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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.