Ask your own question, for FREE!
Physics 11 Online
OpenStudy (abhisar):

Wave Help!

OpenStudy (abhisar):

@IrishBoy123

OpenStudy (abhisar):

I have seen in many textbooks stating that equation for a plane progressive wave is \[y=a \sin (kx-\omega t)\] if the wave is moving in +ve direction but in some books they say it is \[y=a \sin (\omega t -kx)\] Are these both same or different? @IrishBoy123 @Michele_Laino @ganeshie8

ganeshie8 (ganeshie8):

How can they be both same when \(\sin(x)\ne \sin(-x)\) ?

OpenStudy (irishboy123):

the first one is more orthodox as it's travelling to right from x = 0 so maybe also see if you can manipulate the second to get a phase difference. sin (π-x) = sin(-x)... rather than a backward moving which is what it looks like

OpenStudy (irishboy123):

but as a slight aside.... maybe! ....... anything in the form f(kx - wt) satisfies the wave equation as does, it would seem combinations thereof, including the negative version...... so they're all OK in that sense

OpenStudy (abhisar):

Yes, so they both represent travelling wave equation but they are not exact if taken in same sense. I'll have to follow any one way but I can't intermix them. Right?

OpenStudy (irishboy123):

you can mix them to see the interference pattern. that's one of the cool things about it!

OpenStudy (irishboy123):

https://www.desmos.com/calculator

OpenStudy (michele_laino):

here is my reasoning: we can write a plane wave in this form: \[\Large a\sin \left( {kx - \omega t} \right) = \Im \left\{ {a\exp i\left( {kx - \omega t} \right)} \right\}\] furthermore, we have: \[\Large \begin{gathered} \sin \left( {kx - \omega t + \pi } \right) = \sin \left( {kx - \omega t} \right) \cdot \left( { - 1} \right) = \hfill \\ \hfill \\ = - \sin \left( {kx - \omega t} \right) = \sin \left( {\omega t - kx} \right) \hfill \\ \end{gathered} \] therefore: \[\Large \begin{gathered} {\psi _1} = a\exp i\left( {\omega t - kx} \right) = a\exp i\left( {kx - \omega t} \right) \cdot \exp \left( {i\pi } \right) = \hfill \\ \hfill \\ = {\psi _2} \cdot \exp \left( {i\pi } \right) \hfill \\ \end{gathered} \] in other words the plane waves: \[\Large {\psi _1} = a\exp i\left( {\omega t - kx} \right),\quad {\psi _2} = a\exp i\left( {kx - \omega t} \right)\] differ each from other, by a constant phase factor, so, thanks to \(Ehrenfest\), such waves represent the same particle

OpenStudy (abhisar):

Yes! I get it now. Thank you @Michele_Laino @IrishBoy123 and @ganeshie8 !

Can't find your answer? Make a FREE account and ask your own questions, OR help others and earn volunteer hours!

Join our real-time social learning platform and learn together with your friends!
Can't find your answer? Make a FREE account and ask your own questions, OR help others and earn volunteer hours!

Join our real-time social learning platform and learn together with your friends!