00:01
All right, so here, we are given that, we are given the depression and the interference combined, right? so we will consider the interference pattern produced by two parallel slates, which is here, right? so these are two parallel slits, right? these are two parallel slits right and we will consider these two slits and these are the thickness of the slit which is a and the separation distance is d here and this is d in d is 3a right and we know that a pram here a is d by 3 and here from the formula, we know that the condition part the interference maxima is a plus b l sine theta, this is n lambda, right? so let in part a part the first order, n will be one.
01:19
And let a plus d sine theta 1 is limda and sine theta 1 is 3 limba by 4d and putting these values here we will get that sine theta 1 is sine inverse a theta 1 is sine inverse 3 limda or 4 d right and part the second order this in will be 2 here and putting the values there here a theta 2 will be sine and verse of 3 limda by 2d right now part the third order n is 3 and sine theta 3 or theta 3 is sine inverse of 9 limna right over 4d and for the third of theta 4 is sine inverse of 3 limda over d right which is here and in part d we know that this is the intensity i not at a central maxima right and this is intensity at any point or at any theta.
02:25
And the formula part, this is i now, this is intensity, i.
02:32
I not, sine square alpha, or alpha square, k square beta, right? now we know the formulas per alpha and beta.
02:40
So these are alpha and beta and are the first theta, right? so we are doing part b here, right? so par the pus theta, which is lambda by 4a, this will be alpha, which is pi by 4, and this is pi run...