Antennas causing destructive interference

In summary: The phase difference of 4.5λ correspond to 4.5 full cycles around the circle, so after 1 full cycle, there are 4.5/(2π) cycles.= 0.7168 cycles.The total distance travelled is 0.7168*2π*200m = 900.9m, which is also the magnitude of the circle centre A and radius 200m. So the point on the circle above is 900.9m from A along the line perpendicular to AB.In summary, two radio antennas radiating in phase, with a frequency of 5.80MHz, are located at
  • #1
PirateFan308
94
0

Homework Statement


Two radio antennas radiating in phase are located at points A and B, 200m apart. The radio waves have a frequency of 5.80MHz. A radio receiver is moved out from point B along a line perpendicular to the line connecting A and B.

At what distances from B will there be destructive interference? (Note: The distance of the receiver from the sources is not large in comparison to the separation of the sources, so equation [itex]dsin\theta = (m+0.5)λ[/itex] does not apply.)



The Attempt at a Solution


I tried looking at the difference in path lengths separately, because I know that for destructive interference to occur, (m+1/2)λ=Δray length.

I drew a right angle triangle, where one side was 200m, the other side was r2 and the hypotenuse was r1. I said that θ was the angle between the 200m and r1. So then:
[itex]r_1=200tanθ,~~ r_2=\frac{200}{cosθ}

~~~~~Δr = 200 \frac{sinθ-1}{cosθ} = (m+1/2)λ[/itex]

But I can't figure out how to solve this equation, nor can I see another way to solve this problem. Thanks!
 
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  • #2
PirateFan308 said:

Homework Statement


Two radio antennas radiating in phase are located at points A and B, 200m apart. The radio waves have a frequency of 5.80MHz. A radio receiver is moved out from point B along a line perpendicular to the line connecting A and B.

At what distances from B will there be destructive interference? (Note: The distance of the receiver from the sources is not large in comparison to the separation of the sources, so equation [itex]dsin\theta = (m+0.5)λ[/itex] does not apply.)



The Attempt at a Solution


I tried looking at the difference in path lengths separately, because I know that for destructive interference to occur, (m+1/2)λ=Δray length.

I drew a right angle triangle, where one side was 200m, the other side was r2 and the hypotenuse was r1. I said that θ was the angle between the 200m and r1. So then:
[itex]r_1=200tanθ,~~ r_2=\frac{200}{cosθ}

~~~~~Δr = 200 \frac{sinθ-1}{cosθ} = (m+1/2)λ[/itex]

But I can't figure out how to solve this equation, nor can I see another way to solve this problem. Thanks!

The first thing I would have calculated is the wavelength of these radio waves, and thus how many wavelengths the separation (200m) represents. That is the maximum path difference possible.
That will show you how many points exist where there is destructive interference.
 
  • #3
[itex]\lambda = \frac{c}{f} = \frac{3.0*10^8}{5.80*10^6} = 51.7m[/itex]
So the separation represents 3.86 wavelengths, meaning there will be a maximum of 3 path differences.

As I was thinking further, I drew another right triangle with the distance between the sources being 200m, the hypotenuse being r1 and the other side being r2. If I put r2=x, then [itex] r_1 = \sqrt{x^2+200^2} [/itex] so i could solve as follows:

[itex] \sqrt{x^2+200^2}-x=(m+1/2)λ[/itex]

[itex]x^2+40000 = (m+1/2)^2(1/2*51.7m)^2+(m+1/2)(51.7m)x + x^2[/itex]

[itex]x=\frac{40000-(m+1/2)^2(25.86)^2}{(m+1/2)(51.7)}[/itex]

for m=0,

[itex]x=\frac{40000-(0+1/2)^2(25.86)^2}{(0+1/2)(51.7)} = 1540m[/itex]

for m=1,

[itex]x=\frac{40000-(1+1/2)^2(25.86)^2}{(1+1/2)(51.7)} = 496.4m[/itex]

for m=2,

[itex]x=\frac{40000-(2+1/2)^2(25.86)^2}{(2+1/2)(51.7)} = 277.1m[/itex]

for m=3,

[itex]x=\frac{40000-(3+1/2)^2(25.86)^2}{(3+1/2)(51.7)} = 175.78m[/itex]

form m=4, x=113.7. For m=5, x=69.53. For m=6, x=34.95. For m=7, x=6.15. For m=8, x=-18.9.

So the idea that I would only have 3 destructive interference spots doesn't line up with this. But I'm not sure where I made the mistake.
 
  • #4
PirateFan308 said:
[itex]\lambda = \frac{c}{f} = \frac{3.0*10^8}{5.80*10^6} = 51.7m[/itex]
So the separation represents 3.86 wavelengths, meaning there will be a maximum of 3 path differences.

As I was thinking further, I drew another right triangle with the distance between the sources being 200m, the hypotenuse being r1 and the other side being r2. If I put r2=x, then [itex] r_1 = \sqrt{x^2+200^2} [/itex] so i could solve as follows:

[itex] \sqrt{x^2+200^2}-x=(m+1/2)λ[/itex]

[itex]x^2+40000 = (m+1/2)^2(1/2*51.7m)^2+(m+1/2)(51.7m)x + x^2[/itex]

[itex]x=\frac{40000-(m+1/2)^2(25.86)^2}{(m+1/2)(51.7)}[/itex]

for m=0,

[itex]x=\frac{40000-(0+1/2)^2(25.86)^2}{(0+1/2)(51.7)} = 1540m[/itex]

for m=1,

[itex]x=\frac{40000-(1+1/2)^2(25.86)^2}{(1+1/2)(51.7)} = 496.4m[/itex]

for m=2,

[itex]x=\frac{40000-(2+1/2)^2(25.86)^2}{(2+1/2)(51.7)} = 277.1m[/itex]

for m=3,

[itex]x=\frac{40000-(3+1/2)^2(25.86)^2}{(3+1/2)(51.7)} = 175.78m[/itex]

form m=4, x=113.7. For m=5, x=69.53. For m=6, x=34.95. For m=7, x=6.15. For m=8, x=-18.9.

So the idea that I would only have 3 destructive interference spots doesn't line up with this. But I'm not sure where I made the mistake.

Potentially, destructive interference occurs at (m+1/2)λ as you said

That predicts 0.5λ, 1.5λ, 2.5λ, 3.5λ, 4.5λ, 5.5λ, etc

You calculated the maximum path difference [separation] = 3.86λ so any from the list that are less than that are possible.

0.5λ, 1.5λ, 2.5λ, 3.5λ

So you should have expected 4 points, not just 3. I think your following mathematics prompted that too.

EDIT: sorry for the delay in response - time zone problems; I am in Australia.
 
  • #5
PeterO said:
Potentially, destructive interference occurs at (m+1/2)λ as you said

That predicts 0.5λ, 1.5λ, 2.5λ, 3.5λ, 4.5λ, 5.5λ, etc

You calculated the maximum path difference [separation] = 3.86λ so any from the list that are less than that are possible.

0.5λ, 1.5λ, 2.5λ, 3.5λ

So you should have expected 4 points, not just 3. I think your following mathematics prompted that too.

EDIT: sorry for the delay in response - time zone problems; I am in Australia.

No worries - thank you for your help!

I first tried answering with 34.94,69.53,113.7,175.78 before I realized that was the distance less than 200m rather than the correct m≤3. Next, I tried answering 175.78,277.1,496.4,1540 and this was also wrong, but I can't find any errors in my computation.
 
  • #6
PirateFan308 said:
No worries - thank you for your help!

I first tried answering with 34.94,69.53,113.7,175.78 before I realized that was the distance less than 200m rather than the correct m≤3. Next, I tried answering 175.78,277.1,496.4,1540 and this was also wrong, but I can't find any errors in my computation.

In the second lne of your working (copied crudely here)

x2+40000=(m+1/2)2(1/2∗51.7m)2+(m+1/2)(51.7m)x+x2

You have halved the wavlength, while the formula you were using had the 1/2 with the m rather than with the λ. Perhaps I am mis-reading something?
 
  • #7
PirateFan308 said:
No worries - thank you for your help!

I first tried answering with 34.94,69.53,113.7,175.78 before I realized that was the distance less than 200m rather than the correct m≤3. Next, I tried answering 175.78,277.1,496.4,1540 and this was also wrong, but I can't find any errors in my computation.

An interesting way to get the answers would be:

Instead of starting with directions perpendicular to the line joining A & B, find the places on a circle created with A as the centre and radius 200m

Lets go for the point where m = 3, the path difference is 3.5 * 51.7 ≈ 181

The chord length from B must be 200 - 181 = 19

From that you can find the angle to the destructive interference point.

Now look at the perpendicular direction, and use trigonometry [tangent function actually], along with the angle you have calculate above, to compute the distance from B along the perpendicular.

Repeat for the other 3 path differences.
 
  • #8
PeterO said:
In the second lne of your working (copied crudely here)

x2+40000=(m+1/2)2(1/2∗51.7m)2+(m+1/2)(51.7m)x+x2

You have halved the wavlength, while the formula you were using had the 1/2 with the m rather than with the λ. Perhaps I am mis-reading something?

You're right, for some reason I plugged in half λ. It should have been [itex]x^2+40000 = (m+1/2)^2λ^2+2(m+1/2)λx+x^2[/itex] which would reduce to [itex]x=\frac{40000-(m+1/2)^2λ^2}{2(m+1/2)λ}[/itex]. Thank you so much! You were a huge help!
 

Related to Antennas causing destructive interference

1. What is destructive interference?

Destructive interference is the phenomenon that occurs when two or more waves meet and their amplitudes cancel each other out, resulting in a decrease in overall intensity or amplitude. This can happen with any type of wave, including electromagnetic waves such as those used in antennas.

2. How do antennas cause destructive interference?

Antennas can cause destructive interference when they are placed too close together or are broadcasting on the same frequency. This can create overlapping waves that cancel each other out, resulting in a weaker signal or loss of signal in certain areas.

3. Can destructive interference be prevented?

Yes, destructive interference can be prevented by properly spacing antennas and using different frequencies for broadcasting. This ensures that the waves do not overlap and cancel each other out, resulting in a stronger and more reliable signal.

4. How does destructive interference affect wireless communication?

Destructive interference can greatly affect wireless communication by causing a weaker or lost signal, resulting in dropped calls, slow internet speeds, and other communication issues. This is why it is important for antennas to be properly placed and spaced to prevent interference.

5. Is destructive interference always a bad thing?

Not necessarily. In some cases, destructive interference can be intentionally used to cancel out unwanted signals or noise, resulting in a clearer and stronger signal. However, in most cases, it is undesirable and steps should be taken to prevent it from occurring in wireless communication systems.

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