Laser Gyroscope: Difference between revisions
Line 23: | Line 23: | ||
simplifying, | simplifying, | ||
<math> t_{CW} = \frac{L_{0}}{c-R\Omega}, \quad t_{CCW} = \frac{L_{0}}{c+R\Omega} </math> | <math> t_{CW} = \frac{L_{0}}{c-R\Omega}, \quad t_{CCW} = \frac{L_{0}}{c+R\Omega}, \quad \Delta t = t_{CW} - t_{CCW} = \frac{L_{0} \cdot 2R\Omega}{c^{2}} \cdot \frac{1}{1+\left(\frac{R\Omega}{c}\right)^{2}} </math> | ||
==Setup== | ==Setup== |
Revision as of 11:14, 31 January 2025
Some Description
Team members
Darren e0303300@u.nus.edu
Wen Xin e0309271@u.nus.edu
Idea
This project aims to measure some rotation by using the Sagnac effect, by using a loop of fiber as a ring interferometer.
Sagnac effect
When two beams of light are sent into the two ports of a ring interferometer, they travel clockwise (CW) and counter-clockwise (CCW) paths respectively. For a stationary ring interferometer, since the path length traversed by each beam is the same, this leads to complete constructive interference at the output port.
Now let's say the interferometer is spinning in the CW direction with rotation rate . Then there will be a difference in path length:
which results in a timing difference of:
simplifying,
Setup
The main setup will be a fiber based sagnac intereferometer with detection of the output done using photodiodes. We are aiming to build everything in the 1550nm wavelength range.
We can put the setup on a chair to spin it a bit :0
Measurements
....