One dimensional wave, function of a wave

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SUMMARY

The discussion centers on the function of a wave as described in 'Optics' by Eugene Hecht, specifically focusing on the equation ##\psi(x)=f(x-vt)##. This equation represents a wave traveling to the right, and its alternative form ##\psi(x,t)=g(t-\frac{x}{v})## is highlighted for its relevance in analyzing wave behavior over time. The conversation also references a specific homework problem from Physics Forums that illustrates the application of these concepts. Understanding these equations is crucial for grasping wave dynamics in physics.

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  • Understanding of wave functions and their mathematical representations
  • Familiarity with the concept of wave velocity and its implications
  • Basic knowledge of calculus, particularly in relation to functions of multiple variables
  • Experience with physics problems involving wave motion
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  • Study the implications of the wave equation ##\psi(x,t)=f(x-vt)## in different contexts
  • Explore the concept of wave propagation and its mathematical modeling
  • Analyze the homework problem referenced from Physics Forums for practical application
  • Learn about the relationship between wave functions and boundary conditions in physics
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Students of physics, educators teaching wave mechanics, and anyone interested in the mathematical modeling of wave phenomena will benefit from this discussion.

Taylor_1989
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I am currently reading through 'Optics' by Eugene Hecht chp 2 page 20, he talks about the function of the wave and the direction of travel of the wave i.e ##\psi(x)=f(x-t)## and right at the bottom of the page he say this:

Equation (2.5) is often expressed equivalently as some function of ##t - x/v)##, since,

$$f(x-vt)=F(-\frac{x-vt}{v})=F(t-\frac{x}{v})$$

What I am trying to understand is the relevance of this, because he make no mentioned to this again in the chapter nor dose he refer to it in any of the exercise at then end, and just curious to now when this type of format would be used?

edit: the equation 2.5 he is referring to is: ##\psi(x)=f(x-vt)##
 
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For a wave traveling to the right ## \psi(x,t)=f(x-vt) ##. If we have the form ##\psi(x,0)=f(x) ## at ## t=0 ##, we can find the form at any other time by taking ## \psi(x,t)=\psi(x-vt,0) =f(x-vt) ##. ## \\ ## Alternatively, and this is what he is referring to, if we have ## \psi(x,t) ## as a function of time at ## x=0 ##, which is ## \psi(0,t)=g(t) ##, if it is a traveling wave with velocity ## v ##, it obeys ## \psi(x,t)=g(t-\frac{x}{v}) ##.
 
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And if you want to see an application of this, try working this homework problem that appeared on Physics Forums about a year ago. The solution is in post 2, but you might see if you can work it yourself before looking at the solution. https://www.physicsforums.com/threads/reflection-of-em-wave.934953/ Also notice it fooled a couple of other people who tried to work the problem without using the concept of your post above.
 
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