haruspex said:
You omitted this step:
"changing the sign of -Kx to +Kx to indicate change in direction (A sin(wt+Kx))"
Yes. At the time it I considered it a distraction from my point about changing the sign of ##y## being a fundamental error.
haruspex said:
It's a bit confusing because the standard procedure the OP quotes takes the original wave as ##y=A \sin (\omega t-kx)##, not ##y=A \sin (kx-\omega t)##.
Agreed. When the OP stated this ...
mrpurpletoes said:
i've been told the reflection of the wave y=A sin(wt-Kx) is y=-Asin(wt+Kx) which is obtained by:
- changing the sign of -Kx to +Kx to indicate change in direction (A sin(wt+Kx))
- then multiplying with -1 to indicate inversion of the wave
... as I believe has already been pointed out, it is not consistent with what he did.
mrpurpletoes said:
but when i follow these steps for the wave y=2 sin(4x-8t)
i get 2 sin(4x+8t)
Which side tracked the first four responses. It wasn't until your (fifth) response that it got straightened out.
And notice that after that the OP disappeared. Once he knew he'd made the right answer he lost interest.
For a physics instructor this is a major problem. Students are understandably interested in answer-making. After all, that's how their success in the course is measured. But instructors want students to instead be interested in sense-making, and that makes for a challenge. In this case the OP seems to have no interest in making sense of the situation, only in making the right answer.
This is why, in my opinion, if the statement of the problem is not given in the template, it's the first thing we should ask for before we start guiding the student towards an understanding of the physics involved in solving the problem.
Herman Trivilino said:
If a pulse of height ##y=2## reflects off a fixed end, the returning pulse does indeed have a height ##y=-2##. But to see that one has to wait for a time ##t## equal to one quarter of the wave's period.
haruspex said:
I don't see that. When the "in principle" wave height of 2 reaches the fixed point then, at that instant, the reflected wave must have height -2 at that point.
As an example, think about stretching a rope or the like, with one end attached to a hook in the wall and you holding the other end in your hand. You stretch the rope taut and "in principle" it has a height ##y=0## all along its length. Then you send a pulse of height ##y=2## towards the wall. When that pulse hits the wall, the value of ##y## at the wall is still zero. After all, that's what it means to have a fixed end. After reflection, the pulse has a height of ##y=-2## but that is not at the location of the wall. It
starts to form there, but it's not fully formed until after a time ##t## equal to one-fourth of the period, at a value of ##x## located one-fourth of a wavelength away from the wall. Of course, to even speak of a period and wavelength one must assume you will continue to send repeated pulses of the same height, equally spaced in time, so that the standing wave can be created.
Alternatively, you can attach the end of the rope, not to a hook, but to a vertical section of pipe attached to the wall, with a loop in the end of the rope so that it's free to slide up and down the pipe. Again, in principle, you've created not a fixed end but a free end. Now when the pulse hits the end of the rope the reflected pulse will not be inverted, and will be fully formed by the time it begins to return towards your hand.