Superposition of Waves - Standing Waves

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SUMMARY

The discussion focuses on the superposition of waves, specifically the formation of standing waves when a wave traveling in the negative x-direction reflects off a barrier. The equations provided include E_{1} = E_{0}sin(ωt + kx) and E_{2} = E_{0}sin(ωt - kx - θ_{R}), leading to the resultant wave E_{R} = 2E_{0}cos(kx + θ_{R}/2)sin(ωt - θ_{R}/2). A key point of confusion arises from the phase shift substitutions, particularly the transformation of sin(x - π/2) to -cos(x), which leads to a negative amplitude in the user's calculations. The correct interpretation of these phase shifts is essential for understanding the positive amplitude of standing waves.

PREREQUISITES
  • Understanding of wave equations and superposition principles
  • Familiarity with trigonometric identities, particularly sine and cosine transformations
  • Knowledge of phase shifts in wave mechanics
  • Basic concepts of standing waves and their formation
NEXT STEPS
  • Study the derivation of standing waves in detail using E_{R} = 2E_{0}sin(kx)cos(ωt)
  • Learn about phase shifts in wave functions and their implications in wave interference
  • Explore the application of trigonometric identities in wave mechanics
  • Investigate the effects of boundary conditions on wave reflection and standing wave formation
USEFUL FOR

Students of physics, particularly those studying wave mechanics, educators teaching wave phenomena, and anyone interested in the mathematical foundations of standing waves.

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Homework Statement



Consider a situation in which a wave is traveling in the negative x-direction encounters a barrier and is reflected. Assume an ideal situation in which none of the energy is lost on reflection nor absorbed by the transmitting medium. This permits us to write both waves with the same amplitude. I will represent these equations as

E_{1} = E_{0}sin(ωt + kx)
E_{2} = E_{0}sin(ωt - kx - θ_{R})

Here θ_{R} is included to account for possible phase shifts upon reflection. The resultant wave of the two waves can be represented as

E_{R} = E_{1} + E_{2} = E_{0}[sin(ωt + kx) + sin(ωt - kx - θ_{R})]

Next I make the substitution

β_{+} = ωt + kx and β_{+} = ωt - kx - θ_{R}

and employ the identity

sin(β_{+}) + sin(β_{-}) = 2sin(\frac{1}{2}(β_{+} + β_{-}))cos(\frac{1}{2}(β_{+} + β_{-}))

This yields

E_{R} = 2E_{0}cos(kx + \frac{θ_{R}}{2})sin(ωt - \frac{θ_{R}}{2})

Consider the situation in which a standing wave results when \frac{θ_{R}}{2} = \frac{∏}{2} and you get

E_{R} = 2E_{0}sin(kx)cos(ωt)

Homework Equations


The Attempt at a Solution



This is what my book claims. The only problem I have is that it looks like it made the substitution

sin(x - \frac{∏}{2}) = -cos(x) and cos(x - \frac{∏}{2}) = sin(x)

The problem is that when I make these substitutions I get

-2E_{0}sin(kx)cos(ωt)

I'm not exactly sure how it's supposed to be positive. Thanks for any help.
 
Physics news on Phys.org
if cos(x-pi/2) = sin(x), what does cos(x+pi/2) equal?
 
Oh wow. I can't believe I didn't see that thanks.
 

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