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 \lambda >> D. 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 I(\theta)=I(0)\frac{\sin \beta}{\beta} where \beta=\frac{kD \sin \theta}{2}. Thus \beta=\frac{\pi D \sin (\theta)}{\lambda}.
In my case this reduces to \beta \approx 1 and therefore I(\theta)\approx I(0) for all \theta... 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 I(\theta)=I(0)\frac{\sin \beta}{\beta} where \beta=\frac{kD \sin \theta}{2}. Thus \beta=\frac{\pi D \sin (\theta)}{\lambda}.
In my case this reduces to \beta \approx 1 and therefore I(\theta)\approx I(0) for all \theta... 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?