A common way for deriving the expression for the minima in a single slit diffraction pattern involves dividing the slit into even number of zones and pairing up the wavelets so that they cancel out for a particular angle.
Dividing the slit into two zones and applying the condition for destructive interference gives
$$\frac{a}{2} \sin{\theta} = \frac\lambda 2$$
And generalizing this, we get
$$a \sin\theta = m \lambda$$
Now this is my question:
The expression $\frac{a}{2} \sin{\theta} = \frac\lambda 2$ says that for some angle $\theta$ , the wavelets from the two zones will interfere destructively, producing the first minima. Now, $\frac{a}{2} \sin{\theta}$ is simply the path difference between the wavelets, and if I equate the path difference to, say, $\lambda$ , i.e, the condition for constructive interference , I will get
$$a \sin\theta = 2 \lambda$$
which should give the angular position of a maxima. But this contradicts with the position for minima, given by $a \sin\theta = m \lambda$ , when $m = 2$ .
So what's wrong with my reasoning ?