Single slit, optics, special case

In summary: If you have a flat viewing-screen, as you get further away from the center, the light has to travel a longer distance from the slit, so you have a 1/r^2 decrease in intensity, multiplied onto your I(\theta).So basically the wave can pass through the slit but the intensity on a far screen (Fraunhaufer conditions) is very small and spread almost equally everywhere on the screen. Is my interpretation right?I'd have to go back over the derivation, but IIRC that formula for irradiance is valid only in the far-field. The near field distribution (the Fresnel region) is much more complex than the Frauhofer distribution.
  • #1
fluidistic
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I've thought about the case when the wavelength of the incident EM waves on a single slit is much greater than the width of the slit. When we have [tex]\lambda >> D[/tex]. It could be the case of a radiowave incidating over a single slit whose width is day a nanometer large.
According to Hecht, the irradiance is worth [tex]I(\theta)=I(0)\frac{\sin \beta}{\beta}[/tex] where [tex]\beta=\frac{kD \sin \theta}{2}[/tex]. Thus [tex]\beta=\frac{\pi D \sin (\theta)}{\lambda}[/tex].
In my case this reduces to [tex]\beta \approx 1[/tex] and therefore [tex]I(\theta)\approx I(0)[/tex] for all [tex]\theta[/tex]... This means that the intensity over the screen does not almost change and is therefore almost constant whatever theta is. Now I realize that I(0) is likely a very small value, in other words it's like if I spread the incident wave over a gigantic screen.
So basically the wave can pass through the slit but the intensity on a far screen (Fraunhaufer conditions) is very small and spread almost equally everywhere on the screen. Is my interpretation right?
 
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  • #3
Andy Resnick said:
I'd have to go back over the derivation, but IIRC that formula for irradiance is valid only in the far-field. The near field distribution (the Fresnel region) is much more complex than the Frauhofer distribution.

http://en.wikipedia.org/wiki/Near-field_diffraction_pattern

Thanks for the info Andy. I was considering the far field thus (?) Fraunhaufer diffraction.

I mean the screen where I observe the irradiance is very far from the slit. Is my reasoning valid?
 
  • #4
If you have a flat viewing-screen, as you get further away from the center, the light has to travel a longer distance from the slit, so you have a 1/r^2 decrease in intensity, multiplied onto your [itex]I(\theta)[/itex].

If you have a semicircular viewing-screen, with the slit at the center of curvature, so all points on the screen are the same distance from the slit, than I think your conclusion is valid. (I'm going from my memory of the assumptions that go into the derivation of Fraunhofer diffraction.)
 
  • #5
jtbell said:
If you have a flat viewing-screen, as you get further away from the center, the light has to travel a longer distance from the slit, so you have a 1/r^2 decrease in intensity, multiplied onto your [itex]I(\theta)[/itex].

If you have a semicircular viewing-screen, with the slit at the center of curvature, so all points on the screen are the same distance from the slit, than I think your conclusion is valid. (I'm going from my memory of the assumptions that go into the derivation of Fraunhofer diffraction.)

I think I understand what you mean.
In fact I(0) is definied as being the maximum of irradiance (or intensity, I don't remember) viewed on the viewing-screen. So I'm totally safe not using a 1/r^2 relation. I'm sorry that I haven't clarified it.
 
  • #6
There are two complications to this problem.

1. One must take the obliquity factor into account, if you are looking at angles that are far off-axis. This multiplicative factor has a maximum for θ=0. So the the intensity will diminish away from the central maximum, even for a semicircular screen.

2. My recollection about large wavelengths is: for a wavelength comparable to, or larger, than the slit width, we need to know about the boundary conditions at the slit border. The electric field doesn't abruptly go to zero at the slit boundary, though that is a reasonable approximation when the wavelength is a lot smaller than the slit size.
 
  • #7
fluidistic said:
Thanks for the info Andy. I was considering the far field thus (?) Fraunhaufer diffraction.

I mean the screen where I observe the irradiance is very far from the slit. Is my reasoning valid?

Well, my point is that if you have a sub-wavelength aperture, the far-field pattern will not be given by the Fraunhofer distribution. In fact, it's likely that the irradiance will simply be zero.
 

1. What is a single slit in optics?

A single slit in optics refers to a narrow opening through which light passes, typically used in experiments to study diffraction. It is a common setup in optics experiments and is used to demonstrate the wave nature of light.

2. How does a single slit affect light waves?

A single slit causes light waves to diffract, or spread out, as they pass through the narrow opening. This results in a pattern of light and dark fringes, known as a diffraction pattern, on a screen placed behind the slit. The width of the slit and the wavelength of the light determine the spacing of the fringes.

3. What is the special case of a single slit?

The special case of a single slit refers to when the width of the slit is very small compared to the wavelength of the light passing through it. In this case, the diffraction pattern produced on the screen is a single bright central maximum with very faint secondary maxima on either side.

4. What is the significance of the special case in optics?

The special case of a single slit is significant because it demonstrates the relationship between the width of a slit and the resulting diffraction pattern. It also shows that light can behave as both a wave and a particle, as the central maximum is a result of the wave nature of light and the secondary maxima are a result of the particle nature of light.

5. How is the width of a single slit determined?

The width of a single slit can be determined by measuring the distance between the central maximum and the first secondary maximum on either side of the diffraction pattern on the screen. This distance is known as the angular width and can be used to calculate the width of the slit using the formula w = λ/d, where λ is the wavelength of light and d is the distance between the slit and the screen.

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