Confused about interefence patterns

In summary, "Confused about interference patterns" discusses the complexities and variations in interference patterns observed in wave interactions, particularly focusing on constructive and destructive interference. It emphasizes the importance of understanding wave behavior, phase differences, and the conditions under which these patterns occur, often illustrated through examples such as light and sound waves. The piece aims to clarify common misconceptions and provide insights into the underlying physics driving these phenomena.
  • #1
sdfsfasdfasf
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Homework Statement
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Relevant Equations
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I am confued with what is meant when it says "about the line AB", does this mean horizontally or vertically? The question states that the sources produce vertically polarised microwaves (I know this is relavant) and I also know that waves moving in different planes cannot interfere. Does it mean that X is rotated "towards us" and then the full rotation has X facing backwards, "to the left"? If so, how can there be a pattern at 180 degrees as X isnt facing the detector?
Sorry if it sounds like im being stupid, I am really confused.

Thank you.
 
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  • #2
I think it means that line AB and transmitter X stay fixed in the plane of the screen while detector Y is raised and rotated above the plane of the screen keeping the distance X-Y constant. At 90°, Y is directly above X and the line joining Y and X is perpendicular to the screen. At 180°, Y is back in the plane of the screen but on the other side of X (above the words "student connects" in the figure.)
 
  • #3
I'd take "rotated about the line AB" to mean that AB is the axis of rotation. You (the OP) are describing rotation about a line perpendicular to the plane of the page.
 
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  • #4
vela said:
I'd take "rotated about the line AB" to mean that AB is the axis of rotation. You (the OP) are describing rotation about a line perpendicular to the plane of the page.
Does your answer agree with kurumans answer?
 
  • #5
Obviously not. He's talking about moving transmitter (not detector) Y. I'm saying Y and D don't move and X rotates about its axis.
 
  • #6
vela said:
Obviously not. He's talking about moving transmitter (not detector) Y. I'm saying Y and D don't move and X rotates about its axis.
I am struggling to visusalise what you mean when you say rotate about its axis, can you draw a picture please?
 
  • #7
sdfsfasdfasf said:
I am struggling to visusalise what you mean when you say rotate about its axis, can you draw a picture please?
Suppose that at first the polarisation of waves from X is in the plane of the page.
Imagine an ant looking at X from B. In the diagram as shown, we are looking down on the top of the ant. The ant sees the polarisation as horizontal.
If we rotate the transmitter about line AB then the ant sees the polarisation as rotating. After 180° it is horizontal again. The face marked X is now at the bottom, facing away from us.
The transmitter points at B at all times.
 
  • #8
If im understanding correctly after 180 degrees the waves emitted are "upside down" so the maxima / minima are reversed on the intereference pattern?
 
  • #9
After rotation by 180 degrees the plane of polarization is the same as before the rotation. There is no upside down. The electric field vector oscillates in the polarization plane, is not a constant vector. Only the orientation of the plane matters.
 
  • #10
nasu said:
After rotation by 180 degrees the plane of polarization is the same as before the rotation. There is no upside down. The electric field vector oscillates in the polarization plane, is not a constant vector. Only the orientation of the plane matters.
Ok, do the maxmima / minima flip? If so why?
 
  • #11
sdfsfasdfasf said:
Ok, do the maxmima / minima flip? If so why?
We often explain interference of two EM waves by considering vector addition of the waves’ electric fields (say ##\vec {E_1}## and ##\vec {E_2}##) at the same time and place.

For vertically polarised waves, we get constructive interference where ##\vec {E_1}## and ##\vec {E_2}## always point in the same direction: both point up during the same half-cycle and both point down during the other half-cycle.

We get destructive interference at places where ##\vec {E_1}## and ##\vec {E_2}## always point in opposite directions: during the half-cylce when##\vec {E_1}## points up, ##\vec {E_2}## points down and vice versa for the other half-cycle.

Rotating transmitter X about AB by ##180^o## (i.e. turning X upside down) will reverse its field direction. That means what would have been an upwards field at some moment in time will now be a downwards field, and vice versa.

So, can you put that all together and answer your question?

Minor edits to improve wording.
 
Last edited:
  • #12
vela said:
Obviously not. He's talking about moving transmitter (not detector) Y. I'm saying Y and D don't move and X rotates about its axis.
Yes, I thought of this as a path-length difference experiment not as a polarization experiment. If it's a polarization experiment, one would have to assume that there is at least some signal in the starting configuration, i.e. there is no destructive interference to begin with. Then just rotating transmitter X about its axis leaving Y and D alone, would modulate the signal as explained by @Steve4Physics in post #11.

I think that rotating X and Y as one about AB (to avoid polarization effects) as described earlier and treating this as a path-length difference situation makes the answer to the question posed, "Describe and explain the observed patterns of maximum and minimum intensity", more interesting.

Below are plots of the path-length difference divided by the wavelength, ##\Delta L/\lambda## as a function of angle at fixed wavelength. Variable ##y## is the perpendicular distance of transmitter X to line PQ and ##d## is the constant separation between transmitters X and Y.

Interference is constructive at angles where ##N=\Delta L/\lambda## is an integer and destructive where it is a half-integer. The zeroth order maximum is at θ = 60° where it can be shown with a diagram and simple geometry that triangle XDY is isosceles.

Rotating interference.png
 
  • #13
Steve4Physics said:
We often explain interference of two EM waves by considering vector addition of the waves’ electric fields (say ##\vec {E_1}## and ##\vec {E_2}##) at the same time and place.

For vertically polarised waves, we get constructive interference where ##\vec {E_1}## and ##\vec {E_2}## always point in the same direction: both point up during the same half-cycle and both point down during the other half-cycle.

We get destructive interference at places where ##\vec {E_1}## and ##\vec {E_2}## always point in opposite directions: during the half-cylce when##\vec {E_1}## points up, ##\vec {E_2}## points down and vice versa for the other half-cycle.

Rotating transmitter X about AB by ##180^o## (i.e. turning X upside down) will reverse its field direction. That means what would have been an upwards field at some moment in time will now be a downwards field, and vice versa.

So, can you put that all together and answer your question?

Minor edits to improve wording.
Am I misreading something? As I read posts #8, #9 and #11, @nasu says @sdfsfasdfasf is wong to say a 180° rotation flips maxima and minima and you are saying post #8 is right.
 
  • #14
haruspex said:
Am I misreading something? As I read posts #8, #9 and #11, @nasu says @sdfsfasdfasf is wong to say a 180° rotation flips maxima and minima and you are saying post #8 is right.
Yes, I think the suggestion in post #8 is correct.

Turning X upside down (i.e. a ##180^o## rotation about AB) effectively introduces a phase-change of ##\pi## between the two signals. (Not the best analogy, but compare it to reversing the polarity of one of a pair of stereo loudspeakers.)

After X’s ##180^o## rotation about AB, X’s plane of polarisation is restored, but the direction of X’s electric field in this plane has been reversed.

Edit - typo'.
 
  • #15
As an A Level student we don't learn about the actual fields that make up an electromagnetic wave, but this makes enough sense to me, the anaolgy of a phase shift of pi makes the most sense. Thank you all
 
  • #16
sdfsfasdfasf said:
As an A Level student we don't learn about the actual fields that make up an electromagnetic wave, but this makes enough sense to me, the anaolgy of a phase shift of pi makes the most sense. Thank you all
Make sure you have carefully read and thought about what the question is asking.

For another mark, I'd guess that you are required to say what happens to the interefernce pattern (along PQ) when the angle of rotation of X about AB is ##90^0## ...
 
  • #17
Steve4Physics said:
Make sure you have carefully read and thought about what the question is asking.

For another mark, I'd guess that you are required to say what happens to the interefernce pattern (along PQ) when the angle of rotation of X about AB is ##90^0## ...
No interference
 
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FAQ: Confused about interefence patterns

What is an interference pattern?

An interference pattern is a pattern formed by the overlapping of two or more waves, resulting in regions of constructive interference (where waves add together) and destructive interference (where waves cancel each other out). This phenomenon is commonly observed in experiments involving light, sound, and water waves.

What causes interference patterns?

Interference patterns are caused by the superposition of waves. When two or more waves meet, they combine according to the principle of superposition, leading to areas of increased amplitude (constructive interference) and areas of decreased amplitude (destructive interference). The specific pattern depends on the wavelength, phase difference, and the geometry of the wave sources.

How do interference patterns differ between light and sound waves?

While both light and sound waves can create interference patterns, the mechanisms and observable effects differ. Light waves, which are electromagnetic, can produce visible patterns on surfaces (like in the double-slit experiment), while sound waves, which are mechanical, create variations in pressure that can be heard as changes in volume or pitch. Additionally, light interference patterns can be more easily observed due to their high speed and the ability to manipulate light with optics.

What is the double-slit experiment and how does it demonstrate interference?

The double-slit experiment involves shining a coherent light source (like a laser) through two closely spaced slits onto a screen. Instead of producing two distinct spots of light, the light creates a series of alternating bright and dark fringes on the screen, demonstrating interference. This experiment illustrates the wave nature of light and shows how waves can interfere with each other, leading to the characteristic pattern.

How can I observe interference patterns in everyday life?

Interference patterns can be observed in various everyday situations. Examples include the colorful patterns seen in soap bubbles or oil slicks on water, which arise from the interference of light waves reflecting off thin films. Additionally, you can observe sound interference when two speakers play the same sound at slightly different times, leading to areas of louder and softer sound in a room.

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