Central Maximum Shift Due to Glass Slit in Double Slit Experiment

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SUMMARY

The discussion centers on calculating the shift of the central maximum in a double slit experiment when a thin piece of glass is introduced in one slit. The light wavelength is 600 nm, and the slits are separated by 0.20 mm, with the screen positioned 1.5 m away. The phase delay introduced by the glass is 5.0 × 10-16s, leading to a calculated shift of approximately 0.00113 meters. A simpler approach using the equation λ/4 = d sin θ is also discussed, providing an alternative method to solve for the shift without computational tools.

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Homework Statement



Light of wavelength 600 nm passes though two slits separated by 0.20 mm and is observed on a screen 1.5 m behind the slits. The location of the central maximum is marked on the screen and labeled y = 0.

A very thin piece of glass is then placed in one slit. Because light travels slower in glass than in air, the wave passing through the glass is delayed by 5.0 ×10−16s in comparison to the wave going through the other slit.

Part E

By how far does the central maximum move?

Homework Equations



\Delta \phi=2\pi m

The Attempt at a Solution



I calculated that the initial phase delay due to the glass is \frac{\pi}{2}. So in order to have constructive interference, the light wave that travels through the slit with no glass must travel an additional distance of \frac{\lambda}{4}. I called the distance that the light through the glass travels x_{1} and the distance that the light through the normal slit travels x_{2}. I know that x_{1}=\sqrt{L^{2}+(\frac{d}{2}-h)^{2}} and x_{2}=\sqrt{L^{2}+(\frac{d}{2}+h)^{2}}So then I have \sqrt{L^{2}+(\frac{d}{2}+h)^{2}}-\sqrt{L^{2}+(\frac{d}{2}-h)^{2}}=\frac{\lambda}{4}
I don't know how to solve this analytically, so I plugged it into Wolfram Alpha and got h\approx 0.00113 meters, which is correct, but I feel that there should be another way to solve for h that doesn't require a computer algebra system.

Is there another way to approach this problem that makes finding h simpler?

Thanks
 
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I would expand each radical in Taylor series. You can write the radicals as ##L\sqrt{1+\epsilon_{\pm}^2}## where ##\epsilon_{\pm}=\frac{d/2 \pm h}{L}## and expand about zero for small values of ##\epsilon_{\pm}##.

On edit: I just did it and the answer is very simple.
 
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Yes, I can see how that works now.

Thank you for your help.
 

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