Single Slit / Wavelength / Central Maximum

Click For Summary

Homework Help Overview

The discussion revolves around a physics problem involving a laser with a wavelength of 560 nm directed at a single slit, creating an interference pattern on a screen located 3.0 m away. The central maximum is noted to be 5.0 cm wide, and participants are tasked with determining the width of the slit.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants present two attempts at solving the problem, each using different equations related to diffraction and interference. There is a question regarding whether the width of the central maximum should be halved to find the distance to the first minimum. Some participants express uncertainty about the definitions and applications of the variables involved.

Discussion Status

There is an ongoing exploration of the problem with various interpretations being discussed. Some participants provide insights into the derivation of the equations and the principles behind the interference pattern, while others seek clarification on specific aspects of the problem.

Contextual Notes

Participants are navigating through the complexities of single slit diffraction and the implications of the central maximum's width. There is a mention of the need for a formal derivation, which some find challenging, and a reference to different approaches to understanding the underlying physics.

julianwitkowski
Messages
133
Reaction score
0

Homework Statement



A laser emitting light with a wavelength of 560 nm is directed at a single slit, producing an interference pattern on a screen that is 3.0 m away. The central maximum is 5.0 cm wide. Determine the width of the slit.

I have two ideas of the answer but I'm not sure which is right... Please help me understand which one and why.

Homework Equations


[/B]
d = λ / sin(Θ)
tan(Θ) = x / L

or...

w = λL / y

The Attempt at a Solution


[/B]
Attempt #1

d = slit width
λ = wavelength (560nm = 5.6· 10⁻⁷m)
Θ = angle

If the central maximum is 5.0cm wide, then is the distance from the center to the first minimum always half of that or 2.5cm?

tan(Θ) = 0.025m / 3m
Θ = tan⁻¹ (0.025m / 3m) = 0.477°
d · sin(Θ) = λ

d = λ / sin(Θ) = 560nm /sin(0.477°) = 5.6· 10⁻⁷m / sin(0.477°) = 6.72 · 10⁻⁵ m = 67200 nm

Attempt #2

d = slit width
λ = wavelength (560nm = 5.6· 10⁻⁷m)
L = distance to screen.
y = central maximum.

w = λL / y = 5.6 ·10⁻⁷m · 3m / 0.05m = 3.36 · 10⁻⁵ m = 33600nm
 
Physics news on Phys.org
julianwitkowski said:

Homework Statement



A laser emitting light with a wavelength of 560 nm is directed at a single slit, producing an interference pattern on a screen that is 3.0 m away. The central maximum is 5.0 cm wide. Determine the width of the slit.

I have two ideas of the answer but I'm not sure which is right... Please help me understand which one and why.

Homework Equations


[/B]
d = λ / sin(Θ)
tan(Θ) = x / L

or...

w = λL / y

The Attempt at a Solution


[/B]
Attempt #1
d = slit width
λ = wavelength (560nm = 5.6· 10⁻⁷m)
Θ = angle
If the central maximum is 5.0cm wide, then is the distance from the center to the first minimum always half of that or 2.5cm?
Yes. the pattern is symmetrical about θ. sinθ is an odd function. So is tanθ.
tan(Θ) = 0.025m / 3m
Θ = tan⁻¹ (0.025m / 3m) = 0.477°
d · sin(Θ) = λ
d = λ / sin(Θ) = 560nm /sin(0.477°) = 5.6· 10⁻⁷m / sin(0.477°) = 6.72 · 10⁻⁵ m = 67200 nm
Stop right there!
Attempt #2
d = slit width
λ = wavelength (560nm = 5.6· 10⁻⁷m)
L = distance to screen.
y = central maximum.
w = λL / y = 5.6 ·10⁻⁷m · 3m / 0.05m = 3.36 · 10⁻⁵ m = 33600nm
Not sure what your y is. Is it the total width of the central maximum? If so the formula is incorrect.
Your 1st formula derivation is not trivial so you should just accept it unless you're afraid you'll have to derive it in a test someday.
 
  • Like
Likes   Reactions: julianwitkowski
rude man said:
Stop right there!
.

I wasn't sure if I was supposed to cut the central maximum in half or not.
Thank you for your time, this has helped me :)
 
Hello Julian,

As Rudy indicates, the formal derivation of the single slit diffraction pattern isn't trivial. And personally I don't like the little arrows addition approach (matter of taste, I suppose). Better to study that using Fourier transformation.
Since I think you are a curious person (and also because you ask for understanding in post #1), this is how they taught me before I knew about Fourier transforms:

According to the Huygens principle, all points in the slit opening function as point sources for the emanating wave.

If you divide the opening in two halves , then for rays that go in the direction of the first minimum from the top half (#3 is shown in the drawing), there is a corresponding ray in the lower half with which it interferes destructively (#4 for #3 and then stepping down until the top one is in the center and the corresponding lower one at the lower end of the slit), i.e. a ray that has a phase difference of ##\lambda/2##. So you get ##d/2 \; \sin\theta = \lambda/2\;## for the first minimum.

You can do the same thing for subdividing in four quarters to get ##d/4 \; \sin\theta = \lambda/2 \; ## for the second minimum.

In between is a (relative) maximum, because if you divide in three parts, two of those will interfere destructively and that leaves the contribution of the remaining third
 
  • Like
Likes   Reactions: julianwitkowski

Similar threads

  • · Replies 2 ·
Replies
2
Views
5K
  • · Replies 6 ·
Replies
6
Views
1K
  • · Replies 3 ·
Replies
3
Views
2K
Replies
2
Views
2K
  • · Replies 6 ·
Replies
6
Views
8K
  • · Replies 4 ·
Replies
4
Views
3K
  • · Replies 6 ·
Replies
6
Views
4K
  • · Replies 10 ·
Replies
10
Views
9K
  • · Replies 5 ·
Replies
5
Views
3K
  • · Replies 5 ·
Replies
5
Views
4K