Wave Confluence: Ship & Radiotowers (Check Needed)

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Homework Help Overview

The problem involves a ship receiving radio signals from two towers, with a focus on wave interference and the calculation of wavelength based on the distances involved. The context includes concepts of constructive and destructive interference as the waves interact at specific points.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the calculation of distances from the towers to the points of interest and how these relate to the conditions for constructive and destructive interference. There is exploration of the implications of the waves being in phase at one point and how that affects the results at another point.

Discussion Status

Some participants have identified errors in their calculations and are revisiting their reasoning. There is an ongoing exploration of the relationship between phase differences and interference patterns, with some guidance provided on the implications of phase shifts.

Contextual Notes

Participants are navigating the complexities of wave interference, including the significance of the distances involved and the conditions for minima and maxima in wave patterns. There is mention of potential confusion regarding the application of formulas in different scenarios of wave phase relationships.

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Homework Statement


A ship floats across the coat, at a distance d = 600 m from it. The radio of the ship receives simultaneously signals of the same frequency from RadioTowers A & B, which are L = 800 m apart. At Point G (Γ), the two waves confluent in a strengthening way, where G's (Γ) distances from A & B are the same (rA = rB). At point D (Δ), which is right across B, the signal reaches its First Minimum. Find the wavelength λ.

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Homework Equations



Δr = n*λ , n = 0,1,2,3... (Strengthening-A'=2)
Δr = n*(λ/2), n = 1,3,5... (Weakening-A'=0)

The Attempt at a Solution



When the book says "First Minimum arrives at..." in every case it means Δr = n*λ/2 with n = 1. So i went ahead and found rA & rB for Δ through the forming triangles, put them in the above formula and got λ = 140 m. Which is wrong. I kinda figured that since I didn't use the stuff for Γ, but anyway. I turned back and saw that the answer was λ = 800 m. Which is a pretty big number.

So I thoughout of it this way: The signals arrive at Γ, the composite wave starts the way a y = Asin(...) wave would (no Initial Phase so it goes from "zero" to +A and then back down) and at Δ it's where the composite wave reaches the "horizontal axis" again, ie it covers λ/2 in length. Through that and the info about Γ (used the rs to find ΑΓ = ΓΒ = 400 m) I did λ/2 = 400 m <=> λ = 800 m

Now the result is correct, but I have no idea if the whole thing has any logic behind it. I was just trying stuff until I got the correct result. I mean, in every exercise thus far "First Minimum" just means Δr = λ/2.

Any help is appreciated!
 
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Darthkostis said:
found rA & rB for Δ through the forming triangles, put them in the above formula, Δr = n*λ/2
It's not clear to me what you did, but it does not sound right. Please post the details.
 
haruspex said:
It's not clear to me what you did, but it does not sound right. Please post the details.
Yeah, I checked it again this morning and figured out my mistake. I messed up on the Pythagorean Theorem. But to break this down:

At Δ we have the "First Minimum", so the signals that arrive from A & B there are out of phase, and result in the Amplitude A of the combined wave being 0. Thus, Δr = n*λ/2, in regards to Δ. But it's the 1st Minimum, so n = 1. Now I need to find rA & rB, or ΑΔ & ΒΔ. ΒΔ is d = 600 m. For ΑΔ we construct the triangle with ΑΔ as the hypotenouse, as seen here:

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So, ΑΔ = sqrt(L2 + d2) = sqrt(8002 m2 + 6002 m2) = 1000 m

Now we have Δr = |rA - rB| = | 1000 m - 600 m | = 400 m = 1*λ/2 <=> λ = 800 m

And that's it. I messed up the Pythagorean at first and then everything spiralled from there. I still have a question though: Why tell me that in Γ the two waves confluent in a strengthening way/A' = 2A? I didn't use it anywhere. Couldn't it have just given me the info about Δ?
 
Darthkostis said:
Why tell me that in Γ the two waves confluent in a strengthening way
Because that tells you that the transmissions are in phase. E.g. if there were 180 degrees out of phase then it would have been destructive interference at Γ and reinforcing at Δ.
 
haruspex said:
Because that tells you that the transmissions are in phase. E.g. if there were 180 degrees out of phase then it would have been destructive interference at Γ and reinforcing at Δ.
I figured as much, but I wasn't sure if it was hiding something else. Just to recap though: Because they arrive at the same time and I know that ΑΓ = ΓΒ, that means they're in phase. Otherwise, I'd get a different result. And thus when I go to Δ and find that Δr = n*λ/2, I don't have to factor any phase differences. Got it.

I have a question though: Doesn't the Δr = ...λ/... give me my answer already? If for example I was given the distance of Δ from Α & Β, plus λ. But I didn't know the confluence there. Then say I just put Δr & λ in both formulas, and for argument's sake, let's say that there was a reinforced interference at Δ (so Δr = n*λ). Would I be able to deduce whether the waves are out of phase or not?

There is an exercise example in my book, where there are there are two speakers. A receiver stands in such a way that the 1st Minimum arrives there, so Δr = λ/2. Then, in the "what if" section, it says that if the waves had a phase difference of λ/2, and due to them being placed in such a way that Δr, in regards to the receiver's position, equals λ/2. So that means that at the receiver the two waves have areinforced interference.

I get that on a theoretical level, but how would that work on a problem? Which formula would I use? Δr = nλ/2 or Δr = nλ? Technically it's the first one, but according to it there should be a destructive interference, which isn't true. Are there any other formulas to use in circumstances where the waves are not in phase? I seem to remember something like that from High School, but my book doesn't have anything. I get the theory part, but don't know how to "work" this in problems.
 
Darthkostis said:
A receiver stands in such a way that the 1st Minimum arrives there, so Δr = λ/2.
Only if they were emitted in phase.
In general, 2πΔr/λ tells you the phase shift. This has to be added to whatever the initial phase difference was.
 
haruspex said:
Only if they were emitted in phase.
In general, 2πΔr/λ tells you the phase shift. This has to be added to whatever the initial phase difference was.
Ah yeah, now I'm starting to remember. Any link to where I can read about that? Wikipedia is pretty unreliable. It seems my book has only the "in phase" occurances, and I'm afraid I'm not learning all that properly.
 

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