±ωt)=f(φ)
For a traveling wave, we are interested in the location xa of a specific φ0 at a time, ta.
So we set kxa±ωta0
So kxa0##\mp##ωta (1)

What happens to xa as ta increases for a specific φ0 in (1)?

For f(kx-ωt), xa increases (moves to the right); i.e., a right traveling wave.

For f(kx+ωt), xa decreases (moves to the left); i.e., a left traveling wave.
 
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Also the A is arbitrary in Asin(φ). You can write Asin(-φ)=-Asin(φ)=Bsin(φ) where B is arbitrary. Once you actually fit the parameter, things are determined uniquely.
 
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caz said:
Ok, let me try to clean my comments up while sitting at a computer. Hopefully, third time is a charm. My apologies.

We have f(kx±ωt)=f(φ)
For a traveling wave, we are interested in the location xa of a specific φ0 at a time, ta.
So we set kxa±ωta0
So kxa0##\mp##ωta (1)

What happens to xa as ta increases for a specific φ0 in (1)?

For f(kx-ωt), xa increases (moves to the right); i.e., a right traveling wave.

For f(kx+ωt), xa decreases (moves to the left); i.e., a left traveling wave.
Yes, I think that matches post #5, except that I allowed a generalised motion, not a constant velocity.
Anyway, as I wrote, this isn't relevant to the question in post #1. @songoku is concerned with the sign of ##\dot y## at (0, 0). The two forms of the basic equation cited effectively differ in terms of the sign of the amplitude, or, equivalently, a half wavelength shift in phase. These forms will yield opposite answers to the question posed.
I must say the usual form I'm aware of is ##A\sin(kx\pm \omega t)##, where all constants are assumed positive - or the same with an arbitrary phase shift, or with cos instead of sin. I'd never seen it given as ##A\sin(\omega t\pm kx)##.
 
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haruspex said:
Yes, I think that matches post #5, except that I allowed a generalised motion, not a constant velocity.
Anyway, as I wrote, this isn't relevant to the question in post #1. @songoku is concerned with the sign of ##\dot y## at (0, 0). The two forms of the basic equation cited effectively differ in terms of the sign of the amplitude, or, equivalently, a half wavelength shift in phase. These forms will yield opposite answers to the question posed.
I must say the usual form I'm aware of is ##A\sin(kx\pm \omega t)##, where all constants are assumed positive - or the same with an arbitrary phase shift, or with cos instead of sin. I'd never seen it given as ##A\sin(\omega t\pm kx)##.
They don’t give different answers. You pick up two negative signs which cancel. One from -A and one from -Φ when you take the derivative using the chain rule.

In your equations, the two A’s are not identical for a specific wave.
 
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  • #10
caz said:
They don’t give different answers. You pick up two negative signs which cancel. One from -A and one from -Φ when you take the derivative using the chain rule.
With ##y=A\sin(kx-\omega t)##, ##\dot y=-A\omega\cos(kx-\omega t)##. The sign of ##\dot y## at (0,0) depends on ##A\omega##. Change the sign of one only and the sign of ##\dot y## changes.
The two forms @songoku quotes effectively have opposite signs for A but the same ##\omega##, or you could view them as the same sign for A and opposite signs for both k and ##\omega##. Either way, they yield opposite signs for ##A\omega##.
 
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  • #11
You need to use the value kx=π/2 to fit A. Everything is uniquely defined. The sign of A is determined by whether you use φ or -φ. You cannot arbitrarily choose it.
 
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  • #12
caz said:
You need to use the value kx=π/2 to fit A. Everything is uniquely defined. The sign of A is determined by whether you use φ or -φ. You cannot arbitrarily choose it.
I would say A is, by convention, nearly always taken to be positive (likewise k and ##\omega##), but I was not suggesting flipping the sign of A. My observation was that the difference between the ##A\sin(kx-\omega t)## and ##A\sin(\omega t-kx)## forms is equivalent to flipping the sign of A and hence leads to opposite signs of ##\dot y(0,0)##.
 
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  • #13
haruspex said:
I would say A is, by convention, nearly always taken to be positive, but I was not suggesting flipping the sign of A. My observation was that the difference between the ##A\sin(kx-\omega t)## and ##A\sin(\omega t-kx)## forms is equivalent to flipping the sign of A and hence leads to opposite signs of ##\dot y(0,0)##.
A is arbitrary. Changing the functional form will change it’s value.
Without loss of generality we can write
Asin(kx-ωt) and Bsin(ωt-kx)
let t = 0.
assume the maximum occurs at x=π/2k
let the maximum value of the wave be C(a positive number)
then
Asin(π/2)=A=C
Bsin(-π/2)=-B=C; B=-C
You are not free to arbitrarily choose both signs. The data have a say in the matter.
 
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  • #14
caz said:
A is arbitrary. Changing the functional form will change it’s value.
Without loss of generality we can write
Asin(kx-ωt) and Bsin(ωt-kx)
let t = 0.
assume the maximum occurs at x=π/2k
let the maximum value of the wave be C(a positive number)
then
Asin(π/2)=A=C
Bsin(-π/2)=-B=C; B=-C
You are not free to arbitrarily choose both signs. The data have a say in the matter.
I think all we are arguing about is how to express the error in (or misleading nature of) the video.
If A is positive in the video the equation adduced does not much the picture at the start. There is a half wavelength phase shift.
Your view, then, is that to match the picture the video effectively makes A negative, so ##\dot y(0,0)=A\omega## is negative.
 
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  • #15
haruspex said:
How exactly does the question specify the wave? If it only tells you which way it is moving as a whole in respect of left/right you cannot tell whether it is moving up or down at the origin at t=0.
The question gives equation of traveling wave, something like ##y=3 \sin (-4x-5t)## then asks about the amplitude, frequency, wavelength, speed, direction of travel of wave (left or right), direction of movement of wave initially (up or down)
 
  • #16
songoku said:
The question gives equation of traveling wave, something like ##y=3 \sin (-4x-5t)## then asks about ... direction of movement of wave initially (up or down)
Direction of movement where, at the origin? Then it's simple. Evaluate ##\dot y(0,0)##.
 
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  • #17
haruspex said:
Direction of movement where, at the origin? Then it's simple. Evaluate ##\dot y(0,0)##.
You can also think about the answer. You have a left going wave. Look at the value of x that is a little bit greater than zero. That point will soon be at 0.
 
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  • #18
haruspex said:
Direction of movement where, at the origin? Then it's simple. Evaluate ##\dot y(0,0)##.
The question does not specify but I think it is at origin

caz said:
You can also think about the answer. You have a left going wave. Look at the value of x that is a little bit greater than zero. That point will soon be at 0.
You mean I put t = 0 and then some random value of x close to zero (e.g. 0.01 m) to the equation to get the sign of y? If y is positive, then the wave travels down. If y negative then the wave travels up?

Thanks
 
  • #19
For a transverse wave yes
haruspex said:
Direction of movement where, at the origin? Then it's simple. Evaluate y˙(0,0).
Why limit yourself to the origin? It will also be true at any x evaluate $$\dot f (x,t)\left. \right |_{t=0}$$
 
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  • #20
songoku said:
You mean I put t = 0 and then some random value of x close to zero (e.g. 0.01 m) to the equation to get the sign of y? If y is positive, then the wave travels down. If y negative then the wave travels up?

You have a left going wave. The wave to the right of you is positive negative. This means …
 
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  • #21
caz said:
You have a left going wave. The wave to the right of you is positive. This means …
Sorry I don't understand your hint
 
  • #22
hutchphd said:
For a transverse wave yes

Why limit yourself to the origin? It will also be true at any x evaluate $$\dot f (x,t)\left. \right |_{t=0}$$
At any time, parts of the wave will be moving one way in the transverse direction, parts the other.
 
  • #23
caz said:
The wave to the right of you is positive.
Not according to post #15.
 
  • #24
haruspex said:
Not according to post #15.
Corrected.
 
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  • #25
songoku said:
Sorry I don't understand your hint
A wave is coming towards a point. What does that mean for the point?
 
  • #26
caz said:
A wave is coming towards a point. What does that mean for the point?
The point will be disturbed so it will have same displacement as the wave
 
  • #27
Yes.
 
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  • #28
Thank you very much for the help and explanation caz, haruspex, hutchphd
 
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