How Does a Thin Glass Plate Affect Young's Double Slit Experiment?

brad sue
Messages
270
Reaction score
0

Homework Statement



The Young's double slit experiment is modified, as shown below, by placing a thin parallel glass plate of thickness d and refractive index n over one of the slits. Here a is the slit width in the x direction and b is the slit separation also in the x direction. The system is excited with on-axis collimated laser light of wavelength. A lens of focal length F is placed immediately behind the slits and a screen is placed a distance F away from the lens, so that a set of well-defined interference fringes are visible on the screen. Ignore all phase changes from reflection and transmission in this problem.

(a) For the case where the glass plate is absent, derive an expression for the position, X2m, of the mth maximum on the screen.
(b) Derive an expression for the spatial frequency shift [(sin (θ’))/λ - (sin θ)/λ] that occurs when the glass slide is inserted in the position shown in the diagram. What important conclusion do you draw from your expression?
(c) Derive an expression for the lateral spatial shift X’2m -X2m on the screen as a result of inserting the glass slide.
(d) In which direction do the fringes shift?






The Attempt at a Solution


I solved this problem but I did not use the fresnel nor fraunhofer equations.
Do you think i should use those equations or concept?
It is the lens that confuses me. I know that when we have a lens, the output field is the Fourier transform of the input field.
I attached the picture.

Please, can I have your suggestions?
thank you
 

Attachments

  • young_experiment.gif
    young_experiment.gif
    14.1 KB · Views: 654
Physics news on Phys.org
You don't need Faraunhofer or Fresnel equations with this problem.
The lens serves to bring the so-called "far-field" (Fraunhofer diffraction) to comfortable distance within the laboratory. Forget about it.
The glass slab is the key. Since the speed of light changes inside the glass, so does the wavelength. Thus, the phase shift, after traveling a distance d changes according the refraction index. This phase shift makes the fringes move up or down. Repeat the basic calculation, but take into account the refractive index of glass.
 
Thank you
As you said the lens just allow the fringes to be seen at a focal length . For example if the distance to the screen was 2* focal length the fringes would appear blurry.
 
Hello everyone, I’m considering a point charge q that oscillates harmonically about the origin along the z-axis, e.g. $$z_{q}(t)= A\sin(wt)$$ In a strongly simplified / quasi-instantaneous approximation I ignore retardation and take the electric field at the position ##r=(x,y,z)## simply to be the “Coulomb field at the charge’s instantaneous position”: $$E(r,t)=\frac{q}{4\pi\varepsilon_{0}}\frac{r-r_{q}(t)}{||r-r_{q}(t)||^{3}}$$ with $$r_{q}(t)=(0,0,z_{q}(t))$$ (I’m aware this isn’t...
Hi, I had an exam and I completely messed up a problem. Especially one part which was necessary for the rest of the problem. Basically, I have a wormhole metric: $$(ds)^2 = -(dt)^2 + (dr)^2 + (r^2 + b^2)( (d\theta)^2 + sin^2 \theta (d\phi)^2 )$$ Where ##b=1## with an orbit only in the equatorial plane. We also know from the question that the orbit must satisfy this relationship: $$\varepsilon = \frac{1}{2} (\frac{dr}{d\tau})^2 + V_{eff}(r)$$ Ultimately, I was tasked to find the initial...
Back
Top