Interference for for N slits formula

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The discussion focuses on the mathematical derivation of the intensity formula for interference patterns produced by a lattice with N slits, specifically referencing a formula found in a PDF document. It clarifies that the maximum intensity, denoted as ##I_{max}##, occurs when both the numerator and denominator of the intensity ratio approach zero. The user demonstrates this by substituting values into the sine functions and analyzing the limit as the variable approaches zero, concluding that the behavior of the ratio is directly linked to the integer nature of N.

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Nikitin
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Interference for a lattice with N slits

OK, so check out the first formula (the one for intensity) in the following pdf:

http://folk.ntnu.no/magnud/OvLf/bolge/oving11.pdf

It's the formula for Intensity as a function of angle from the interference for a lattice with N very thin slits.

Mathematically, why is ##I_{max}## found only when BOTH the numerator and denominator are approaching zero?

I agree that the intensity is largest when the ratio between the numerator and denominator is biggest, but why does this only happen when both approach zero?
 
Last edited:
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Replaces previous post, which was misleading.

Consider when [itex]\theta[/itex] is close to [itex]n\pi[/itex]. Put [itex]\theta = n\pi + \epsilon[/itex].

Then [itex]\frac{sin N\theta}{sin \theta} = \frac{sin (Nn\pi +N\epsilon)}{sin (n\pi + \epsilon)} = \frac{cos (Nn\pi) sin(N\epsilon)}{cos (n\pi) sin\epsilon} = ± \frac{sin N\epsilon}{sin \epsilon}[/itex]

The limit of this as [itex]\epsilon[/itex] approaches zero is simply [itex]±\frac{N\epsilon}{\epsilon} = ±N[/itex].
 
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Oh I just figured it out. When the upper term approaches zero, then so must the lower turn because N is just a whole number.

thanks
 

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