Daniel Gallimore
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Just to clarify, this isn't homework. I took an Optics course a few years ago, but in the time between then and now, I've lost all my notes.
Suppose we have an infinitely tall slit of width a and a parallel screen a distance r_0 away. Let the x axis be parallel to the width of the slit, with the origin at the center of the slit (such that the slit extends from x=-a/2 to x=a/2). The z axis extends toward the screen from the origin. An angle \theta locates a point P on the screen (with respect to the z axis) a distance x=X along the screen. A ray drawn from the origin to P is length r.
Given a plane wave incident on the slit, what is the formula for the irradiance of the diffracted wave as it encounters the screen?
I know the answer is similar (if not equal to) I=I_0\left(\frac{\sin(\beta/2)}{\beta/2}\right)^2 where \beta\equiv ka\sin\theta I also know that E=-\frac{ikE_0}{2\pi r_0}\int_{-a/2}^{a/2} e^{ikr} \, dx To get from the electric field to the irradiance is not a problem.
Any recommendations?
Suppose we have an infinitely tall slit of width a and a parallel screen a distance r_0 away. Let the x axis be parallel to the width of the slit, with the origin at the center of the slit (such that the slit extends from x=-a/2 to x=a/2). The z axis extends toward the screen from the origin. An angle \theta locates a point P on the screen (with respect to the z axis) a distance x=X along the screen. A ray drawn from the origin to P is length r.
Given a plane wave incident on the slit, what is the formula for the irradiance of the diffracted wave as it encounters the screen?
I know the answer is similar (if not equal to) I=I_0\left(\frac{\sin(\beta/2)}{\beta/2}\right)^2 where \beta\equiv ka\sin\theta I also know that E=-\frac{ikE_0}{2\pi r_0}\int_{-a/2}^{a/2} e^{ikr} \, dx To get from the electric field to the irradiance is not a problem.
Any recommendations?