Interference for for N slits formula

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The discussion focuses on the mathematical understanding of intensity in interference patterns for a lattice with N slits. The key point is that maximum intensity, denoted as I_max, occurs when both the numerator and denominator of the intensity formula approach zero simultaneously. This is illustrated by analyzing the behavior of the sine functions as the angle approaches specific values. The limit shows that as the upper term approaches zero, the lower term must also approach zero, which is linked to the integer nature of N. This insight clarifies the conditions for achieving maximum intensity in the interference pattern.
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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?
 
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Replaces previous post, which was misleading.

Consider when \theta is close to n\pi. Put \theta = n\pi + \epsilon.

Then \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}

The limit of this as \epsilon approaches zero is simply ±\frac{N\epsilon}{\epsilon} = ±N.
 
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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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