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OpenStudy (anonymous):

Question regarding light and reflection!

OpenStudy (anonymous):

OpenStudy (anonymous):

@ganeshie8 Hey Ganesh! Do you know much about this material in particular?

ganeshie8 (ganeshie8):

sorry no idea, let me tag @Vincent-Lyon.Fr

OpenStudy (anonymous):

No problem X)

OpenStudy (anonymous):

I think I figured it out but I might be wrong... We have the initial equation for destructive interference:\[\huge \phi=\frac{4\pi n_b t \cos(\theta_i)}{\lambda}-\phi_{r2}-\phi_{r1}\]Since we know that the speed will be greater in air than in glass ( \(c_2<c_1)\), then there is a phase shift of \(\pi\). Because \(\phi_{r1} = \phi_{r2}\), then the equation simplifies to:\[\huge 1=\frac{4n_b t \cos(\theta_i)}{\lambda}\]Additionally, we are given that the incidence is normal, which means that \(\theta_i=0 \implies \cos(0)=1\). Now we have\[\huge 1=\frac{4n_b t}{\lambda}\]Plugging in what we know and solving for \(n_b\), we then have\[\huge n_b=\frac{550\text{nm}}{4(104\text{nm})}=1.32\text{nm}\] I am not 100% certain, though..

OpenStudy (anonymous):

@Astrophysics

OpenStudy (anonymous):

Oops, the initial equation is supposed to have \(\huge +~\phi_{r2}\)

OpenStudy (vincent-lyon.fr):

Hi, no time now to give a full answer, but you can play with this (French) applet that will help you understand what is at stake. http://ressources.univ-lemans.fr/AccesLibre/UM/Pedago/physique/02/optiphy/antirefl.html

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