- #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?
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?