Why is the Central Maximum Shifted Towards P? Ask Here!

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In summary: Now, if you know the total path length and the wavelength, you know how many peaks are in there. If you change the path length, you change the number of peaks (well, the fraction part of it) and thus the phase. And you know that for constructive interference, the rays must be in phase. So, by changing the path length, you change the phase of the rays at the screen. That means the position of the maxima changes. Between the two slits, the path difference must be ##\lambda## for constructive interference, let's say at angle ##\theta## for the first maximum. If you make the path longer, you close the angle. That's all there is to
  • #1
somecelxis
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Homework Statement


the correct ans is A. but my ans is D.
When the thin polaroid is placed in front of S1 , it slow down the light wave . as v = fλ. as v decreases , λ also decreases. This cause the x ( fringe separation ) to be smaller. And this also cause the light ray to conccentrate on the ' bright region' which has smaller area comapred to before. Thus, the intensity of bright fringes is higher. i can't undrstand why the central maximum is shifted towars P. Correct me if i am wrong. Thank in advance!


Homework Equations





The Attempt at a Solution

 

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  • #2
Please help us help you by giving Homework Statement , then 2. Homework Equations and finally: 3. The Attempt at a Solution

In short: use the template.
 
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  • #3
1. Homework Statement
in photo

3. The Attempt at a Solution
When the thin polaroid is placed in front of S1 , it slow down the light wave . as v = fλ. as v decreases , λ also decreases. This cause the x ( fringe separation ) to be smaller. And this also cause the light ray to conccentrate on the ' bright region' which has smaller area compared to before. Thus, the intensity of bright fringes is higher.Why the intensity of bright fringes decreases?

the central maximum is shifted towars P. Because the speed passing thru thin polaroid is slower using v = fλ, as v is slow , causing λ to be low, but since s1 and s2 are coherent , so they produce same no of wavelength , ...So , the distance S1 to O is closer than S2 to O . making the central maximum shift towras P ? am i right?
 
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  • #4
λ decreases, but only while in the plastic.
 
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  • #5
NascentOxygen said:
λ decreases, but only while in the plastic.

then Why the intensity of bright fringes decreases? i can't understand
 
  • #6
OK, here goes:

1. Polaroid blocks about half the light from S1. So bright fringes (constructive interference) get less light and dark fringes don't have as much destructive interference as before, so they appear less dark.

2. As you say, v decreases in the polaroid. So the optical path from S1 to O is a little longer. That means the path from S2 to the new central maximum (where the path lengths are equal again) has to become a little longer too. In other words: Central maximum shifts towards P.

I think this exercise is really quite challenging. Very nice to incorporate in a lab experiment, too ! Seeing is believing !
 
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  • #7
@BvU
It is against forum rules to provide complete solutions to homework exercises. Homework is supposed to challenge the student to think and research.
 
  • #8
@O2 i.s.n. :
You're right. Let's pick up excelcis at post #3 where he (she?) is hopelessly lost. Perhaps we should also require a completed template. Just so he/she chooses the right equations (and hopefully understands them!)
 
  • #9
BvU said:
OK, here goes:

1. Polaroid blocks about half the light from S1. So bright fringes (constructive interference) get less light and dark fringes don't have as much destructive interference as before, so they appear less dark.

2. As you say, v decreases in the polaroid. So the optical path from S1 to O is a little longer. That means the path from S2 to the new central maximum (where the path lengths are equal again) has to become a little longer too. In other words: Central maximum shifts towards P.

I think this exercise is really quite challenging. Very nice to incorporate in a lab experiment, too ! Seeing is believing !

why v decreases in the polaroid. So the optical path from S1 to O is a little longer??
 
  • #10
Now we are back to square 1. Wasn't this what you yourself already wrote in post #1 ? In general the breaking index of plastic is > 1. Optical path is measured as the number of wavelengths to get from a to b. ##\lambda## a bit smaller for part of the trajectory ##\rightarrow## optical path a little longer.
 
  • #11
BvU said:
Now we are back to square 1. Wasn't this what you yourself already wrote in post #1 ? In general the breaking index of plastic is > 1. Optical path is measured as the number of wavelengths to get from a to b. ##\lambda## a bit smaller for part of the trajectory ##\rightarrow## optical path a little longer.

well , why That means the path from S2 to the new central maximum (where the path lengths are equal again) has to become a little longer too
 
  • #12
Quite! and that means...
 
  • #13
BvU said:
Quite! and that means...

why That means the path from S2 to the new central maximum (where the path lengths are equal again) has to become a little longer too ...
what do you mean by quite! that means ... ?
 
  • #14
BvU said:
Now we are back to square 1. Wasn't this what you yourself already wrote in post #1 ? In general the breaking index of plastic is > 1.

It is refractive index :smile:

ehild
 
  • #15
bending index might fit, too! :approve:
 
  • #16
somecelxis said:
When the thin polaroid is placed in front of S1 , it slow down the light wave . as v = fλ. as v decreases , λ also decreases. This cause the x ( fringe separation ) to be smaller.
It doesn't affect fringe separation, because λ in air is unchanged.

And this also cause the light ray to conccentrate on the ' bright region' which has smaller area comapred to before. Thus, the intensity of bright fringes is higher.
No, and no. Quite the opposite.

Just making sure you have this much correct.
 
  • #17
somecelxis said:
well , why That means the path from S2 to the new central maximum (where the path lengths are equal again) has to become a little longer too

Because if one path length becomes longer, for the rays to again be exactly in phase, the other path length must similarly increase.
 
  • #18
We know that both slits s1 and s2 are already coherent unless we change the coherency, e.g. by putting one object like a Polaroid in front of them, to make them no longer coherent. Here we have used a Polaroid to cover the slit s1 which has the role that the emitting wave light started at point s1 coherent with the other falls behind the wave light s2. We know that intensity produced by superposition of two light waves will be minimum if their polarizations change randomly as time goes on. In which case, we will have a minimum picked intensity on the screen.
 
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  • #19
It is refractive index
Yup, it sure is. Slip of the old mother tongue. :redface:
 
  • #20
what do you mean by quite! that means ... ?
Quite is a subtle way to say "Yes!" when you are at the same time trying to express some doubt about whether the other party has really fully understood whatever it's about.

Now I've already been put right about the refractive index, so perhaps this tidbit of english idiom is also just hearsay and imagination...

Otherwise the preceding post might as well read

Quite! Slip of the old mother tongue. :smile:

At the risk of hijacking this thread into the languages domain: let's leave it at this.
Quite!
 
  • #21
The issue Mr. Dirac's namesake brings up is quite a bit more interesting. How about the polarization in this diffraction business?

My picture was that the source produces unpolarized lightwaves; all that was given is "monochromatic". My rather limited knowledge didn't bring up any drastic influences on this polarization from the various slits involved (after all they can't be all that narrow, or we would be in the dark completely). So I gather the piece of polaroid simply let's through linearly polarized light with polarization in one direction and blocks the light with polarization in the direction perpendicular to that. Effectively reducing the intensity of the S1 source by two, so that both constructive and destructive interference are limited to at best 75%, respectively at worst 25%.

Any other views on this ? I wish I had the stuff at home to try it out. Might go out and buy one of these laser pointer things (but aren't they polarized?)
 
  • #22
BvU said:
Yup, it sure is. Slip of the old mother tongue.

I wonder what language it is. As the refractive index in Hungarian is törésmutató and "törés" means "breaking" :smile:

ehild
 
  • #23
BvU said:
I wish I had the stuff at home to try it out. Might go out and buy one of these laser pointer things (but aren't they polarized?)

Cheap lasers produce randomly polarized light. So a polariser will reduce the average intensity.

ehild
 

Related to Why is the Central Maximum Shifted Towards P? Ask Here!

1. Why is the central maximum shifted towards P?

The central maximum is shifted towards P because of the diffraction phenomenon. Diffraction occurs when a wave encounters an obstacle or slit that is comparable in size to its wavelength. This leads to the bending of the wave and the formation of a pattern of bright and dark fringes. In the case of light passing through a single slit, the central maximum is shifted towards the point of diffraction, which in this case is P.

2. How does the size of the slit affect the shift of the central maximum towards P?

The size of the slit plays a crucial role in determining the shift of the central maximum towards P. The smaller the slit, the greater the shift towards P. This is because the smaller slit size leads to a larger diffraction effect, resulting in a greater bending of the wave towards P.

3. Can the shift of the central maximum towards P be observed in other types of waves?

Yes, the shift of the central maximum towards P can be observed in other types of waves, such as sound waves and water waves. The phenomenon of diffraction applies to all types of waves, and the central maximum will always be shifted towards the point of diffraction.

4. Are there any real-life applications of the shift of the central maximum towards P?

Yes, there are several real-life applications of the shift of the central maximum towards P. One example is in the field of optics, where this phenomenon is utilized in the design of diffraction gratings, which are used to split light into its component wavelengths. It is also used in the study of crystal structures and in the production of holographic images.

5. How does the distance between the slit and the screen affect the shift of the central maximum towards P?

The distance between the slit and the screen has a minimal effect on the shift of the central maximum towards P. As long as the distance is large enough to ensure that the wave has fully diffracted, the shift will remain relatively constant. However, as the distance increases, the overall intensity of the diffraction pattern decreases due to spreading out of the wave.

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